pscp-1992.csv

# Data from paperscape.org
# If you use this data, please give due credit to: Damien P. George and Rob Knegjens, Paperscape
# A citable DOI for this data can be found at http://github.com/paperscape/paperscape-data
#
# Format is 1 line per entry, with 7 fields separated by semicolons:
# arxiv-id;comma-separated-arxiv-categories;num-found-refs;num-total-refs;comma-separated-refs;comma-separated-authors;title
# Parse with Python code: entries = [line.split(";", 7) for line in open("file")]
# See comments at the bottom of this file for statistics
hep-th/9201001;hep-th,math.QA;0;17;;C.Itzykson,J.-B.Zuber;Combinatorics of the Modular Group II: the Kontsevich integrals
hep-lat/9201001;hep-lat;0;0;;J.Berlin;Monte Carlo Simulations of Higgs-Fermion Systems
hep-lat/9201002;hep-lat;0;4;;R.V.Gavai,U.M.Heller,F.Karsch,B.Plache,T.Neuhaus;A Study of Symmetry Restoration at Finite Temperature in the O(4) Model Using Anisotropic Lattices
hep-lat/9201003;hep-lat;0;11;;S.Caracciolo,R.G.Edwards,A.Pelissetto,A.D.Sokal;Dynamic Critical Behaviour of Wolff's Algorithm for $RP^N$ $σ$-Models
hep-lat/9201004;hep-lat;0;9;;U.M.Heller,M.Klomfass,H.Neuberger,P.Vranas;How to Put a Heavier Higgs on the Lattice
hep-lat/9201005;hep-lat;0;4;;K.M.Bitar,R.Edwards,T.A.DeGrand,S.Gottlieb,U.M.Heller,A.D.Kennedy,J.B.Kogut,A.Krasnitz,W.Liu,M.C.Ogilvie,R.L.Renken,D.K.Sinclair,R.L.Sugar,D.Toussaint,K.C.Wang;QCD Hadron Spectroscopy with Staggered Dynamical Quarks at $β= 5.6$
hep-lat/9201006;hep-lat;0;2;;K.M.Bitar;Path Integrals and Voronin's Theorem on the Universality of the Riemann Zeta Function
hep-lat/9201007;hep-lat;0;6;;A.D.Kennedy,R.G.Edwards;On the Dynamics of Light Wilson Quarks
hep-th/9201002;hep-th;0;0;;F.Bonechi,E.Celeghini,R.Giachetti,E.Sorace,M.Tarlini;Inomogeneous Quantum Groups as Symmetries of Phonons
hep-th/9201003;hep-th;0;105;;R.Dijkgraaf;Intersection Theory, Integrable Hierarchies and Topological Field Theory
hep-th/9201004;hep-th;0;0;;N.Berkovits;The Heterotic Green-Schwarz Superstring on an N=(2,0) Super-Worldsheet
hep-th/9201005;hep-th;1;22;hep-th/9109032;I.R.Klebanov;Ward Identities in Two-Dimensional String Theory
hep-th/9201006;hep-th;0;31;;D.Bernard;On Symmetries of Some Massless 2D Field Theories
hep-th/9201007;hep-th;0;21;;M.Cvetic,S.Griffies,S.-J.Rey;Static Domain Walls in N=1 Supergravity
math/9201201;math.CV;0;0;;E.M.Chirka;On the Removable Singularities for Meromorphic Mappings
math/9201202;math.FA;0;0;;T.Figiel,W.B.Johnson,G.Schechtman;Factorizations of natural embeddings of l_p^n int L_r
math/9201203;math.MG,math.FA;0;0;;K.Ball,A.Pajor;Convex bodies with few faces
math/9201204;math.MG,math.FA;0;0;;K.Ball;Shadows of convex bodies
math/9201205;math.MG,math.FA;0;0;;K.Ball;Volume ratios and a reverse isoperimetric inequality
math/9201206;math.FA,math.MG;0;0;;G.Schechtman,J.Zinn;On the volume of the intersection of two $L_p^n$ balls
math/9201207;math.FA;0;0;;S.J.Montgomery-Smith,M.Talagrand;The Rademacher cotype of operators from $l_∞^N$
math/9201208;math.PR,math.FA;0;0;;W.B.Johnson,G.Schechtman;Remarks on Talagrand's deviation inequality for Rademacher functions
math/9201209;math.FA;0;0;;N.Ghoussoub,W.B.Johnson;Operators which factor through Banach lattices not containing c_0
math/9201210;math.FA;0;0;;P.Saab;Integral Operators on Spaces of Continuous Vector-valued Functions
math/9201211;math.FA;0;0;;P.Saab,B.Smith;Nuclear operators on spaces of continuous vector-valued functions
math/9201212;math.FA;0;0;;D.J.H.Garling,S.J.Montgomery-Smith;Complemented subspaces of spaces obtained by interpolation
math/9201213;math.FA;0;5;;P.F.X.Müller;Permutations of the Haar system
math/9201214;math.FA;0;0;;D.E.Alspach;On the complemented subspaces of X_p
math/9201215;math.FA;0;0;;S.J.Montgomery-Smith,P.Saab;p-summing operators on injective tensor products of spaces
math/9201216;math.FA;0;0;;B.Maurey;Some deviation inequalities
math/9201217;math.MG,math.FA;0;0;;K.Ball;Ellipsoids of maximal volume in convex bodies
math/9201218;math.MG,math.FA;0;0;;K.Ball;The plank problem for symmetric bodies
math/9201219;math.FA;0;0;;E.Odell;On quotients of Banach spaces having shrinking unconditional bases
math/9201220;math.FA;0;0;;W.B.Johnson,G.Pisier;The proportional UAP characterizes weak Hilbert spaces
math/9201221;math.FA;0;0;;S.J.Montgomery-Smith;Comparison of Orlicz-Lorentz spaces
math/9201222;math.FA;0;0;;S.A.Argyros,I.Deliyanni;Non dentable sets in Banach spaces with separable dual
math/9201223;math.FA;0;0;;D.E.Alspach;Level sets and the uniqueness of measures
math/9201224;math.FA;0;0;;E.Odell;On Schreier unconditional sequences
math/9201225;math.FA;0;0;;T.Schlumprecht;An arbitrarily distortable Banach space
math/9201226;math.FA;0;0;;J.Bastero,F.J.Ruiz;Interpolation of operators when the extreme spaces are $L^∞$
math/9201227;math.OA,math.FA;0;0;;G.Pisier;Remarks on complemented subspaces of von-Neumann algebras
math/9201228;math.FA;0;0;;G.Pisier;A simple proof of a theorem of Jean Bourgain
math/9201229;math.FA;0;0;;G.Pisier;Interpolation between H^p spaces and non-commutative generalizations, I
math/9201230;math.FA;0;9;;D.H.Leung;Banach spaces with Property (w)
math/9201231;math.FA;0;0;;B.Khaoulani;A Gordon-Chevet type Inequality
math/9201232;math.FA;0;0;;G.Pisier;The K_t-functional for the interpolation couple L_1(A_0),L_infinity(A_1)
math/9201233;math.FA;0;0;;P.Ørno;On J. Borwein's concept of sequentially reflexive Banach spaces
math/9201234;math.FA;0;0;;B.J.Cole,T.W.Gamelin,W.B.Johnson;Analytic Disks in Fibers over the Unit Ball of a Banach Space
math/9201235;math.FA;0;9;;N.Asmar,S.J.Montgomery-Smith;On the distribution of Sidon series
math/9201236;math.FA;0;0;;R.Haydon,E.Odell,H.P.Rosenthal;On certain classes of Baire-1 functions with applications to Banach space theory
hep-th/9201008;hep-th;0;0;;S.Matsuda;Coulomb Gas Representations and Screening Operators of the N=4 Superconformal Algebras
hep-th/9201009;hep-th;0;14;;E.Silverstein;Large-Small Equivalence in String Theory
hep-th/9201010;hep-th;0;14;;A.Marshakov,A.Mironov,A.Morozov;From Virasoro Constraints in Kontsevich's Model to $\cal W$-constraints in 2-matrix Models
hep-th/9201011;hep-th;0;15;;A.Marshakov,A.Mironov,A.Morozov;On Equivalence of Topological and Quantum 2d Gravity
hep-th/9201012;hep-th;0;38;;A.Mironov,A.Zabrodin;The Asymptotics of the Correlations Functions in $(1+1)d$ Quantum Field Theory From Finite Size Effects in Conformal Theories
hep-th/9201013;hep-th;0;46;;S.Kharchev,A.Marshakov,A.Mironov,A.Morozov,A.Zabrodin;Towards unified theory of $2d$ gravity
hep-th/9201014;hep-th;0;25;;P.Berglund,T.Hübsch;A Generalized Construction of Mirror Manifolds
hep-th/9201015;hep-th;0;0;;S.Kar,S.Khastgir,A.Kumar;An Algorithm to Generate Classical Solutions for String Effective Action
hep-th/9201016;hep-th;0;0;;L.Castellani;Bicovariant Differential Calculus on the Quantum D=2 Poincare Group
hep-th/9201017;hep-th;0;56;;N.Seiberg,S.Shenker;A Note on Background (In)dependence
hep-th/9201018;hep-th;0;0;;W.Ogura;Discrete and Continuum Virasoro Constraints in Two-Cut Hermitian Matrix Models
hep-th/9201019;hep-th;0;0;;J.A.Dixon,M.J.Duff,E.Sezgin;The Coupling of Yang-Mills to Extended Objects
hep-th/9201020;hep-th;0;0;;A.S.Galperin,K.S.Stelle;The Superparticle and the Lorentz Group
hep-th/9201021;hep-th;0;0;;J.Russo,A.A.Tseytlin;Scalar-Tensor Quantum Gravity in Two Dimensions
hep-th/9201022;hep-th;0;12;;H.Fukutaka;Anomalous Jacobian Factor in the Polyakov Measure for Abelian Gauge Field in Curved Spacetimes
hep-th/9201023;hep-th;0;0;;C.N.Pope;$SL(∞,R)$ Symmetry of $W_∞$ Gravity
hep-th/9201024;hep-th;0;26;;H.Aratyn,L.A.Ferreira,J.F.Gomes,A.H.Zimerman;A New Deformation of W-Infinity and Applications to the Two-loop WZNW and Conformal Affine Toda Models
hep-th/9201025;hep-th;0;9;;M.Forger,J.Laartz,U.Schaeper;Current Algebra of Classical Non-Linear Sigma Models
hep-th/9201026;hep-th;0;50;;J.-L.Gervais,Y.Matsuo;Classical A_n--W-Geometry
hep-th/9201027;hep-th;0;21;;J.M.Isidro,J.M.F.Labastida,A.V.Ramallo;Coset Constructions in Chern-Simons Gauge Theory
math/9201237;math.FA;0;5;;D.H.Leung;Isomorphisms of certain weak L^p spaces
hep-th/9201028;hep-th;0;0;;T.Gannon,C.S.Lam;Can a Lattice String Have a Vanishing Cosmological Constant?
math/9201238;math.LO,math.GN;0;0;;S.Shelah;Existence of endo-rigid Boolean algebras
math/9201239;math.LO;0;0;;T.Jech,S.Shelah;A note on canonical functions
math/9201240;math.LO;0;13;;B.Hart,S.Shelah;Categoricity over P for first order T or categoricity for phi in L_{omega_1 omega} can stop at aleph_k while holding for aleph_0, ..., aleph_{k-1}
math/9201241;math.LO;0;9;;J.T.Baldwin,S.Shelah;The primal framework. I
math/9201242;math.LO;0;0;;T.Jech,S.Shelah;Full reflection of stationary sets below aleph_omega
math/9201243;math.LO;0;0;;S.Shelah;The Hanf numbers of stationary logic. II. Comparison with other logics
math/9201244;math.LO;0;0;;S.Shelah;Strong partition relations below the power set: consistency, was Sierpinski right, II?
math/9201245;math.LO;0;0;;S.Shelah;Viva la difference I: Nonisomorphism of ultrapowers of countable models
math/9201246;math.LO;0;0;;J.T.Baldwin,S.Shelah;The primal framework. II. Smoothness
math/9201247;math.LO;0;0;;T.Jech,S.Shelah;On a conjecture of Tarski on products of cardinals
math/9201248;math.LO;0;0;;T.Jech,S.Shelah;A partition theorem for pairs of finite sets
math/9201249;math.LO;0;0;;S.Shelah,L.Stanley;Coding and reshaping when there are no sharps
math/9201250;math.LO,math.GN;0;0;;S.Shelah;Factor = quotient, uncountable Boolean algebras, number of endomorphism and width
math/9201251;math.LO;0;0;;S.Shelah;Cardinal arithmetic for skeptics
math/9201252;math.LO,math.FA;0;0;;M.R.Burke,S.Shelah;Linear liftings for non complete probability space
math/9201253;math.LO;0;0;;M.Kojman,S.Shelah;The universality spectrum of stable unsuperstable theories
math/9201254;math.FA,math.CA,math.DG;0;0;;A.Kriegl,P.W.Michor;A convenient setting for real analytic mappings
math/9201255;math.DG;0;0;;P.W.Michor,H.Schicketanz;A cohomology for vector valued differential forms
math/9201256;math.RT;0;0;;P.W.Michor;The moment mapping for a unitary representation
math/9201257;math.QA;0;0;;P.Lecomte,P.W.Michor,H.Schicketanz;The multigraded Nijenhuis-Richardson Algebra, its universal property and application
math/9201258;math.DG,math.FA;0;3;;O.Gil-Medrano,P.W.Michor,M.Neuwirther;Pseudoriemannian metrics on spaces of bilinear structures
math/9201259;math.DG,math.FA;0;3;;O.Gil-Medrano,P.W.Michor;The Riemannian manifold of all Riemannian metrics
math/9201260;math.AP;0;0;;M.Christ;Some non-analytic-hypoelliptic sums of squares of vector fields
math/9201261;math.AP;0;0;;P.Deift,X.Zhou;A steepest descent method for oscillatory Riemann-Hilbert problems
math/9201262;math.HO;0;0;;M.W.Hirsch,R.S.Palais;Editors' remarks (on two complexity theory surveys in the Bulletin)
math/9201263;math.GT,math.CV;0;0;;L.Keen,C.Series;Pleating coordinates for the Teichmüller space of a punctured torus
math/9201264;math.GR,math.GT;0;0;;M.L.Mihalik,S.T.Tschantz;Semistability of amalgamated products, HNN-extensions, and all one-relator groups
math/9201265;math.GR,math.DS,math.GT;0;0;;J.W.Morgan;$Λ$\<-Trees and Their Applications
math/9201266;math.NA;0;0;;B.N.Parlett;Some basic information on information-based complexity theory
math/9201267;math.CV,math.AG;0;0;;Z.Ran;Lifting of cohomology and unobstructedness of certain holomorphic maps
math/9201268;math.AP;0;0;;M.Struwe;Semilinear wave equations
math/9201269;math.NA;0;0;;J.F.Traub,H.Woźniakowski;Perspectives on information-based complexity
math/9201270;math.DG;0;0;;B.White;Nonunique tangent maps at isolated singularities of harmonic maps
math/9201271;math.DS;0;0;;B.Bielefeld,A.Douady,C.McMullen,J.Milnor,M.Shishikura,F.Tangerman,P.Veerman;Conformal dynamics problem list
math/9201272;math.DS,math.CV;0;0;;J.W.Milnor;Dynamics in one complex variable: introductory lectures
math/9201273;math.DS;0;0;;J.W.Milnor;Remarks on iterated cubic maps
math/9201274;math.DS;0;11;;G.Swiatek;One-dimensional maps and Poincaré metric
math/9201275;math.DS,math-ph,math.MP;0;32;;P.Bleher,M.Lyubich;The Julia sets and complex singularities in hierarchical Ising models
math/9201276;math.DS,math.DG;0;18;;G.Paternain,R.J.Spatzier;New examples of manifolds with completely integrable geodesic flows
math/9201277;math.DS;0;21;;Y.Jiang;Dynamics of certain smooth one-dimensional mappings I: The $C^{1+α}$-Denjoy-Koebe distortion lemma
math/9201278;math.DS;0;15;;Y.Jiang;Dynamics of certain smooth one-dimensional mappings II: geometrically finite one-dimensional mappings
math/9201279;math.DS;0;0;;M.Rees;A partial description of the parameter space of rational maps of degree two: Part 2
math/9201280;math.DS,math.NA;0;28;;M.-H.Kim,S.Sutherland;Polynomial root-finding algorithms and branched covers
math/9201281;math.DS;0;18;;Y.Jiang,T.Morita,D.Sullivan;Expanding direction of the period doubling operator
math/9201282;math.DS;0;0;;M.Shishikura;The Hausdorff dimension of the boundary of the Mandelbrot set and Julia sets
math/9201283;math.DS;0;13;;J.Graczyk,G.Swiatek;Critical circle maps near bifurcation
math/9201284;math.DS;0;28;;E.E.Cawley;The Teichmüller space of an Anosov diffeomorphism of $T^2$
math/9201285;math.DS;0;0;;M.Lyubich;On the Lebesgue measure of the Julia set of a quadratic polynomial
math/9201286;math.DS;0;28;;M.Lyubich;Ergodic theory for smooth one-dimensional dynamical systems
math/9201287;math.DS;0;13;;Y.Jiang;Dynamics of certain smooth one-dimensional mappings III: Scaling function geometry
math/9201288;math.DS;0;14;;Y.Jiang;Dynamics of certain smooth one-dimensional mappings IV: Asymptotic geometry of Cantor sets
math/9201289;math.DS;0;0;;A.M.Blokh;Periods implying almost all periods, trees with snowflakes, and zero entropy maps
math/9201290;math.DS;0;0;;A.M.Blokh;The "spectral" decomposition for one-dimensional maps
math/9201291;math.DS;0;0;;M.Lyubich,J.W.Milnor;The Fibonacci unimodal map
math/9201292;math.DS;0;22;;M.Jakobson,G.Swiatek;Quasisymmetric conjugacies between unimodal maps
math/9201293;math.DS;0;0;;B.Bielefeld,S.Sutherland,F.Tangerman,J.J.P.Veerman;Dynamics of certain non-conformal degree two maps on the plane
math/9201294;math.DS;0;20;;Y.Jiang;On the quasisymmetrical classification of infinitely renormalizable maps: I. Maps with Feigenbaum's topology.
math/9201295;math.DS;0;3;;Y.Jiang;On the quasisymmetrical classification of infinitely renormalizable maps: II. remarks on maps with a bounded type topology.
math/9201296;math.DS;0;0;;A.Poirier;On the realization of fixed point portraits (an addendum to Goldberg, Milnor: Fixed point portraits)
math/9201297;math.DS;0;0;;C.Golé;Periodic orbits for Hamiltonian systems in cotangent bundles
math/9201298;math.DS;0;0;;P.Jones;On removable sets for Sobolev spaces in the plane
math/9201299;math.DG,math.GT;0;19;;L.Keen,B.Maskit,C.Series;Geometric finiteness and uniqueness for Kleinian groups with circle packing limit sets
math/9201300;math.DS;0;0;;M.Martens;The existence of sigma-finite invariant measures, applications to real one-dimensional dynamics
math/9201301;math.QA,math.GT;0;14;;G.Kuperberg;Involutory Hopf algebras and 3-manifold invariants
math/9201302;math.QA,math.GT;0;10;;G.Kuperberg;The quantum G_2 link invariant
math/9201303;math.CO,math.PR;0;0;;D.E.Knuth,R.Motwani,B.Pittel;Stable husbands
math/9201304;math.GR;0;0;;D.E.Knuth;Efficient representation of perm groups
math/9201305;math.CO;0;20;;N.Elkies,G.Kuperberg,M.Larsen,J.Propp;Alternating sign matrices and domino tilings
hep-th/9201029;hep-th;0;19;;R.Kallosh;Supersymmetric Black Holes
hep-th/9201030;hep-th;0;27;;L.A.Ferreira,J.F.Gomes,R.M.Ricotta,A.H.Zimerman;Supersymmetric Construction of W-Algebras from Super Toda and Wznw Theories
hep-th/9201031;hep-th;0;0;;M.Ruiz--Altaba;New Solutions to the Yang--Baxter Equation from Two--Dimensional Representations of $U_q(sl(2))$ at Roots of Unit
hep-th/9201032;hep-th;0;30;;M.J.Martins;The thermodynamic Bethe ansatz for deformed W$A_{N-1}$ conformal field theories
hep-th/9201033;hep-th;0;26;;L.Chekhov,Yu.Makeenko;The Multicritical Kontsevich-Penner Model
hep-th/9201034;hep-th;1;63;hep-th/9109032;K.Itoh,N.Ohta;Spectrum of Two-Dimensional (Super)Gravity
hep-th/9201035;hep-th;0;16;;O.Babelon,M.Talon;Separation of variables for the classical and quantum Neumann model
hep-th/9201036;hep-th;1;71;hep-th/9109032;M.Spiegelglas,S.Yankielowicz;$G/G$--Topological Field Theories by Cosetting $G_k$
hep-th/9201037;hep-th;0;40;;J.Feinberg;String Field Theory for d ≤0 Matrix Models via Marinari-Parisi
hep-th/9201038;hep-th;0;0;;L.Feher,L.O'Raifeartaigh,P.Ruelle,I.Tsutsui;Rational vs Polynomial Character of W$_n^l$-Algebras
hep-th/9201039;hep-th;0;0;;I.Jack,D.R.T.Jones,J.Panvel;Exact Bosonic and Supersymmetric String Black Hole Solutions
hep-th/9201040;hep-th;0;56;;T.Kugo,B.Zwiebach;Target Space Duality as a Symmetry of String Field Theory
hep-th/9201041;hep-th;0;0;;A.Sen;On the Background Independence of String Field Theory: III. Explicit Field Redefinitions
hep-th/9201042;hep-th;0;0;;A.Carlini,M.Martellini;Stabilizing the gravitational action and Coleman's solution to the cosmological constant problem
hep-th/9201043;hep-th;0;0;;A.Carlini,M.Martellini;The phase of scalar field wormholes at one loop in the path integral formulation for Euclidean quantum gravity
hep-th/9201044;hep-th;0;17;;M.A.R.Osorio,M.A.Vazquez-Mozo;Strings below the Planck scale
hep-th/9201045;hep-th;0;9;;R.R.Khuri,H.La;Orbits of a String around a Fivebrane
hep-th/9201046;hep-th;0;14;;R.R.Khuri,H.La;String Motion in Fivebrane Geometry
hep-th/9201047;hep-th;0;0;;D.Lüst,C.Muñoz;Duality-Invariant Gaugino Condensation and One-Loop Corrected Kahler Potentials in String Theory
hep-th/9201048;hep-th;0;54;;A.P.Balachandran,G.Bimonte,K.S.Gupta,A.Stern;The Chern-Simons Source as a Conformal Family and Its Vertex Operators
hep-th/9201049;hep-th;0;20;;E.Smith;Light-Cone Gauge for 1+1 Strings
hep-th/9201050;hep-th;0;0;;H.Lu,C.N.Pope,S.Schrans,K.W.Xu;The Complete Spectrum of the $W_N$ String
hep-th/9201051;hep-th,math.QA;0;16;;M.Bordemann,M.Forger,J.Laartz,U.Schaeper;The Lie-Poisson Structure of Integrable Classical Non-Linear Sigma Models
hep-th/9201052;hep-th;0;0;;J.Maharana,S.mukherji;Gauge Transformations in String Field Theory and canonical Transformation in String Theory
hep-th/9201053;hep-th;0;27;;S.P.de Alwis;Comments on No-Hair Theorems and Stabilty of Blackholes
hep-th/9201054;hep-th;0;12;;M.B.Green;Temperature Dependence of String Theory in the Presence of World-Sheet Boundaries
hep-th/9201055;hep-th,math.QA;0;0;;C.Itzykson,J.-B.Zuber;Addendum to the paper "Combinatorics of the modular group II: the Kontsevich integrals"
hep-th/9201056;hep-th;1;41;hep-th/9109032;E.Witten,B.Zwiebach;Algebraic Structures and Differential Geometry in 2D String Theory
hep-th/9201057;hep-th;0;64;;C.M.Hull;Classical and Quantum W-Gravity
hep-th/9201058;hep-th;0;0;;R.Efraty,V.P.Nair;The Secret Chern-Simons Action for the Hot Gluon Plasma
hep-th/9201059;hep-th;0;19;;S.Coleman,J.Preskill,F.Wilczek;Quantum Hair on Black Holes
hep-th/9201060;hep-th;0;0;;J.M.Lina,P.K.Panigrahi;Lax Pair Formulation of the W-gravity Theories in two Dimensions
hep-th/9201061;hep-th;0;15;;T.Banks,A.Dabolkhar,M.R.Douglas,M.O.Loughlin;Are Horned Particles the Climax of Hawking Evaporation?
hep-th/9201062;hep-th;0;18;;G.Bimonte,P.Salomonson,A.Simoni,A.Stern;Poisson bracket algebra for chiral group elements in the WZNW model
hep-th/9201063;hep-th;0;16;;M.Kamionkowski,J.March-Russell;Are Textures Natural?
hep-th/9201064;hep-th;1;18;hep-th/9109032;J.L.F.Barbón;Perturbing the Ground Ring of 2-D String Theory
hep-th/9201065;hep-th;0;0;;Y.Matsumura,N.Sakai,Y.Tanii;Coupling of Tachyons and Discrete States in $c = 1$ 2-D Gravity
hep-th/9201066;hep-th;0;0;;Y.Matsumura,N.Sakai,Y.Tanii;Interaction of Tachyons and Discrete States in c=1 2-D Quantum Gravity
hep-th/9201067;hep-th;0;22;;G.W.Delius,M.T.Grisaru,D.Zanon;Exact S-Matrices for Nonsimply-Laced Affine Toda Theories
hep-th/9201068;hep-th;0;0;;M.Martellini,M.Spreafico,K.Yoshida;On the Black-Hole Conformal Field Theory Coupled to the Polyakov's String Theory. A Non Perturbative Analysis
hep-th/9201069;hep-th;0;0;;M.Martellini,M.Spreafico,K.Yoshida;A continuum string model for $D>1$
hep-th/9201070;hep-th;0;41;;E.Nissimov,S.Pacheva,I.Vaysburd;Induced $W_∞$ Gravity as a WZNW Model
hep-th/9201071;hep-th,math.RT;0;0;;N.Chair,V.K.Dobrev,H.Kanno;SO(2,C) invariant ring structure of BRST cohomology and singular vectors in 2D gravity with c < 1 matter
hep-th/9201072;hep-th;0;0;;S.Kachru;Quantum Rings and Recursion Relations in 2D Quantum Gravity
hep-th/9201073;hep-th;0;0;;A.Lyons;All-orders wormhole vertex operators from the Wheeler-deWitt equation
hep-th/9201074;hep-th;0;0;;J.Russo,L.Susskind,L.Thorlacius;Black Hole Evaporation in 1+1 Dimensions
hep-th/9201075;hep-th;0;0;;K.Amano,S.Higuchi;Topology change in ISO(2,1) Chern-Simons gravity
hep-th/9201076;hep-th;0;16;;M.Doyle;Dilaton Contact Terms in the Bosonic and Heterotic Strings
hep-th/9201077;hep-th;1;22;hep-th/9109032;Vl.S.Dotsenko;Remarks on the Physical States and the Chiral Algebra of 2D Gravity Coupled to $C ≤1$ Matter
hep-th/9201078;hep-th;0;0;;P.C.Argyres,K.R.Dienes,S.-H.H.Tye;New Jacobi-Like Identities for Z_k Parafermion Characters
hep-th/9201079;hep-th;0;17;;M.Bauer,N.Sochen;Fusion and singular vectors in A1{(1)} highest weight cyclic modules
hep-th/9201080;hep-th;0;45;;P.Furlan,A.Ch.Ganchev,R.Paunov,V.B.Petkova;Solutions of the Knizhnik - Zamolodchikov Equation with Rational Isospins and the Reduction to the Minimal Models
hep-th/9201081;hep-th;0;0;;A.R.Lugo;Comments on Gauged WZW Models
hep-lat/9202001;hep-lat;0;0;;W.Janke,B.A.Berg,M.Katoot;Monte Carlo Calculation of the Surface Free Energy for the 2d 7-state Potts Model, and an Estimate for 4d SU(3) Gauge Theory
hep-lat/9202002;hep-lat;0;11;;J.Kiskis,R.Narayanan,P.Vranas;Random Walks and the Correlation Length Critical Exponent in Scalar Quantum Field Theory
hep-lat/9202003;hep-lat;0;0;;S.Gottlieb,U.M.Heller,A.D.Kennedy,J.B.Kogut,A.Krasnitz,W.Liu,R.L.Renken,D.K.Sinclair,R.L.Sugar,D.Toussaint,K.C.Wang;Thermodynamics of Lattice QCD with 2 Light Dynamical (Staggered) Quark Flavours on a $16^3×8$ Lattice
hep-lat/9202004;hep-lat;0;13;;B.A.Berg,T.Neuhaus;Multicanonical Ensemble: A New Approach to Simulate First-order Phase Transitions
hep-th/9202001;hep-th;0;37;;N.Read,G.Moore;Fractional quantum Hall effect and nonabelian statistics
hep-th/9202002;hep-th;2;52;hep-th/9109001,hep-th/9110052;S.-wei.Chung,S.-H.H.Tye;Chiral Gauged WZW Theories and Coset Models in Conformal Field Theory
hep-th/9202003;hep-th;0;27;;M.Kamionkowski,J.March-Russell;Planck-Scale Physics and the Peccei-Quinn Mechanism
hep-th/9202004;hep-th;0;21;;S.B.Giddings,A.Strominger;Dynamics of Extremal Black Holes
hep-th/9202005;hep-th;0;0;;D.Gershon;Exact Solutions of Four Dimensional Black Holes in String Theory
hep-th/9202006;hep-th;0;25;;L.Chekhov,Yu.Makeenko;A Hint on the External Field Problem for Matrix Models
hep-th/9202007;hep-th;2;27;hep-th/9109001,hep-th/9110052;P.C.Argyres,J.M.Grochocinski,S.-H.H.Tye;Construction of the K=8 Fractional Superconformal Algebras
hep-th/9202008;hep-th;1;58;hep-th/9109032;P.Horava;Two Dimensional String Theory and the Topological Torus
hep-th/9202009;hep-th;0;0;;Y.Imamura,M.Sakamoto,T.Sasada,M.Tabuse;String Theories on the Asymmetric Orbifolds with Twist-Untwist Intertwining Currents
hep-th/9202010;hep-th;0;6;;G.Nagao;Toward a Conformal Field Theory for the Quantum Hall Effect
hep-th/9202011;hep-th;1;74;hep-th/9108005;P.Fendley,K.Intriligator;Scattering and Thermodynamics of Integrable N=2 Theories
hep-th/9202012;hep-th;0;1;;S.Iso,D.Karabali,B.Sakita;One-Dimensional Fermions as Two-Dimensional Droplets Via Chern-Simons Theory
hep-th/9202013;hep-th;0;49;;V.Spiridonov;Deformed Conformal and Supersymmetric Quantum Mechanics
hep-th/9202014;hep-th;0;20;;C.F.E.Holzhey,F.Wilczek;Black Holes as Elementary Particles
hep-th/9202015;hep-th;0;17;;B.Zwiebach;Interpolating String Field Theories
alg-geom/9202001;alg-geom,math.AG;0;25;;S.Katz;Rational Curves on Calabi-Yau Threefolds
hep-th/9202016;hep-th;0;0;;N.Linden,M.Perry;Path Intergals and Perturbative Expansions for Non-Compact Symmetric Spaces
alg-geom/9202002;alg-geom,math.AG;0;34;;S.Katz,D.R.Morrison;Gorenstein Threefold Singularities with Small Resolutions via Invariant Theory for Weyl Groups
hep-th/9202017;hep-th,math.AG;0;25;;S.Katz;Rational Curves on Calabi-Yau Threefolds
hep-th/9202018;hep-th;1;35;hep-th/9202054;B.Bruegmann,R.Gambini,J.Pullin;Jones Polynomials for Intersecting Knots as Physical States of Quantum Gravity
hep-th/9202019;hep-th;0;0;;S.Ben-Menahem;D=0 Matrix Model as Conjugate Field Theory
hep-th/9202020;hep-th;0;30;;F.Ravanini;Thermodynamic Bethe Ansatz for G_k x G_l / G_{k+l} Coset Models Perturbed by Their φ_{1,1,Adj} Operator
hep-th/9202021;hep-th;1;28;hep-th/9109032;E.Verlinde;The Master Equation of 2D String Theory
hep-th/9202022;hep-th;1;94;hep-th/9202054;L.Smolin;Recent Developments in Non-Perturbative Quantum Gravity
hep-th/9202023;hep-th;0;18;;R.H.Price,J.Pullin;The Emergence of Radiation from Gravitational Potential Wells: The Absence of $ωM$ Effects
hep-th/9202024;hep-th;0;38;;C.Ting,C.H.Lai;Spinning Braid Group Representation and the Fractional Quantum Hall Effect
math/9202201;math.CV;0;0;;F.Haslinger;Szegö kernels for certain unbounded domains in $\Bbb C^2$
hep-th/9202025;hep-th;0;25;;J.W.van Holten;BRST Field Theory of Relativistic Particles
hep-th/9202026;hep-th;0;0;;G.Ferretti,S.G.Rajeev;$CP^N$ Model With a Chern-Simons Term
hep-th/9202027;hep-th;0;5;;G.Nagao;A Conformal Field Theory for the Quantum Hall Effect
alg-geom/9202003;alg-geom,math.AG;0;0;;Y.-G.Ye;Complex Contact Threefolds and Their Contact Curves
hep-th/9202028;hep-th;0;0;;C.Ahn;RG Flows of Non-Unitary Minimal CFTs
hep-th/9202029;hep-th;0;0;;A.Balatsky;Spin Singlet Quantum Hall Effect and Nonabelian Landau-Ginzburg Theory
hep-th/9202030;hep-th;0;40;;L.F.Cugliandolo,G.L.Rossini,F.A.Schaposnik;Stochastic Quantization of the Chern-Simons Theory
hep-th/9202031;hep-th;0;0;;S.Mignemi,D.L.Wiltshire;Black Holes in Higher Derivative Gravity Theories
hep-th/9202032;hep-th;0;0;;H.Awata;Screening Currents Ward Identity and Integral Formulas for the WZNW Correlation Functions
hep-th/9202033;hep-th;0;22;;G.Papadopoulos,B.Spence;The Canonical Structure of Wess-Zumino-Witten Models
alg-geom/9202004;alg-geom,math.AG;0;40;;D.R.Morrison;Mirror symmetry and rational curves on quintic threefolds: a guide for mathematicians
hep-th/9202034;hep-th;0;74;;T.R.Klassen,E.Melzer;Kinks in Finite Volume
alg-geom/9202005;alg-geom,math.AG;0;0;;G.M.Ziegler;On the difference between real and complex arrangements
hep-th/9202035;hep-th;0;14;;A.Bilal;Remarks on the BRST-cohomology for $c_M > 1$ matter coupled to ``Liouville gravity"
alg-geom/9202006;alg-geom,math.AG;0;21;;C.LeBrun,Y.-S.Poon;Twistors, Kaehler Manifolds, and Bimeromorphic Geometry II
alg-geom/9202007;alg-geom,math.AG;0;24;;T.Oda;The algebraic de Rham theorem for toric varieties
hep-th/9202036;hep-th;0;27;;P.S.Howe,G.Papadopoulos;Holonomy groups and W-symmetries
hep-th/9202037;hep-th;0;0;;D.R.Brill;Splitting of an Extremal Reissner-Nordström Throat via Quantum Tunneling
hep-th/9202038;hep-th;0;25;;L.F.Cugliandolo,F.A.Schaposnik,H.Vucetich;A Topological Model for Two Dimensional Gravity Coupled to Matter
hep-th/9202039;hep-th;0;11;;M.Kreuzer,H.Skarke;On the Classification of Quasihomogeneous Functions
alg-geom/9202008;alg-geom,math.AG;0;0;;W.D.Neumann,L.V.Thanh;On irregular links at infinity of algebraic plane curves
hep-th/9202040;hep-th;0;0;;J.M.Figueroa-O'Farrill,E.Ramos;The Classical Limit of W-Algebras
hep-th/9202041;hep-th;0;10;;M.Lassig;Exact Critical Exponents of the Staircase Model
alg-geom/9202009;alg-geom,math.AG;0;7;;V.B.Mehta,W.van der Kallen;On a Grauert-Riemenschneider vanishing theorem for Frobenius split varieties in characteristic p
alg-geom/9202010;alg-geom,math.AG;0;0;;J.B.Little;Another Relation Between Approaches to the Schottky Problem
hep-th/9202042;hep-th;0;16;;M.J.Martins;The two-dimensional O(3) nonlinear $σ$-model at finite temperature
hep-th/9202043;hep-th;0;18;;H.O.Girotti,M.Gomes,V.O.Rivelles;Chiral Bosons Through Linear Constraints
hep-th/9202044;hep-th,math.GR,math.QA;0;0;;F.Quinn;Representation theory, topological field theory, and the Andrews-Curtis conjecture
hep-th/9202045;hep-th;0;10;;A.Lahiri;An Alternative Scenario for Non-Abelian Quantum Hair
hep-th/9202046;hep-th;0;0;;L.E.Ibanez,D.Luest;Duality Anomaly Cancellation, Minimal String Unification and the Effective Low-Energy Lagrangian of 4-D Strings
hep-th/9202047;hep-th,math.QA;0;46;;D.Altschuler,A.Coste;Quasi-Quantum Groups, Knots, Three-Manifolds, and Topological Field Theory
alg-geom/9202011;alg-geom,math.AG;0;0;;P.F.Stiller;The Geometry and Arithmetic of Elliptic Surfaces
hep-th/9202048;hep-th;0;18;;A.Moroz;Bloch Electron in a Magnetic Field : Diagonalization of Tight-Binding Models
hep-th/9202049;hep-th;0;55;;I.Ya.Aref'eva,A.P.Zubarev;Non-critical NSR string field theory and discrete states interaction in 2D supergravity
hep-th/9202050;hep-th;0;45;;J.D.Cohn,H.Dykstra;The Marinari-Parisi Model and Collective Field Theory
hep-th/9202051;hep-th;0;19;;P.Berglund,B.R.Greene,T.Hübsch;Classical {\it vs.} Landau-Ginzburg Geometry of Compactification
hep-th/9202052;hep-th;0;0;;A.P.Balachandran,W.D.McGlinn,L.O'Raifeartaigh,S.Sen,R.D.Sorkin,A.M.Srivastava;Topological Spin-Statistics Theorem for Strings
alg-geom/9202012;alg-geom,math.AG;0;2;;G.R.Kempf;Cohomology of coherent sheaves on a proper scheme
alg-geom/9202013;alg-geom,math.AG;0;0;;G.R.Kempf;Deformations of Semi-Euler Characteristics
hep-th/9202053;hep-th;0;26;;A.Ashtekar,C.J.Isham;Representations of the holonomy algebras of gravity and non-Abelian gauge theories
hep-th/9202054;hep-th;0;27;;A.Ashtekar,C.Rovelli,L.Smolin;Gravitons and Loops
alg-geom/9202014;alg-geom,math.AG;0;0;;M.Schlichenmaier;Degenerations of generalized KNN algebras on tori
alg-geom/9202015;alg-geom,math.AG;0;8;;E.Colombo,B.van Geemen;Note on curves in a Jacobian
hep-th/9202055;hep-th;0;28;;A.Mikovic;Canonical Quantization of 2d Gravity Coupled to c<1 Matter
hep-th/9202056;hep-th;0;0;;D.B.Fairlie,J.Govaerts;Universal Field Equations with Reparametrisation Invariance
hep-th/9202057;hep-th;0;0;;A.P.Polychronakos;Exchange Operator Formalism for Integrable Systems of Particles
alg-geom/9202016;alg-geom,math.AG;0;16;;G.Mikhalkin;Congruences for real algebraic curves on an ellipsoid
hep-th/9202058;hep-th;0;33;;K.Ito,J.O.Madsen;Hamiltonian Reduction and Classical Extended Superconformal Algebras
hep-th/9202059;hep-th;0;33;;M.K.Gaillard,T.R.Taylor;Axion Couplings and Effective Cut-Offs in Superstring Compactifications
alg-geom/9202017;alg-geom,math.AG;0;12;;G.Mikhalkin;Extensions of Rokhlin congruence for curves on surfaces
hep-th/9202060;hep-th;0;0;;H.Lu,C.N.Pope,S.Schrans,X.J.Wang;On Sibling and Exceptional W Strings
hep-th/9202061;hep-th;0;23;;P.Bowcock;Exceptional Superconformal Algebras
hep-th/9202062;hep-th;0;0;;M.Wolf,B.Zwiebach;The Plumbing of Minimal Area Metrics
hep-th/9202063;hep-th;1;35;hep-th/9202054;A.Ashtekar,C.Rovelli;A Loop Representation for the Quantum Maxwell Field
hep-th/9202064;hep-th;0;34;;F.A.Schaposnik;Anomalies and Deconfinement
alg-geom/9202018;alg-geom,math.AG;0;9;;S.Katz;Arithmetically Cohen-Macaulay Curves cut out by Quadrics
hep-th/9202065;hep-th;0;0;;J.Avan,A.Jevicki;Algebraic Structures and Eigenstates for Integrable Collective Field Theories
alg-geom/9202019;alg-geom,math.AG;0;0;;F.DeMeyer,T.Ford,R.Miranda;The cohomological Brauer group of a toric variety
hep-th/9202066;hep-th;0;0;;V.G.J.Rodgers;QCD Instantons and 2D Surfaces
hep-th/9202067;hep-th;1;59;hep-th/9205068;M.Cvetic;Stringy Domain Walls and Other Stringy Topological Defects
hep-th/9202068;hep-th;0;17;;R.B.Mann,M.S.Morris,S.F.Ross;Properties of Asymptotically Flat Two-Dimensional Black Holes
hep-th/9202069;hep-th;0;30;;G.W.Delius,M.T.Grisaru,D.Zanon;Quantum Conserved Currents in Affine Toda Theories
hep-th/9202070;hep-th;0;27;;H.G.Kausch,G.M.T.Watts;Duality in Quantum Toda theory and W-algebras
hep-th/9202071;hep-th;0;16;;G.Immirzi;The reality conditions for the new canonical variables of General Relativity
alg-geom/9202020;alg-geom,math.AG;0;0;;G.Niesi,L.Robbiano;Disproving Hibi's Conjecture with CoCoA or Projective Curves with bad Hilbert Functions
hep-th/9202072;hep-th;0;0;;X.Shen;W-Infinity and String Theory
alg-geom/9202021;alg-geom,math.AG;0;7;;D.Bayer,A.Galligo,M.Stillman;Grobner bases and extension of scalars
hep-th/9202073;hep-th;0;0;;P.G.O.Freund,A.V.Zabrodin;$Z_n$ Baxter Models and Quantum Symmetric Spaces
alg-geom/9202022;alg-geom,math.AG;0;42;;R.Hain;Classical Polylogarithms
alg-geom/9202023;alg-geom,math.AG;0;39;;J.Dupont,R.Hain,S.Zucker;Regulators and characteristic classes of flat bundles
hep-th/9202074;hep-th;1;31;hep-th/9108006;D.Boulatov;A Model of Three-Dimensional Lattice Gravity
alg-geom/9202024;alg-geom,math.AG;0;0;;A.Beauville;Sur la cohomologie de certains espaces de modules de fibrés vectoriels
math/9202202;math.FA;0;0;;D.H.Fremlin,J.Mendoza;On the integration of vector-valued functions
hep-th/9202075;hep-th;0;0;;M.Alford,A.Strominger;S-Wave Scattering of Charged Fermions by a Magnetic Black Hole
alg-geom/9202025;alg-geom,math.AG;0;0;;A.Grassi;The Singularities of the parameter surface of a minimal elliptic threefold
hep-th/9202076;hep-th;0;41;;L.Smolin;The G_Newton --> 0 Limit of Euclidean Quantum Gravity
hep-th/9202077;hep-th;0;14;;B.S.Balakrishna,K.C.Wali;Non-Abelian Monopoles Coupled to Gravity
hep-th/9202078;hep-th;2;27;hep-th/9109032,hep-th/9111028;Z.Yang;A Possible Black Hole Background in c=1 Matrix Model
hep-th/9202079;hep-th;0;0;;A.Ashtekar,C.Rovelli,L.Smolin;Self Duality and Quantization
hep-th/9202080;hep-th;0;22;;Y.Itoh,Y.Tanii;Schwinger-Dyson Equations of Matrix Models for Open and Closed Strings
hep-th/9202081;hep-th;0;0;;M.Takama;Matrix model with superconformal symmetry
hep-th/9202082;hep-th;0;24;;H.Hinrichsen,V.Rittenberg;The Pokrovski-Talapov Phase Transitions and Quantum Groups
hep-th/9202083;hep-th;0;0;;M.Sakamoto,M.Tabuse;The General Class of String Theories on Orbifolds
hep-th/9202084;hep-th;0;0;;T.Horiguchi,M.Sakamoto,M.Tabuse;Cocycle Properties of String Theories on Orbifolds
hep-th/9202085;hep-th;0;21;;C.Callan,A.Felce,D.Freed;Critical Theories of the Dissipative Hofstadter Model
hep-th/9202086;hep-th;0;0;;E.Sezgin;Area-Preserving Diffeomorphisms, w_∞Algebras and w_∞Gravity
alg-geom/9202026;alg-geom,math.AG;0;29;;D.R.Morrison;Picard-Fuchs equations and mirror maps for hypersurfaces
hep-th/9202087;hep-th;0;0;;R.Saroja,A.Sen;Picture Changing Operators in Closed Fermionic String Field Theory
alg-geom/9202027;alg-geom,math.AG;0;0;;K.H.Paranjape;Cohomological and Cycle-theoretic connectivity
hep-th/9202088;hep-th,math.GT;0;0;;D.H.Gottlieb,G.Samaranayake;The Index of discontinuous Vector Fields: Topological Particles and Vector Fields
hep-th/9202089;hep-th;0;0;;E.Abdalla,M.C.B.Abdalla,D.Dalmazi,K.Harada;Correlation Functions in non critical (super) string theory
hep-th/9202090;hep-th;2;46;0809.0907,0809.0927;B.M.Visser;From wormhole to time machine: Comments on Hawking's Chronology Protection Conjecture
alg-geom/9202028;alg-geom,hep-th,math.AG;0;4;;A.A.Voronov;Complex Divisors on Algebraic Curves and Some Applications to String Theory
math/9202203;math.FA;0;18;;S.Geiss;Lower estimates of random unconditional constants of Walsh-Paley martingales with values in banach spaces
math/9202204;math.FA;0;0;;D.E.Alspach,S.Argyros;Complexity of weakly null sequences
math/9202205;math.LO;0;0;;T.Hyttinen,S.Shelah;Constructing strongly equivalent nonisomorphic models for unsuperstable theories. Part B
math/9202206;math.DG,math.FA;0;2;;A.Kriegl,P.W.Michor;Aspects of the theory of infinite dimensional manifolds
math/9202207;math.DG;0;0;;P.W.Michor;Graded derivations of the algebra of differential forms associated with a connection
math/9202208;math.DG;0;2;;V.Cervera,F.Mascaró,P.W.Michor;The action of the diffeomorphism group on the space of immersions
math/9202209;math.DS;0;11;;J.Graczyk,G.Swiatek,F.Tangerman,J.J.P.Veerman;Scalings in circle maps III
math/9202210;math.DS;0;0;;J.W.Milnor,A.Poirier;Hyperbolic components in spaces of polynomial maps
hep-th/9202091;hep-th;0;24;;A.Berkovich,C.Gomez,G.SIERRA;On a New Class of Integrable Models
hep-th/9202092;hep-th;0;52;;P.Ginsparg,F.Quevedo;Strings on Curved Spacetimes: Black Holes, Torsion, and Duality
hep-ph/9203201;hep-ph;0;43;;M.Dine,R.G.Leigh,P.Huet,A.D.Linde,D.A.Linde;Comments on the Electroweak Phase Transition
hep-th/9203001;hep-th;0;0;;J.Morse,R.Schimmrigk;Topological Phases of the Heterotic String
hep-lat/9203001;hep-lat,hep-ph;0;9;;K.M.Bitar,P.M.Vranas;Is there a $ρ$ in the O(4) $λφ^4_4$ theory?
hep-lat/9203002;hep-lat;1;7;hep-lat/9202004;U.Hansmann,B.A.Berg,T.Neuhaus;Multimagnetical Simulations
hep-th/9203002;hep-th;0;22;;Y.Tanii,S.-ichi.Yamaguchi;Disk Amplitudes in Two-Dimensional Open String Theories
hep-th/9203003;hep-th;0;18;;F.Colomo,A.Koubek,G.Mussardo;The Sub-leading Magnetic Deformation of the Tricritical Ising Model in 2D as RSOS Restriction of the Izergin-Korepin Model
hep-th/9203004;hep-th;0;0;;A.N.Kirillov,P.Mathieu,D.Senechal,M.Walton;Can fusion coefficients be calculated from the depth rule ?
hep-th/9203005;hep-th;1;30;hep-th/9109015;K.N.Anagnostopoulos,M.J.Bowick;Unitary One Matrix Models: String Equations and Flows
hep-th/9203006;hep-th;0;9;;K.Kamimura,S.Makita,T.Fukuyama;Mtric from Non-Metric Action of Gravity
hep-th/9203007;hep-th;0;31;;D.Giulini,J.Louko;No-Boundary Theta-Sectors in Spatially Flat Quantum Cosmology
hep-th/9203008;hep-th;1;26;hep-th/9109032;A.Giveon,A.Shapere;Gauge Symmetries of the N=2 String
hep-th/9203009;hep-th;1;39;hep-th/9109032;J.Ambjorn,L.Chekhov,Yu.Makeenko;Higher Genus Correlators from the Hermitian One-Matrix Model
hep-th/9203010;hep-th;0;0;;S.Mukherji;On The Interpolating Solutions of Strings in Different Backgrounds
hep-th/9203011;hep-th,math.QA;0;19;;D.Arnaudon;Fusion Rules and R-Matrices For Representations of $SL(2)_q$ at Roots of Unity
alg-geom/9203001;alg-geom,math.AG;0;0;;S.Zube;Exceptional linear systems on curves on Enriques surfaces
hep-th/9203012;hep-th;2;69;hep-th/9109027,hep-th/9109032;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;Measuring the $W$-hair of String Black Holes
hep-th/9203013;hep-th;0;17;;T.R.Govindarajan,R.Shankar,N.Shaji,M.Sivakumar;Is the $O(3) σ$ Model with the Hopf Term Exactly Equivalent to a Higher Spin Theory?
hep-th/9203014;hep-th;0;17;;L.N.Chang,C.Soo;Brst Cohomology and Invariants of 4D Gravity in Ashtekar Variables
hep-th/9203015;hep-th;0;23;;N.Maggiore,P.Provero;Chiral Current Algebras in Three--Dimensional Bf--Theory with Boundary
hep-th/9203016;hep-th;0;0;;G.Kleppe,R.P.Woodard;Nonlocal Yang-Mills
hep-th/9203017;hep-th;0;0;;J.Mickelsson;Current algebras and light-cone quantization in 3+1 dimensions
math/9203201;math.CV;0;0;;E.Bedford,S.Pinchuk;Domains in $\cx {n+1}$ with Noncompact Automorphism Group. II
math/9203202;math.DG;0;4;;P.W.Michor;The relation between systems and associated bundles
hep-th/9203018;hep-th;0;0;;L.J.Romans;Supersymmetric, cold and lukewarm black holes in cosmological Einstein-Maxwell theory
hep-ph/9203202;hep-ph;0;0;;C.P.Burgess,J.Cline,M.Luty;A Natural Framework for Solar and 17 keV Neutrinos
hep-ph/9203203;hep-ph;0;55;;M.Dine,R.Leigh,P.Huet,A.Linde,D.Linde;Towards the Theory of Cosmological Phase Transitions
hep-th/9203019;hep-th;0;35;;S.Dalley;The Weingarten Model a la Polyakov
hep-th/9203020;hep-th;0;7;;J.Laartz;The Extension Structure of 2D Massive Current Algebras
hep-th/9203021;hep-th;0;37;;J.Gomis,H.Suzuki;Covariant Currents in N=2 Super-Liouville Theory
hep-th/9203022;hep-th;0;0;;C.Johnson,T.Morris,B.Spence;Stable Non--Perturbative Minimal Models Coupled to 2D Quantum Gravity
hep-ph/9203204;hep-ph;2;195;hep-th/9109053,hep-th/9205068;F.Zwirner;The quest for low-energy supersymmetry and the role of high-energy $e^+e^-$ colliders
hep-th/9203023;hep-th;0;17;;G.W.Gibbons,M.E.Ortiz,F.R.Ruiz,T.M.Samols;Semilocal strings and monopoles
hep-ph/9203205;hep-ph;0;0;;O.F.Hernandez;Extended Color Models with a Heavy Top Quark
hep-ph/9203206;hep-ph;0;36;;R.Holman,S.D.H.Hsu,T.Kephart,E.Kolb,R.Watkins,L.Widrow;Solutions to the strong CP problem in a world with gravity
hep-th/9203024;hep-th;0;0;;H.Lu,C.N.Pope,S.Schrans,X.J.Wang;New Realisations of W Algebras and W Strings
hep-th/9203025;hep-th;3;80;hep-th/9109053,hep-th/9110023,hep-th/9205068;J.Lopez,D.Nanopoulos,K.Yuan;The Search for a realistic flipped SU(5) string model
hep-th/9203026;hep-th,math.QA;0;48;;M.Blau;The Mathai-Quillen Formalism and Topological Field Theory
hep-ph/9203207;hep-ph;0;0;;P.Haagensen,J.I.Latorre;Differential Renormalization of Massive Quantum Field Theories
hep-ph/9203208;hep-ph;0;27;;E.G.L.K.J.Terning;Monopole annihilation at the electroweak scale---Not!
hep-th/9203027;hep-th;0;22;;C.K.Zachos;Altering the Symmetry of Wavefunctions in Quantum Algebras and Supersymmetry
hep-th/9203028;hep-th;0;0;;A.Pasquinucci;A note on the Zakharov-Shabat topological model
hep-th/9203029;hep-th;0;19;;K.Haller,E.Lombridas;Canonical Quantization of $(2+1)$ Dimensional Qed with Topological Mass Term
hep-th/9203030;hep-th;0;36;;I.K.Kostov,M.Staudacher;Multicritical Phases of the O(n) Model on a Random Lattice
hep-ph/9203209;hep-ph;0;0;;R.Holman,T.W.B.Kibble,S.-J.Rey;How Efficient Is The Langacker-Pi Mechanism of Monopole Annihilation?
hep-th/9203031;hep-th;1;42;hep-th/9111001;P.Horava;Two Dimensional Stringy Black Holes with One Asymptotically Flat Domain
hep-th/9203032;hep-th;0;0;;R.Brooks;Relating Scattering Amplitudes in Bosonic and Topological String Theories
math/9203203;math.DS;0;11;;E.E.Cawley;The Teichmüller space of the standard action of $SL(2,Z)$ on $T^2$ is trivial
hep-th/9203033;hep-th;0;0;;A.A.Tseytlin;Cosmological solutions with dilaton and maximally symmetric space in string theory
hep-th/9203034;hep-th;0;0;;K.Takasaki;Volume-preserving diffeomorphisms in integrable deformations of selfdual gravity
hep-th/9203035;hep-th;0;24;;C.Gomez,G.Sierra;New Integrable Deformations of Higher Spin Heisenberg-Ising Chains
hep-th/9203036;hep-th;0;22;;G.Aldazabal,J.M.Maldacena;On the quantization of the N=2 supersymmetric non linear sigma model
hep-th/9203037;hep-th,math.QA,nlin.SI,solv-int;0;12;;I.T.Ivanov,D.B.Uglov;R-matrices for the semicyclic representations of U_q sl^(2)
hep-th/9203038;hep-th;0;19;;F.D.Jonghe,R.Siebelink,W.Troost;Nonlocal regularisation and two-dimensional induced actions
hep-ph/9203210;hep-ph;2;51;hep-ph/9801208,hep-ph/9801209;F.del Aguila,M.Martinez,M.Quiros;Precision bounds on $m_H$ and $m_t
hep-ph/9203211;hep-ph;0;0;;A.Rebhan;Comment on ``Damping of energetic gluons and quarks in high-temperature QCD''
hep-ph/9203212;hep-ph;0;32;;L.M.Krauss,S.-J.Rey;Spontaneous CP Violation at the Electroweak Scale
hep-th/9203039;hep-th;0;27;;J.-L.Gervais,M.V.Saveliev;Black Holes from Non-Abelian Toda Theories
hep-ph/9203213;hep-ph;0;33;;E.Gates,L.M.Krauss,M.White;Solar Neutrino Data and Its Implications
hep-ph/9203214;hep-ph;0;54;;A.Linde;Strings, Textures, Inflation and Spectrum Bending
hep-th/9203040;hep-th;0;23;;B.Bruegmann,R.Gambini,J.Pullin;How the Jones Polynomial Gives Rise to Physical States of Quantum General Relativity
hep-th/9203041;hep-th;0;44;;J.Barbour,L.Smolin;Extremal variety as the foundation of a cosmological quantum theory
hep-th/9203042;hep-th;1;11;hep-th/9111056;B.Birnir,S.B.Giddings,J.A.Harvey,A.Strominger;Quantum Black Holes
hep-th/9203043;hep-th;0;19;;S.Kharchev,A.Marshakov,A.Mironov,A.Morozov;Generalized Kontsevich Model Versus Toda Hierarchy and Discrete Matrix Models
hep-th/9203044;hep-th;0;37;;A.Marshakov,A.Mironov,A.Morozov,M.Olshanetsky;$c = r_g$ Theories of $W_G$-Gravity: The Set of Observables as a Model of Simply Laced $G$
hep-th/9203045;hep-th;0;0;;E.S.Fradkin,V.Y.Linetsky;Results of the classification of superconformal algebras in two dimensions
hep-th/9203046;hep-th;0;17;;F.A.Bais,P.van Driel,M.de Wild Propitius;Quantum symmetries in discrete gauge theories
hep-th/9203047;hep-th;0;21;;F.A.Bais,P.van Driel,M.de Wild Propitius;Anyons in discrete gauge theories with Chern-Simons terms
hep-th/9203048;hep-th;0;0;;F.Bonechi,E.Celeghini,R.Giachetti,E.Sorace,M.Tarlini;Quantum Galilei Group as Symmetry of Magnons
hep-th/9203049;hep-th;0;19;;H.Fukutaka;Path-Integral Measure of Linearized Gravity in Curved Spacetime
hep-th/9203050;hep-th;0;33;;D.Christensen,R.B.Mann;The Causal Structure of Two-Dimensional Spacetimes
hep-ph/9203215;hep-ph;0;0;;C.P.Burgess,D.London;Light Spin-One Particles Imply Gauge Invariance
hep-ph/9203216;hep-ph;0;0;;C.P.Burgess,D.London;Uses and Abuses of Effective Lagrangians
hep-ph/9203217;hep-ph;0;12;;D.B.DeLaney,S.Jadach,Ch.Shio,G.Siopsis,B.F.L.Ward;Multiple photon effects in fermion-(anti)fermion scattering at SSC energies
hep-th/9203051;hep-th;0;27;;A.Galperin,E.Sokatchev;A twistor-like D=10 superparticle action with manifest N=8 world-line supersymmetry
hep-th/9203052;hep-th;0;0;;S.W.Hawking;Evaporation of Two Dimensional Black Holes
hep-th/9203053;hep-th;0;16;;M.Carfora,M.Martellini,A.Marzuoli;Combinatorial and topological phase structure of non-perturbative n-dimensional quantum gravity
hep-ph/9203218;hep-ph;0;0;;M.A.Luty;Electroweak Symmetry Breaking via a Technicolor Nambu--Jona-Lasinio Model
hep-th/9203054;hep-th;0;18;;L.Susskind,L.Thorlacius;Hawking Radiation and Back-Reaction
hep-th/9203055;hep-th;0;0;;G.Bonacina,A.Gamba,M.Martellini;Interacting Euclidean 3D Quantum Gravity
alg-geom/9203002;alg-geom,math.AG;0;27;;Y.Li,M.Mulase;Prym Varieties and Integrable Systems
alg-geom/9203003;alg-geom,math.AG;0;4;;T.J.Ford;Computing the Cohomological Brauer Group of a Toric Variety
alg-geom/9203004;alg-geom,math.AG;0;0;;E.Bifet,F.Ghione,M.Letizia;On the Abel-Jacobi Map for Divisors of Higher Rank on a Curve
hep-th/9203056;hep-th;0;0;;D.Cangemi,R.Jackiw;Gauge Invariant Formulations of Lineal Gravity
hep-th/9203057;hep-th;1;18;hep-th/9112065;M.Visser;Dirty blackholes: Thermodynamics and horizon structure
hep-th/9203058;hep-th;0;21;;J.Distler,M.Doyle;World-Sheet Supersymmetry Without Contact Terms
hep-th/9203059;hep-th;0;43;;S.B.Giddings;Black Holes and Massive Remnants
hep-th/9203060;hep-th,hep-ph;0;36;;G.Moore,R.Plesser;Classical Scattering in $1+1$ Dimensional String Theory
hep-th/9203061;hep-th;0;22;;G.Moore;Gravitational Phase Transitions and the Sine-Gordon Model
hep-th/9203062;hep-th;0;37;;D.A.Depireux;A note on the KP hierarchy
hep-th/9203063;hep-th;0;0;;D.P.Jatkar;The Spectrum of Sl(2, R)/U(1) Black Hole Conformal Field Theory
hep-th/9203064;hep-th;0;16;;C.Destri,H.J.de Vega;New Approach to Thermal Bethe Ansatz
hep-th/9203065;hep-th;0;11;;C.Destri,H.J.de Vega;Bethe Ansatz and Quantum Groups: The Light--Cone Approach. II. From RSOS($p+1$) models to $p-$restricted Sine--Gordon Field Theories
hep-ph/9203219;hep-ph;0;102;;M.Drees,R.M.Godbole;Aspects of Two-Photon Physics at Linear e+e- Colliders
alg-geom/9203005;alg-geom,math.AG;0;0;;A.Libgober;Homotopy groups of the complements to singular hypersurfaces,II
hep-th/9203066;hep-th;1;24;hep-th/9111016;S.Cecotti,C.Vafa;Massive Orbifold
hep-th/9203067;hep-th;0;0;;R.Lano,V.G.J.Rodgers;Applications of W-algebras to BF theories, QCD and 4D Gravity
hep-th/9203068;hep-th;0;0;;V.G.J.Rodgers;$W_∞$ and Anomalies of Self-Dual Einstein Theories
hep-th/9203069;hep-th,math.QA;0;31;;L.Rozansky,H.Saleur;S and T matrices for the super $U(1,1)$ WZW model. Application to surgery and 3-manifold invariants based on the Alexander Conway polynomial
hep-th/9203070;hep-th;0;36;;P.S.Howe,G.Papadopoulos;Finiteness and anomalies in (4,0) supersymmetric sigma models
hep-th/9203071;hep-th;0;0;;I.Antoniadis,E.Gava,K.S.Narain;Moduli Corrections to Gravitational Couplings from String loops
hep-th/9203072;hep-th;0;0;;F.D.Mazzitelli;Midisuperspace-Induced Corrections to the Wheeler De Witt Equation
hep-ph/9203220;hep-ph;0;19;;V.Barger,M.S.Berger,T.Han,M.Zralek;Test of the Dimopouos-Hall-Raby Ansatz for Fermion Mass Matrices
hep-ph/9203221;hep-ph,hep-lat;0;0;;O.F.Hernandez,B.R.Hill;Improved Heavy Quark Effective Theory Currents
hep-th/9203073;hep-th;0;27;;S.V.Pokrovsky;Quantum Group Analysis of the Bound States in the Strong Coupling Regime of the Modified Sine-Gordon Model
hep-ph/9203222;hep-ph;0;30;;G.P.Korchemsky,A.V.Radyushkin;Infrared Factorization, Wilson Lines and the Heavy Quark Limit
hep-th/9203074;hep-th;0;0;;A.Parkes;A cubic action for self-dual Yang-Mills
hep-th/9203075;hep-th;0;7;;E.Abdalla,M.Forger;Current Algebra of WZNW Models at and away from Criticality
hep-ph/9203223;hep-ph;0;115;;Z.Kunszt,F.Zwirner;Testing the Higgs Sector of the Minimal Supersymmetric Standard Model at Large Hadron Colliders
hep-th/9203076;hep-th;0;0;;T.J.Hollowood;Quantizing SL(N) Solitons and the Hecke Alegbra
hep-ph/9203224;hep-ph;0;0;;T.G.Rizzo;Phenomenology of R-Parity Breaking in E6 Models
hep-th/9203077;hep-th;0;15;;T.Tjin;Finite W-algebras
hep-th/9203078;hep-th;0;0;;S.J.Gates Jr,H.Nishino,S.V.Ketov;Extended Supersymmetry and Self-Duality in 2+2 Dimensions
hep-th/9203079;hep-th;0;0;;A.Ashtekar,C.Rovelli,L.Smolin;Weaving a classical geometry with quantum threads
hep-th/9203080;hep-th;0;0;;H.Nishino,S.J.Gates Jr,S.V.Ketov;Supersymmetric Self-Dual Yang-Mills and Supergravity as Background of Green-Schwarz Superstring
hep-th/9203081;hep-th;0;36;;S.V.Ketov,S.J.Gates,Jr.,H.Nishino;Majorana-Weyl Spinors and Self-Duality Gauge Fields in 2+2 Dimensions
hep-th/9203082;hep-th;0;0;;D.Kabat,M.Ortiz;Eikonal Quantum Gravity and Planckian Scattering
hep-th/9203083;hep-th;0;0;;J.H.Horne,G.T.Horowitz;Rotating Dilaton Black Holes
hep-ph/9203225;hep-ph;0;26;;P.Cho;Chiral perturbation theory for hadrons containing a heavy quark: the sequel
hep-ph/9203226;hep-ph;0;13;;M.Kenmoku,E.Kitajima,Y.Okamoto,K.Shigemoto;Rotation Curves of Spiral Galaxies and Large Scale Structure of Universe under Generalized Einstein Action
hep-th/9203084;hep-th;0;0;;A.Font;Periods and Duality Symmetries in Calabi-Yau Compactifications
hep-th/9204001;hep-th;0;0;;A.Aurilia,E.Spallucci;Axionic Membranes
hep-ph/9204201;hep-ph;0;0;;L.E.Ibanez,G.G.Ross;Electroweak Breaking in Supersymmetric Models
hep-ph/9204202;hep-ph;0;45;;V.Barger,K.Cheung,B.A.Kniehl,R.J.N.Phillips;Intermediate and Heavy Higgs Boson Physics at a 0.5 TeV e^+ e^- Collider
hep-ph/9204203;hep-ph;0;35;;U.Baur,M.A.Doncheski;Probing the $WWγ$ Vertex in $e^±p→ν\gammaX $
hep-ph/9204204;hep-ph;0;0;;S.P.Martin;A Tumbling Top-Quark Condensate Model
hep-th/9204002;hep-th;0;0;;T.T.Burwick,A.H.Chamseddine;Classical and Quantum Considerations of Two-dimensional Gravity
hep-ph/9204205;hep-ph;0;23;;L.E.Ibanez,F.Quevedo;Supersymmetry Protects the Primordial Baryon Asymmetry
alg-geom/9204001;alg-geom,math.AG;0;8;;M.Coppens,T.Kato;Weierstrass Gap Sequence at Total Inflection Points of Nodal Plane Curves
hep-th/9204003;hep-th;0;0;;S.Dasmahapatra,R.Kedem,B.McCoy;Physics beyond quasi-particles: Spectrum and completeness of the 3 state superintegrable chiral Potts model
hep-th/9204004;hep-th;0;0;;D.Z.Freedman,G.Grignani,N.Rius,K.Johnson;Conformal Symmetry and Differential Regularization of the Three-Gluon Vertex
hep-ph/9204206;hep-ph;0;0;;B.Grinstein,P.F.Mende;Heavy Mesons in Two Dimensions
hep-th/9204005;hep-th;0;0;;W.Siegel;The N=4 string is the same as the N=2 string
hep-th/9204006;hep-th;0;29;;F.Quevedo;Noncompact Coset Spaces in String Theory
hep-ph/9204207;hep-ph;0;13;;B.Grinstein,E.Jenkins,A.V.Manohar,M.J.Savage,M.B.Wise;Chiral Perturbation Theory for $f_{D_S}/f_D$ and $B_{B_S}/B_B$
hep-th/9204007;hep-th;0;26;;H.Itoyama,B.Razzaghe-Ashrafi;Anomalous Transformation in Supersymmetric Yang-Mills Theory
hep-th/9204008;hep-th;0;0;;D.Cangemi;Self-Dual Chern-Simons Solitons with Non-Compact Groups
hep-th/9204009;hep-th;0;0;;G.Bonacina,M.Martellini,M.Rasetti;2+1 Dimensional Quantum Gravity as a Gaussian Fermionic System and the 3D-Ising Model
hep-th/9204010;hep-th;0;25;;T.Kashiwa,S.Nima,S.Sakoda;Berry's Phase and Euclidean Path Integral
hep-th/9204011;hep-th;3;14;hep-th/9108026,hep-th/9109026,hep-th/9110004;S.K.Kar,A.Kumar;Target Space Structure of a Chiral Gauged Wess-Zumino-Witten Model
hep-ph/9204208;hep-ph;0;0;;A.V.Manohar;An Introduction to Spin Dependent Deep Inelastic Scattering
hep-ph/9204209;hep-ph;0;27;;B.Machet;4-dimensional spontaneously broken U(1)L gauge theories with a composite Wess-Zumino field
hep-ph/9204210;hep-ph;0;0;;A.Rebhan;Comment on ``High Temperature Fermion Propagator -- Resummation and Gauge Dependence of the Damping Rate''
hep-th/9204012;hep-th;2;72;hep-th/9109053,hep-th/9205068;B.de Carlos,J.A.Casas,C.Muñoz;Supersymmetry Breaking and Determination of the Unification Gauge Coupling Constant in String Theories
hep-ph/9204211;hep-ph;0;38;;J.Bagger,S.Dawson,G.Valencia;Effective Field Theory of Anomalous Gauge-Boson Couplings at High-Energy pp Colliders
hep-th/9204013;hep-th;0;23;;J.A.Minahan;Matrix Models and One Dimensional Open String Theory (Revised)
hep-th/9204014;hep-th;0;0;;C.G.Torre;Is General Relativity an 'Already Parametrized' Field Theory?
hep-th/9204015;hep-th;0;0;;T.T.Burwick,A.H.Chamseddine,K.Meissner;Matter Coupling and Spontaneous Symmetry Breaking in Topological Gravity
hep-th/9204016;hep-th;0;28;;E.Ivanov,S.Krivonos,A.Pichugin;Nonlinear realizations of $W_3$ symmetry
hep-ph/9204212;hep-ph;0;38;;J.Ellis,Y.Frishman,A.Hanany,M.Karliner;Quark solitons as constituents of hadrons
hep-ph/9204213;hep-ph;1;51;hep-th/9109049;J.A.Casas,J.García--Bellido,M.Quiros;Scalar--Tensor Theories of Gravity with \PHI Dependent Masses
hep-ph/9204214;hep-ph;0;26;;R.S.Chivukula,S.B.Selipsky,E.H.Simmons;Non-Oblique Effects in the Z b b_bar Vertex from ETC Dynamics
hep-th/9204017;hep-th;0;14;;S.Jain,S.D.Mathur;World-Sheet Geometry and Baby Universes in 2-D Quantum Gravity
hep-th/9204018;hep-th;0;0;;E.Brezin,S.Hikami;A naive matrix-model approach to two-dimensional quantum gravity coupled to matter of arbitrary central charge
hep-th/9204019;hep-th;0;15;;L.Bonora,C.S.Xiong;An alternative approach to KP hierarchy in matrix models
hep-th/9204020;hep-th;0;17;;D.Gepner,A.Schwimmer;Symplectic fusion rings and their metric
hep-ph/9204215;hep-ph;0;9;;G.F.Giudice;A new ansatz for quark and lepton mass matrices
hep-lat/9204001;hep-lat;1;17;hep-lat/9202004;B.A.Berg,T.Celik;A New Approach to Spin Glass Simulations
hep-th/9204021;hep-th;0;18;;C.Coriano';Electrodynamics in the presence of an axion
hep-th/9204022;hep-th;0;0;;N.Manojlovic,A.Mikovic;Ashtekar Formulation of 2+1 Gravity on a Torus
hep-ph/9204216;hep-ph;0;21;;R.R.Parwani;Resummation in a Hot Scalar Field Theory
hep-th/9204023;hep-th;0;22;;E.Ivanov,S.Krivonos;Superfield Realizations of $N=2$ Super-$W_3$
hep-th/9204024;hep-th;0;0;;J.Panvel;Higher Order Conformal Invariance of String Backgrounds Obtained by O(d,d) Transformations
cond-mat/9204001;cond-mat;0;35;;S.Sachdev,J.Ye;Universal quantum critical dynamics of two-dimensional antiferromagnets
cond-mat/9204002;cond-mat;0;0;;A.Balatsky;Spin Singlet Quantum Hall Effect and Nonabelian Landau-Ginzburg Theory
cond-mat/9204003;cond-mat;0;0;;A.Balatsky,E.Abrahams;A novel class of singlet superconductors
hep-th/9204025;hep-th;0;10;;R.Gregory,J.Harvey;Quantum Fermion Hair
hep-th/9204026;hep-th;0;0;;O.Lechtenfeld,C.Nappi;Dilaton Gravity and No-Hair Theorem in Two Dimensions
hep-th/9204027;hep-th;0;13;;M.Li;Gauge Symmetries and Amplitudes in N=2 Strings
hep-th/9204028;hep-th;1;35;hep-th/9111021;A.Dhar,G.Mandal,S.R.Wadia;Classical Fermi Fluid and Geometric Action for $c=1$
hep-th/9204029;hep-th;0;0;;V.Husain;2+1 Gravity without dynamics
hep-ph/9204217;hep-ph;0;0;;J.Bijnens,F.Hoogeveen;Two--Body Decays of $B_s$ Mesons
hep-ph/9204218;hep-ph;0;0;;S.Aoki;On the Renormalization of the S Parameter
hep-th/9204030;hep-th;1;13;hep-th/9205068;I.Antoniadis,E.Gava,K.S.Narain;Moduli Corrections to Gauge and Gravitational Couplings in four dimensional Superstrings
hep-lat/9204002;hep-lat;0;29;;C.F.Baillie,D.A.Johnston;A Numerical Test of KPZ Scaling: Potts Models Coupled to Two-Dimensional Quantum Gravity
hep-th/9204031;hep-th;0;10;;M.Cvetic,S.Griffies;Gravitational Effects in Supersymmetric Domain Wall Backgrounds
hep-lat/9204003;hep-lat;0;37;;C.F.Baillie,D.A.Johnston;Multiple Potts Models Coupled to Two-Dimensional Quantum Gravity
cond-mat/9204004;cond-mat;0;0;;S.Dasmahapatra,R.Kedem,B.M.McCoy;Physics beyond quasi-particles: Spectrum and completeness of the 3 state superintegrable chiral Potts model
astro-ph/9204001;astro-ph;0;0;;R.Narayan,B.Paczyński,T.Piran;Gamma-Ray Bursts as the Death Throes of Massive Binary Stars
hep-ph/9204219;hep-ph;0;13;;M.Luke,A.V.Manohar,M.J.Savage;A QCD Calculation of the Interaction of Quarkonium with Nuclei
hep-th/9204032;hep-th;0;6;;A.Carlini,F.Fucito,M.Martellini;On the Stability of a Stringy Black Hole
hep-ph/9204220;hep-ph;0;20;;R.S.Chivukula,M.Golden,M.V.Ramana;Colored Pseudo-Goldstone Bosons and Gauge Boson Pairs
hep-th/9204033;hep-th;0;21;;N.Weiss;Bosonic Chern-Simons Field Theory of Anyon Superconductivity
hep-lat/9204004;hep-lat;0;28;;M.E.Agishtein,A.A.Migdal;Critical Behavior of Dynamically Triangulated Quantum Gravity in Four Dimensions
cond-mat/9204005;cond-mat;0;13;;M.I.Dobroliubov,I.I.Kogan,G.W.Semenoff;Investigations of Pairing in Anyon Systems
hep-ph/9204221;hep-ph;0;7;;D.Ng;QCD renormalization for the top-quark mass in a mass geometrical mean hierarchy
hep-th/9204034;hep-th;0;0;;A.J.van Tonder;A Continuum Description of Super-Calogero Models
hep-ph/9204222;hep-ph;0;0;;A.Donnachie,P.V.Landshoff;Unusual high-pT jet events at HERA
cond-mat/9204006;cond-mat;0;0;;D.M.Gaitonde,D.P.Jatkar,S.Rao;Chirality Ordering of Chiral Spin Liquids
cond-mat/9204007;cond-mat;0;60;;R.D.Kamien,P.L.Doussal,D.R.Nelson;Theory of Directed Polymers
hep-th/9204035;hep-th;0;0;;A.Ceresole,R.D'Auria,S.Ferrara,W.Lerche,J.Louis;Picard-Fuchs Equations and Special Geometry
hep-th/9204036;hep-th;0;0;;P.Roche;On the construction of integrable dilute ADE models
hep-th/9204037;hep-th;0;27;;S.Stieberger,D.Jungnickel,J.Lauer,M.Spalinski;Yukawa Couplings for Bosonic $Z_N$ Orbifolds: Their Moduli and Twisted Sector Dependence
hep-th/9204038;hep-th;0;0;;H.Lu,C.N.Pope;On Realisations of W Algebras
hep-th/9204039;hep-th;0;0;;A.Aurilia,A.Smailagic,E.Spallucci;Membrane Pregeometry and the Vanishing of the Cosmological Constant
hep-th/9204040;hep-th;0;0;;S.Ferrara,P.Frè,P.Soriani;On the Moduli Space of the $T^6/Z_3$ Orbifold and Its Modular Group
hep-th/9204041;hep-th;0;0;;P.Fre',L.Girardello,A.Lerda,P.Soriani;Topological First-Order Systems with Landau-Ginzburg Interactions
hep-th/9204042;hep-th;0;13;;E.Raiten;Asymptotic Behavior of 2-d Black Holes
hep-th/9204043;hep-th;1;20;hep-th/9111001;T.Nakatsu,Y.Sugawara;BRST-Fixed Points and Topological Conformal Symmetry
hep-th/9204044;hep-th;0;38;;N.Maggiore,S.P.Sorella;Perturbation Theory for Antisymmetric Tensor Fields in Four Dimensions
hep-th/9204045;hep-th;0;16;;A.Blasi,N.Maggiore,S.P.Sorella;Non-Renormalization Properties of the Chern-Simons Action Coupled to Matter
hep-th/9204046;hep-th;0;0;;A.Sen;Rotating Charged Black Hole Solution in Heterotic String Theory
hep-th/9204047;hep-th;0;0;;G.Semenoff;Strong Coupling Qed Breaks Chiral Symmetry
hep-th/9204048;hep-th;0;0;;D.Eliezer,G.Semenoff;Intersections forms and the geometry of lattice Chern-Simons theory
hep-th/9204049;hep-th;1;23;hep-th/9109032;M.Bershadsky,D.Kutasov;Scattering of Open and Closed Strings in 1+1 Dimensions
hep-th/9204050;hep-th;0;68;;T.Nakatsu,Y.Sugawara;Topological Gauged WZW Models and 2D Gravity
hep-th/9204051;hep-th;0;22;;S.Forste;String amplitudes in arbitrary dimensions
hep-lat/9204005;hep-lat;0;0;;M.Creutz;Microcanonical cluster algorithms
hep-th/9204052;hep-th;0;0;;I.R.Klebanov,A.Pasquinucci;Correlation functions from two-dimensional string Ward identities
hep-lat/9204006;hep-lat;0;0;;O.F.Hernandez,B.R.Hill;Point-Split Lattice Operators for B Decays
hep-ph/9204223;hep-ph;0;19;;S.D.H.Hsu;On tunneling at finite energies and temperatures
hep-th/9204053;hep-th;2;32;hep-th/9109032,hep-th/9201005;S.Kachru;Extra States and Symmetries in D<2 Closed String Theory
hep-th/9204054;hep-th;0;0;;F.Bonechi,E.Celeghini,R.Giachetti,E.Sorace,M.Tarlini;Heisenberg XXZ Model and Quantum Galilei Group
hep-th/9204055;hep-th;0;0;;C.G.Torre;Covariant Phase Space Formulation of Parametrized Field Theories
hep-th/9204056;hep-th;0;0;;G.Dunne,R.Jackiw;Chern-Simons Solitons, Toda Theories and the Chiral Model
hep-th/9204057;hep-th;0;0;;G.Dunne,R.Jackiw;"Peireles Substitution" and Chern-Simons Quantum Mechanics
hep-lat/9204007;hep-lat;0;0;;C.Bernard,M.Golterman;Chiral Perturbation Theory for the Quenched Approximation of QCD
hep-th/9204058;hep-th;0;31;;J.-S.Park;Algebraic Structures of Topological Yang-Mills Theory
hep-th/9204059;hep-th;0;12;;H.Aoyama,A.Tamura;Path-Integral for Quantum Tunneling
hep-th/9204060;hep-th;1;69;hep-th/9112047;A.Klemm,R.Schimmrigk;Landau-Ginzburg String Vacua
hep-th/9204061;hep-th;0;0;;J.P.Rodrigues,A.J.van Tonder;Marinari-Parisi and Supersymmetric Collective Field Theory
hep-th/9204062;hep-th;0;18;;M.Visser;Hawking radiation: a particle physics perspective
hep-th/9204063;hep-th;0;44;;A.M.Semikhatov;Solving Virasoro Constraints on Integrable Hierarchies via the Kontsevich-Miwa Transform
hep-lat/9204008;hep-lat;0;22;;K.M.Bitar,T.A.DeGrand,R.G.Edwards,S.Gottlieb,U.M.Heller,A.D.Kennedy,J.B.Kogut,A.Krasnitz,W.Liu,M.C.Ogilvie,R.L.Renken,P.Rossi,D.K.Sinclair,R.L.Sugar,D.Toussaint,K.C.Wang;Hadron Spectrum in QCD with Valence Wilson Fermions and Dynamical Staggered Fermions at $6/g^2=5.6
hep-lat/9204009;hep-lat;0;0;;D.Espriu,J.Matias;Spectrum of Relativistic Fermions in a 2d Doped Lattice
hep-ph/9204224;hep-ph;0;12;;M.Bander,H.R.Rubinstein;Proton $β% decay in large magnetic fields
cond-mat/9204008;cond-mat;0;0;;M.E.Flatte;Image of the Energy Gap Anisotropy in the Vibrational Spectum of a High Temperature Superconductor
hep-th/9204064;hep-th;0;0;;B.Davies,O.Foda,M.Jimbo,T.Miwa,A.Nakayashiki;Diagonalization of the XXZ Hamiltonian by Vertex Operators
hep-th/9204065;hep-th;0;30;;J.Gomis,J.París;Field-Antifield formalism for Anomalous Gauge Theories
hep-th/9204066;hep-th;0;0;;C.S.Aulakh;Syncyclons or Solitonic Signals from Extra Dimensions
hep-th/9204067;hep-th;0;36;;K.Aoki,E.D'Hoker;W--Gravity and Generalized Lax Equations for (super) Toda Theory
hep-lat/9204010;hep-lat;0;14;;W.Beirl,E.Gerstenmayer,H.Markum;Influence of the Measure on Simplicial Quantum Gravity in Four Dimensions
cond-mat/9204009;cond-mat;0;3;;J.P.Sethna;Order Parameters, Broken Symmetry, and Topology
cond-mat/9204010;cond-mat;0;7;;J.P.Sethna,M.Huang;Meissner Effect and Constraints
hep-ph/9204225;hep-ph;0;0;;H.Arason,D.J.Castano,E.J.Piard,P.Ramond;Mass and mixing angle patterns in the Standard Model and its Minimal Supersymmetric Extension
math/9204201;math.CV;0;2;;A.Russakovskii;Zero sets of some classes of entire functions
math/9204202;math.LO;0;0;;W.J.Mitchell;On the Singular Cardinal Hypothesis
math/9204203;math.LO;0;0;;R.Laver;A division Algorithm for the Free Left Distributive Algebra
math/9204204;math.LO;0;0;;R.Laver;On the Algebra of Elementary Embeddings of a Rank into Inself
math/9204205;math.LO;0;0;;S.Shelah,J.Steprāns;Maximal Chains in ^ωωand Ultrapowers of the Integers
math/9204206;math.LO;0;0;;T.Jech;A short proof of the irreflexivity conjecture
math/9204207;math.LO;0;0;;T.Jech;On Gödel's second incompleteness theorem
math/9204208;math.LO;0;5;;D.M.Larue;On Braid Words and Irreflexivity
math/9204209;math.LO;0;0;;W.Mitchell;Embeddings of Iteration Trees
hep-ph/9204226;hep-ph;0;40;;M.A.Doncheski,J.L.Hewett;Signals for Virtual Leptoquark Exchange at HERA
cond-mat/9204011;cond-mat;0;0;;F.Colomo,A.G.Izergin,V.Korepin;Fredholm Determinant Representation for Correlation Functions in XXO Heisenberg Chain
hep-lat/9204011;hep-lat;0;0;;D.Daniel,R.Gupta,G.Kilcup,A.Patel,S.Sharpe;Phenomenology with Wilson fermions using smeared sources
hep-lat/9204012;hep-lat;0;8;;A.Patel;Scalar and axial matrix elements of the nucleon: sea quark content
math/9204210;math.LO;0;5;;A.Dow,J.Steprāns,W.S.Watson;Reaping Numbers of Boolean Algebras
math/9204211;math.FA;0;0;;J.Taskinen;Structure of local Banach spaces of locally convex spaces
math/9204212;math.FA;0;16;;M.Meyer,S.Reisner,M.Schmuckenschlager;The volume of the intersection of a convex body with its translates
math/9204213;math.FA;0;0;;E.Odell,T.Schlumprecht;The Distorion Problem
hep-ph/9204227;hep-ph;0;0;;S.Ben-Menahem,A.Cooper;Superconductivity Solves the Monopole Problem for Alice Strings
hep-ph/9204228;hep-ph;0;14;;P.Arnold;Phase Transition Temperatures at Next-to-Leading Order
hep-ph/9204229;hep-ph;1;43;hep-ph/9908362;A.F.Falk,M.Neubert,M.Luke;The Residual Mass Term in the Heavy Quark Effective Theory
hep-ph/9204230;hep-ph;0;8;;R.Basu,D.Choudhury;Confinement in a Chromoelectric Vacuum
hep-th/9204068;hep-th,nlin.SI,solv-int;0;0;;O.Foda,T.Miwa;Corner Transfer Matrices and Quantum Affine Algebras
hep-th/9204069;hep-th,gr-qc;0;13;;P.Peldan;Ashtekar's Variables for Arbitrary Gauge Group
hep-th/9204070;hep-th;0;0;;A.Smailagic,E.Spallucci;Gravitational and Schwinger model anomalies: how far can the analogy go?
hep-th/9204071;hep-th;2;20;hep-th/9109039,hep-th/9201020;F.Delduc,E.Ivanov,E.Sokatchev;Twistor-like superstrings with D = 3, 4, 6 target-superspace and N = (1,0), (2,0), (4,0) world-sheet supersymmetry
hep-th/9204072;hep-th;0;27;;S.B.Giddings,W.M.Nelson;Quantum Emission from Two-Dimensional Black Holes
hep-th/9204073;hep-th;0;8;;H.Nohara;Dynamical Topological Phase Transition in Massless Thirring Model
hep-ph/9204231;hep-ph;0;0;;M.Jacob,P.V.Landshoff;Reaction rate in a heat bath
cond-mat/9204012;cond-mat;0;0;;J.P.Sethna,S.Kartha,T.Cast'an,J.A.Krumhansl;Tweed in Martensites: A Potential New Spin Glass
hep-lat/9204013;hep-lat;0;0;;K.Kajantie,L.Karkkainen,K.Rummukainen;The Free Energy of Spherical Bubbles in Lattice SU(3) Gauge Theory
hep-th/9204074;hep-th;0;0;;D.B.Fairlie,J.Govaerts;Euler Hierarchies and Universal Equations
hep-th/9204075;hep-th;0;0;;G.Ferretti,S.G.Rajeev,Z.Yang;The Effective Lagrangian of Three Dimensional Quantum Chromodynamics
hep-th/9204076;hep-th;0;0;;G.Ferretti,S.G.Rajeev,Z.Yang;Baryons as Solitons in Three Dimensional Quantum Chromodynamics
hep-th/9204077;hep-th;0;8;;A.Kent,G.Watts;Signature Characters for A_2 and B_2
hep-ph/9204232;hep-ph;0;17;;A.Kusenko;New Tools for Analyzing Quark Mixing
hep-ph/9204233;hep-ph;0;16;;D.Bhowmick,A.K.Ray,S.Raychaudhuri,S.U.Sankar;CP-violating Phenomena in an $ SU(2)_L ×SU(2)_R ×U(1)_{B-L} ×SU(3)_H^{VL}$ Horizontal Symmetric Model
hep-th/9204078;hep-th;0;23;;K.Behrndt;Non-Critical Strings in Robertson-Walker Space Time
hep-th/9204079;hep-th;2;33;hep-th/9109048,hep-th/9109049;J.Garcia-Bellido,M.Quiros;String Effective Actions and Cosmological Stability of Scalar Potentials
hep-th/9204080;hep-th;0;18;;C.Coriano',R.R.Parwani,H.Yamagishi,I.Zahed;Scattering in Soliton Models and the Bosonic Exchange description
hep-th/9204081;hep-th;0;8;;A.Kent;Signature Characters for the Virasoro Algebra
cond-mat/9204013;cond-mat;0;0;;J.Hodgdon,J.P.Sethna;Beyond the ``principle of local symmetry'': derivation of a general crack propagation law
math/9204214;math.FA;0;4;;N.J.Nielsen;A Note on Unconditional Structures in Weak Hilbert Spaces
hep-th/9204082;hep-th;0;24;;B.Eynard,J.Zinn-Justin;The $O(n)$ model on a random surface: critical points and large order behaviour
hep-th/9204083;hep-th;0;48;;E.Witten;Two Dimensional Gauge Theories Revisited
hep-th/9204084;hep-th;1;19;hep-th/9109032;D.A.Lowe;Unitarity Relations in c=1 Liouville Theory
hep-th/9204085;hep-th;0;27;;B.Gato-Rivera,A.M.Semikhatov;Minimal Models from W-Constrained Hierarchies via the Kontsevich-Miwa Transform
astro-ph/9204002;astro-ph;0;35;;L.Krauss,M.White;Gravitational Lensing and the Variability of G
hep-lat/9204014;hep-lat;0;91;;A.Brandt;Multigrid Methods in Lattice Field Computations
hep-th/9204086;hep-th;0;22;;Y.Frishman,J.Lukierski,W.J.Zakrzewski;Quantum Group $σ$ Models
hep-th/9204087;hep-th,math.GT;0;0;;D.H.Gottlieb;Vector Fields and the Unity of Mathematics and Physics
math/9204215;math.FA;0;0;;D.E.Alspach;A l_1-predual which is not isometric to a quotient of C(alpha)
math/9204216;math.FA;0;8;;P.F.X.Müller;Jean Bourgain's analytic partition of unity via holomorphic martingales
math/9204217;math.NT;0;0;;J.B.Conrey,A.Ghosh;On the Selberg class of Dirichlet series: small weights
math/9204218;math.LO;0;0;;T.Jech,S.Shelah;Full reflection of stationary sets at regular cardinals
math/9204219;math.LO,math.RA;0;10;;P.C.Eklof,A.H.Mekler,S.Shelah;Uniformization and the diversity of Whitehead groups
math/9204220;math.GR,math.RA;0;0;;P.W.Michor;Knit products of graded Lie algebras and groups
math/9204221;math.DG;0;2;;M.Mauhart,P.W.Michor;Commutators of flows and fields
math/9204222;math.RT;0;0;;P.W.Michor;All unitary representations admit moment mappings
math/9204223;math.DG;0;0;;O.Gil-Medrano,P.W.Michor;Geodesics on spaces of almost hermitian structures
math/9204224;math.CV,math.PR;0;0;;S.Albeverio,Z.-M.Ma;A general correspondence between Dirichlet forms and right processes
math/9204225;math.AG;0;0;;D.Arapura;Higgs line bundles, Green-Lazarsfeld sets,and maps of Kähler manifolds to curves
math/9204226;math.DG,math.AG;0;0;;C.P.Boyer,J.Hurtubise,B.M.Mann,R.J.Milgram;The Atiyah-Jones Conjecture
math/9204227;math.RT;0;0;;R.Brylinski,B.Kostant;Nilpotent orbits, normality, and Hamiltonian group actions
math/9204228;math.OA;0;0;;L.J.Bunce,J.D.M.Wright;The Mackey-Gleason Problem
math/9204229;math.RT,math.NT;0;0;;M.Burger,J.-S.Li,P.Sarnak;Ramanujan duals and automorphic spectrum
math/9204230;math.AG;0;0;;E.M.Friedlander,H.B.Lawson Jr;A theory of algebraic cocycles
math/9204231;math.AT,math.GT;0;0;;I.M.Gelfand,R.D.MacPherson;A combinatorial formula for the Pontrjagin classes
math/9204232;math.CV;0;0;;H.Hauser,G.Muller;Analytic varieties versus integral varieties of Lie algebras of vector fields
math/9204233;math.MG,math.CO;0;0;;G.Kalai,D.J.Kleitman;A quasi-polynomial bound for the diameter of graphs of polyhedra
math/9204234;math.NT;0;0;;H.W.Lenstra Jr;Algorithms in algebraic number theory
math/9204235;math.SP,math.RT;0;0;;P.Levy-Bruhl,A.Mohamed,J.Nourrigat;Spectral Theory and Representations of Nilpotent Groups
math/9204236;math.CA;0;0;;S.C.Milne,G.M.Lilly;The $\bal $ and $\bcl $ Bailey Transform and Lemma
math/9204237;math.CV,math.DG;0;0;;S.Nag;A period mapping in universal Teichmüller space
math/9204238;math.CV,math.FA;1;20;math-ph/0210005;K.Seip;Density theorems for sampling and interpolation in the Bargmann-Fock space
math/9204239;math.AP;0;7;;W.Xie;A sharp pointwise bound for functions with $L^2$-Laplacians on arbitrary domains and its applications
math/9204240;math.DS;0;14;;Y.Jiang;Dynamics of certain non-conformal semigroups
math/9204241;math.DS;0;0;;F.Przytycki,F.Tangerman;Cantor sets in the line: scaling function and the smoothness of the shift map
hep-ph/9204234;hep-ph;0;0;;R.N.Mohapatra,M.K.Parida;Threshold Effects in SO(10) Grandunified Models and Solar Neutrino Puzzle
hep-th/9204088;hep-th;0;20;;H.Dorn,H.-J.Otto;Analysis of All Dimensionful Parameters Relevant in Gravitational Dressing of Conformal Theories
hep-ph/9204235;hep-ph;0;23;;O.Tornkvist;Ginzburg-Landau Theory of the Electroweak Phase Transition and Analytical Results
cond-mat/9204014;cond-mat;0;9;;U.-J.Wiese,H.-P.Ying;Blockspin Cluster Algorithms for Quantum Spin Systems
hep-lat/9204015;hep-lat;0;9;;U.-J.Wiese,H.-P.Ying;Blockspin Cluster Algorithms for Quantum Spin Systems
hep-th/9204089;hep-th;0;26;;A.T.Filippov,A.P.Isaev,A.B.Kurdikov;Paragrassmann Analysis and Quantum Groups
hep-th/9204090;hep-th;0;25;;G.W.Gibbons,M.J.Perry;The Physics of 2-d Stringy Spacetimes
cond-mat/9204015;cond-mat;0;0;;J.D.Shore,M.Holzer,J.P.Sethna;Logarithmically slow domain growth in nonrandomly frustrated systems: Ising models with competing interactions
hep-th/9204091;hep-th;0;28;;W.T.IV;Virasoro Representations on (Diff S1)/S1 Coadjoint Orbits
hep-th/9204092;hep-th;0;0;;L.Dickey;Additional symmetries of KP, Grassmannian, and the string equation
hep-th/9204093;hep-th;0;0;;C.N.Pope;Review of W Strings
cond-mat/9204016;cond-mat;0;0;;J.D.Shore,J.P.Sethna,M.Holzer,V.Elser;Logarithmically slow domain growth in nonrandomly frustrated systems--- A summary of the major results
cond-mat/9204017;cond-mat;0;9;;Z.N.C.Ha,F.D.M.Haldane;On Models with Inverse-Square Exchange
hep-th/9204094;hep-th;1;41;hep-th/9111014;P.Fendley,H.Saleur;N=2 Supersymmetry, Painleve III and Exact Scaling Functions in 2D Polymers
hep-th/9204095;hep-th;0;49;;O.Aharony,O.Ganor,N.S.J.Sonnenschein,S.Yankielowicz;Physical States in G/G Models and 2d Gravity
hep-th/9204096;hep-th;5;77;hep-th/9109027,hep-th/9109032,hep-th/9111001,hep-th/9111031,hep-th/9112062;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;On the W-hair of String Black Holes and the Singularity Problem
hep-ph/9204236;hep-ph;0;32;;V.Koch,E.V.Shuryak,G.E.Brown,A.D.Jackson;The Propagation of Quarks in the Spatial Direction in Hot QCD
astro-ph/9204003;astro-ph;0;0;;J.I.Katz;The Ptolemaic Gamma-Ray Burst Universe
hep-ph/9204237;hep-ph;0;23;;P.Cho,B.Grinstein;Heavy Hadron Form Factor Relations for $m_c\ne ∞$ and $\bas (m_c)\ne 0$
hep-th/9204097;hep-th;0;16;;A.Kent;Singular Vectors of the Virasoro Algebra
hep-th/9204098;hep-th;0;14;;A.Kent;Projections of Virasoro Singular Vectors
hep-th/9204099;hep-th;5;19;hep-th/9505037,gr-qc/9506079,gr-qc/9705016,hep-th/9912259,gr-qc/0101029;M.Bañados,C.Teitelboim,J.Zanelli;The Black Hole in Three Dimensional Space Time
hep-th/9204100;hep-th;0;58;;Z.Maassarani,D.Nemeschansky,N.P.Warner;Lattice Analogues of $N=2$ Superconformal Models via Quantum Group Truncation
hep-ph/9204238;hep-ph;0;14;;E.Jenkins,M.Luke,A.V.Manohar,M.J.Savage;Semileptonic $B_c$ Decay and Heavy Quark Spin Symmetry
hep-lat/9204016;hep-lat;0;15;;M.Grabenstein,K.Pinn;Acceptance Rates in Multigrid Monte Carlo
hep-lat/9204017;hep-lat,hep-ph;1;35;hep-th/9109040;T.Banks,A.Dabholkar;Decoupling a Fermion Whose Mass Comes from a Yukawa Coupling: Nonperturbative Considerations
cond-mat/9204018;cond-mat;0;25;;T.C.Hsu;Absence of Dipole Transitions in Vortices of Type II Superconductors
hep-th/9204101;hep-th;0;0;;D.Cangemi,C.Lee;Self-Dual Chern-Simons Solitons in (2+1)-Dimensional Einstein Gravity
hep-ph/9204239;hep-ph;0;19;;K.Haglin,C.Gale,V.Emel'yanov;Virtual bremsstrahlung from pions and quarks in thermalized hadronic matter
astro-ph/9204004;astro-ph;0;104;;B.P.Schmidt,R.P.Kirshner,R.G.Eastman;Expanding Photospheres of Type II Supernovae and the Extragalactic Distance Scale
astro-ph/9204005;astro-ph;0;0;;B.J.Carrigan,J.I.Katz;Radiation Transfer in Gamma-Ray Bursts
astro-ph/9204006;astro-ph;0;0;;D.J.Johnson,M.W.Friedlander,J.I.Katz;Nova Dust Nucleation: Kinetics and Photodissociation
hep-th/9204102;hep-th;3;62;hep-th/9108005,hep-th/9111014,hep-th/9111016;S.Cecotti,P.Fendley,K.Intriligator,C.Vafa;A New Supersymmetric Index
hep-th/9204103;hep-th;0;0;;D.Kabat;Validity of the Eikonal Approximation
math/9205201;math.LO;0;3;;G.Hjorth;The Cardinality of the second uniform indiscernible
hep-lat/9205001;hep-lat;0;15;;U.Wolff;Scaling topological charge in the CP^3 spin model
hep-lat/9205002;hep-lat;0;25;;K.Funakubo,T.Kashiwa;Chiral Invariance and Species Doublers in Generic Fermion Models on the Lattice
cond-mat/9205001;cond-mat;0;20;;A.-P.Jauho,H.Smith;Coulomb drag between two-dimensional electron systems
hep-th/9205001;hep-th;0;7;;V.Jain,O.Ogievetsky;Classical Isomorphisms for Quantum Groups
hep-th/9205002;hep-th;0;0;;H.Awata,Y.Yamada;Fusion Rules for the q-deformed Vertex Operators of U_q(sl(2)^)
cond-mat/9205002;cond-mat;0;0;;L.Balents,M.Kardar;Roughening of Reconstructed Crystal Surfaces and the Hubbard Model
astro-ph/9205001;astro-ph;0;47;;V.Faraoni;Nonstationary Gravitational Lenses and the Fermat Principle
hep-lat/9205003;hep-lat;0;55;;H.Neuberger;Non--perturbative bounds on the Higgs mass in the minimal standard model
hep-th/9205003;hep-th;0;6;;O.Ogievetsky,B.Zumino;Reality in the Differential Calculus on q-euclidean Spaces
astro-ph/9205002;astro-ph;0;0;;T.Hanawa,R.Matsumoto,K.Shibata;Giant Molecular Cloud Formation through the Parker Instability in a Skewed Magnetic Field
hep-th/9205004;hep-th;0;0;;M.Kreuzer,H.Skarke;No Mirror Symmetry in Landau-Ginzburg Spectra!
alg-geom/9205001;alg-geom,math.AC,math.AG;0;0;;R.W.Berger;Report on the Torsion of the Differential Module of an algebraic Curve
hep-lat/9205004;hep-lat;0;67;;W.Bock,A.K.De,C.Frick,J.Jersák,T.Trappenberg;Spontaneous symmetry breaking on the lattice generated by Yukawa interaction
cond-mat/9205003;cond-mat;0;0;;S.Zhang,M.H.Kalos;Bilinear Quantum Monte Carlo: Expectations and Energy Differences
hep-th/9205005;hep-th;0;15;;G.Barnich,M.Henneaux;Comments on Unitarity in the Antifield Formalism
astro-ph/9205003;astro-ph;0;0;;J.I.Katz;Particle Acceleration in (by) Accretion Discs
hep-lat/9205005;hep-lat;0;105;;S.Caracciolo,R.G.Edwards,A.Pelissetto,A.D.Sokal;Wolff-Type Embedding Algorithms for General Nonlinear $σ$-Models
hep-th/9205006;hep-th,hep-lat;1;39;hep-th/9201042;J.Greensite;Stabilized Quantum Gravity: Stochastic Interpretation and Numerical Simulation
hep-ph/9205201;hep-ph;0;0;;H.König,K.A.Peterson;Production of the Lightest Supersymmetric Particle in Electron-Photon Collisions
hep-ph/9205202;hep-ph;0;119;;K.Choi,D.B.Kaplan,A.E.Nelson;Is CP a Gauge Symmetry?
alg-geom/9205002;alg-geom,math.AG;0;0;;E.Bifet;Cohomology, Symmetry, and Perfection
hep-ph/9205203;hep-ph;0;38;;R.Sundrum;A Realistic Technicolor Model from 150 TeV down
hep-ph/9205204;hep-ph;0;0;;M.A.Luty;Vacuum Alignment in "Composite Technicolor" Models
hep-th/9205007;hep-th,math.QA;0;35;;J.C.Baez;Quantum Gravity and the Algebra of Tangles
hep-ph/9205205;hep-ph;0;39;;M.J.Strassler;Field Theory Without Feynman Diagrams: One-Loop Effective Actions
cond-mat/9205004;cond-mat;0;0;;D.P.Clougherty,W.Kohn;Low Energy Behavior of Quantum Adsorption
hep-th/9205008;hep-th;0;26;;J.P.Gauntlett;Low-Energy Dynamics of Supersymmetric Solitons
hep-th/9205009;hep-th;0;38;;G.L.Cardoso,B.A.Ovrut;Coordinate and Kähler $σ$-Model Anomalies and Their Cancellation in String Effective Field Theories
cond-mat/9205005;cond-mat;0;12;;W.Chen,M.Dobroliubov,G.Semenoff;Z_N Phases in Hot Gauge Theories
hep-th/9205010;hep-th;0;48;;L.Alvarez-Gaume,J.L.F.Barbon;A Proposal for $D>1$ Strings?
funct-an/9205001;funct-an,math.FA;0;0;;A.Bressan,B.Piccoli;A Baire Category Approach to the Bang-Bang Property
hep-ph/9205206;hep-ph;0;0;;J.C.Romao,C.A.Santos,J.W.F.Valle;R parity can spontaneously break
hep-ph/9205207;hep-ph;0;60;;T.G.Rizzo;Contributions to the W-Boson Anomalous Moments in the Two-Higgs-Doublet Model at Collider Energies
cond-mat/9205006;cond-mat;0;0;;A.V.Balatsky;Quaternion Generalization of the Laughlin State and the Three Dimensional Fractional QHE
math/9205202;math.LO;0;0;;R.Dougherty;Critical points in an algebra of elementary embeddings
math/9205203;math.FA;0;0;;G.A.Willis;The Compact Approximation Property does not imply the Approximation Property
math/9205204;math.FA;0;0;;W.T.Gowers,B.Maurey;The unconditional basic sequence problem
hep-th/9205011;hep-th;0;14;;M.Dine,R.G.Leigh,D.A.MacIntire;Of CP and other Gauge Symmetries in String Theory
hep-th/9205012;hep-th;0;0;;B.de Wit,M.T.Grisaru,E.Rabinovici,H.Nicolai;Two-loop finiteness of D=2 supergravity
hep-th/9205013;hep-th;0;23;;G.M.T.Watts;A Note of W-algebra Realisations
math/9205205;math.FA;0;3;;D.H.Leung;On $c_0$-saturated Banach spaces
hep-lat/9205006;hep-lat,hep-ph;0;17;;G.T.Bodwin,E.Braaten,G.P.Lepage;Rigorous QCD Predictions for Decays of P-Wave Quarkonia
hep-th/9205014;hep-th;0;26;;G.P.Korchemsky;Matrix Model Perturbed by Higher Order Curvature Terms
hep-th/9205015;hep-th;0;0;;I.Antoniadis,P.O.Mazur,E.Mottola;Conformal Symmetry and Central Charges in 4 Dimensions
alg-geom/9205003;alg-geom,math.AG;0;0;;X.Wu;Chern classes and degenerations of hypersurfaces and their lines
hep-lat/9205007;hep-lat;0;13;;G.P.Lepage,L.Magnea,C.Nakhleh,U.Magnea,K.Hornbostel;Improved Nonrelativistic QCD for Heavy Quark Physics
hep-th/9205016;hep-th;0;0;;J.Maharana;Duality and $O(d,d)$ Symmetries in String Theory
hep-ph/9205208;hep-ph,astro-ph;0;0;;S.-J.Sin;Late time Cosmological Phase Transition and Galactic Halo as Bose-liquid
alg-geom/9205004;alg-geom,math.AG;0;0;;T.Fujita;Notes on Kodaira energies of polarized varieties
hep-ph/9205209;hep-ph;0;0;;F.Cuypers,G.J.van Oldenborgh,R.Rückl;Supersymmetric Signals in Electron-Photon Collision
astro-ph/9205004;astro-ph;0;55;;A.Cappi,S.Maurogordato;The Spatial Distribution of Nearby Galaxy Clusters in the Northern and Southern Galactic Hemispheres
hep-ph/9205210;hep-ph;0;28;;J.Bijnens,G.Ecker,A.Pich;The Chiral Anomaly in Non-Leptonic Weak Interactions
hep-ph/9205211;hep-ph;0;0;;M.McGuigan,C.B.Thorn;Quark-Antiquark Regge Trajectories in Large N_c QCD
hep-lat/9205008;hep-lat;0;35;;A.S.Kronfeld;Dynamics of Langevin Simulation
hep-ph/9205212;hep-ph;0;32;;L.M.Krauss,M.White;Grand Unification, Gravitational Waves, and the Cosmic Microwave Background Anisotropy
astro-ph/9205005;astro-ph;0;0;;R.Rangarajan,M.Srednicki;Chaotic Dark Matter
hep-ph/9205213;hep-ph;0;28;;L.S.Brown,L.G.Yaffe,C.Zhai;Large-order perturbation theory for the electromagnetic current-current correlation function
hep-th/9205017;hep-th;0;17;;C.Ting,C.H.Lai;c = 1 conformal field theory and the fractional quantum Hall effect
hep-ph/9205214;hep-ph;0;23;;C.Giunti,C.W.Kim,U.W.Lee;Oscillations of Pseudo-Dirac Neutrinos and the Solar Neutrino Problem
hep-th/9205018;hep-th;0;13;;M.Henneaux;Geometric Interpretation of the Quantum Master Equation in the BRST--anti-BRST Formalism
hep-th/9205019;hep-th;0;0;;C.S.Aulakh;Charged Topological Solitons in 4+1 Dimensional YMCS Theory
hep-th/9205020;hep-th;2;24;hep-th/9109032,hep-th/9201005;I.Ya.Aref'eva,A.P.Zubarev;Divergences of Discrete States Amplitudes and Effective Lagrangian in 2D String Theory
hep-lat/9205009;hep-lat;0;17;;C.F.Baillie;Ising Model Coupled to Three-Dimensional Quantum Gravity
funct-an/9205002;funct-an,math.FA;0;0;;G.D.Maso,A.Defranceschi,E.Vitali;Integral representation for a class of $C^1$-convex functionals
math/9205206;math.FA;0;0;;N.J.Kalton,S.J.Montgomery-Smith;Set-functions and factorization
hep-th/9205021;hep-th;0;14;;B.Harms,Y.Leblanc;Statistical Mechanics of Black Holes
hep-th/9205022;hep-th;0;35;;S.Carlip;Entropy vs. Action in the (2+1)-Dimensional Hartle-Hawking Wave Function
hep-ph/9205215;hep-ph,hep-th;0;31;;B.Machet;4-dimensional spontaneously broken U(1)L gauge theories without asymptotic quarks and Higgs boson
hep-ph/9205216;hep-ph;1;48;hep-th/9109049;J.Garcia-Bellido;Dark Matter with Variable Masses
alg-geom/9205005;alg-geom,math.AG;0;0;;P.Aluffi,C.Faber;Linear orbits of d-tuples of points in P^1
hep-th/9205023;hep-th;0;0;;R.-R.Hsu,G.Huang,W.-F.Lin,C.-R.Lee;Stability Analysis of a Stringy Black Hole
hep-th/9205024;hep-th;1;24;hep-th/9201032;M.J.Martins;Renormalization group trajectories from resonance factorized S-matrices
hep-th/9205025;hep-th;0;42;;M.Fabbrichesi,R.Iengo,K.Roland;The Gravitational Field of String Matter
hep-th/9205026;hep-th;0;0;;J.D.Cohn,V.Periwal;Lorentz invariance of effective strings
hep-th/9205027;hep-th;0;46;;R.Kallosh,A.Linde,T.Ortín,A.Peet,A.V.Proeyen;Supersymmetry as a Cosmic Censor
hep-th/9205028;hep-th;0;0;;A.Strominger;Fadeev-Popov Ghosts and 1+1 Dimensional Black Hole Evaporation
hep-th/9205029;hep-th,hep-ph;2;26;hep-th/9109053,hep-th/9205068;M.Cvetic,P.Langacker;Neutrino Masses within the Minimal Supersymmetric Standard Model
hep-th/9205030;hep-th;0;0;;H.Terao;Quantum Analysis of Jackiw and Teitelboim's Model for 1+1 D Gravity and Topological Gauge Theory
hep-ph/9205217;hep-ph;0;7;;M.Bander,H.Rubinstein;Screening of Very Intense Magnetic Fields by Chiral Symmetry Breaking
astro-ph/9205006;astro-ph,hep-lat;0;0;;B.Banerjee,R.V.Gavai;Can the Quark-Gluon Plasma in the Early Universe be supercooled?
hep-th/9205031;hep-th;0;0;;C.Bachas,M.Petropoulos;Topological Models on the Lattice and a Remark on String Theory Cloning
hep-ph/9205218;hep-ph;0;33;;T.G.Rizzo;New Probes for Extended Gauge Structures at HERA
hep-th/9205032;hep-th;0;29;;W.A.Sabra;Restricted Supergauge invariance, N=2 Coadjoint Orbit and N=2 Quantum Supergravity
hep-th/9205033;hep-th;0;36;;M.Fabbrichesi,K.Roland;Strong Antigravity. Life in the Shock Wave
hep-th/9205034;hep-th;0;35;;J.-L.Gervais;Gravity-Matter Couplings from Liouville Theory
hep-th/9205035;hep-th;0;13;;H.La;Sine-Gordon Solitons as Heterotic Fivebranes
hep-th/9205036;hep-th;0;31;;A.S.Goldhaber;Solitons with integer fermion number
hep-th/9205037;hep-th;2;29;hep-th/9108001,hep-th/9110054;I.Bars,K.Sfetsos;Global Analysis of New Gravitational Singularities in String and Particle Theories
cond-mat/9205007;cond-mat;0;24;;V.M.Yakovenko;Theory of Thermodynamic Magnetic Oscillations in Quasi-One-Dimensional Conductors
cond-mat/9205008;cond-mat;0;15;;V.M.Yakovenko;Metals in high magnetic field: a new universality class of Fermi liquids
hep-ph/9205219;hep-ph;0;0;;D.Atwood,C.P.Burgess,A.Soni;A General Lower Bound for Radiative B Decay
hep-ph/9205220;hep-ph;0;41;;A.S.Joshipura,S.D.Rindani;Fast Neutrino Decay in the Minimal Seesaw Model
hep-th/9205038;hep-th;0;0;;A.Ashtekar;Recent Developments in Classical and Quantum Theories of Connections, Including General Relativity
hep-th/9205039;hep-th,nlin.SI,solv-int;0;0;;P.P.Kulish,R.Sasaki,C.Schwiebert;Constant Solutions of Reflection Equations and Quantum Groups
hep-lat/9205010;hep-lat;0;9;;C.Michael;The Running Coupling from Lattice Gauge Theory
hep-th/9205040;hep-th;0;1;;P.Dorey;Partition Functions, Intertwiners and the Coxeter Element
hep-th/9205041;hep-th;0;0;;A.Klemm,S.Theisen;Considerations of One-Modulus Calabi-Yau Compactifications: Picard-Fuchs Equations, Kähler Potentials and Mirror Maps
hep-th/9205042;hep-th,hep-lat;0;0;;P.Suranyi;A New Field Theoretic Approach to Criticality
hep-ph/9205221;hep-ph;0;0;;B.Blok,M.Shifman;Nonfactorizable Amplitudes in Weak Nonleptonic Decays of Heavy Mesons
hep-th/9205043;hep-th;1;10;hep-th/9109007;J.Polchinski,Z.Yang;High Temperature Partition Function of the Rigid String
hep-th/9205044;hep-th;0;21;;T.Kuramoto;Quantum Hamiltonian Reduction of Super Kac-Moody Algebra II
hep-ph/9205222;hep-ph;0;15;;F.Csikor,Z.Fodor;Constraints on Mirror Fermion Mixing Angles from Anomalous Magnetic Moment Data
hep-th/9205045;hep-th;0;44;;S.Penati,D.Zanon;Supersymmetric, Integrable Toda Field Theories: The B(1,1) Model
hep-th/9205046;hep-th;0;0;;C.Kounnas,D.Luest;Cosmological String Backgrounds from Gauged WZW Models
hep-th/9205047;hep-th;1;19;0906.2817;E.Elizalde,S.D.Odintsov;Renormalization group equations in curved space-time with non-trivial Topology
hep-th/9205048;hep-th;0;26;;E.Elizalde,S.D.Odintsov;Higher derivative quantum gravity with torsion in the conformally Self-Dual Limit
hep-th/9205049;hep-th;0;42;;E.Elizalde,S.D.Odintsov;Spontaneous compactification in 2D induced quantum gravity
hep-th/9205050;hep-th;0;39;;E.Elizalde,S.D.Odintsov;Effective potential and stability of the rigid membrane
hep-th/9205051;hep-th;0;30;;R.R.Khuri;A Multimonopole Solution in String Theory
hep-th/9205052;hep-th;0;26;;R.R.Khuri;Scattering of String Monopoles
hep-th/9205053;hep-th;0;20;;N.Mohammedi;A Non Degenerate Semi-Classical Lagrangian for Dilaton-Gravity in Two Dimensions
hep-th/9205054;hep-th;0;0;;H.Lu,C.N.Pope,X.J.Wang,K.W.Xu;Aspects of N=2 Super-W_n Strings
hep-th/9205055;hep-th,nlin.SI,solv-int;0;0;;M.Jimbo,K.Miki,T.Miwa,A.Nakayashiki;Correlation Functions of the XXZ model for $Δ<-1$
hep-th/9205056;hep-th;0;0;;C.V.Johnson,T.R.Morris,A.Wätterstam;Global KdV Flows and Stable 2D Quantum Gravity
cond-mat/9205009;cond-mat;0;24;;F.Colomo,A.Izergin,V.Korepin,V.Tognetti;Determinant Representation for time and temperature dependent correlation functions in the isotropic XY model in the transverse magnetic field
hep-th/9205057;hep-th;0;10;;A.D'Adda;New Methods of Integration in Matrix Models
hep-th/9205058;hep-th;0;0;;A.A.Tseytlin;A class of finite two - dimensional sigma models and string vacua
hep-ph/9205223;hep-ph;0;0;;J.E.Kim;$θ$ Bag and Quark Confinement
hep-th/9205059;hep-th;0;27;;V.Kazakov,I.Kostov;Loop Gas Model for Open Strings
hep-th/9205060;hep-th,hep-ph;1;37;hep-th/9205068;M.Cvetič,R.L.Davis;Cosmological Implications of Domain Walls due to Duality Invariant Moduli Sector of Superstring Vacua
hep-th/9205061;hep-th;0;0;;J.Traschen,R.Ferrel;Quantum-Mechanical Scattering of Charged Black Holes
hep-th/9205062;hep-th;3;42;hep-th/9108001,hep-th/9109026,hep-th/9110065;S.K.Kar,S.P.Khastgir,G.Sengupta;Four Dimensional Stringy Black Membrane
hep-lat/9205011;hep-lat;0;18;;K.Jansen,Y.Shen;Tunneling and Energy Splitting in Ising Models
hep-lat/9205012;hep-lat;0;12;;S.V.Zenkin;Reflection positive formulation of chiral gauge theories on a lattice
hep-th/9205063;hep-th;4;82;hep-th/9109027,hep-th/9109032,hep-th/9111021,hep-th/9111031;U.H.Danielsson;A Study of Two Dimensional String Theory (PhD Thesis)
hep-th/9205064;hep-th;1;34;hep-th/9108007;D.Bernard,A.LeClair;The Quantum Double in Integrable Quantum Field Theory
funct-an/9205003;funct-an,math.OA;0;0;;V.G.Pestov;Nonstandard hulls of Banach-Lie groups and algebras
hep-th/9205065;hep-th;2;28;hep-th/9109032,hep-th/9201005;Vl.S.Dotsenko;The operator algebra of the discrete state operators in 2D gravity with non-vanishing cosmological constant
hep-th/9205066;hep-th;0;23;;H.Y.Lee,A.Nakamichi,T.Ueno;Topological 2-form Gravity in Four Dimensions
hep-ph/9205224;hep-ph;2;58;hep-th/9109049,hep-ph/9204213;J.Garcia-Bellido;Axions with Variable Masses
hep-th/9205067;hep-th;1;22;hep-th/9112006;P.Montague;Discussion of Self-Dual c=24 Conformal Field Theories
alg-geom/9205006;alg-geom,math.AG;0;0;;A.M.Bigatti;Upper Bounds for the Betti Numbers of a given Hilbert Function
hep-lat/9205013;hep-lat,hep-th;0;65;;G.Mack,T.Kalkreuter,G.Palma,M.Speh;Effective Field Theories
hep-th/9205068;hep-th;0;0;;V.Kaplunovsky;ERRATA for "One-Loop Threshold Effects in String Unification"
hep-th/9205069;hep-th;0;13;;S.P.de Alwis;Quantization of a Theory of 2d Dilaton Gravity
hep-th/9205070;hep-th;0;0;;V.Kaplunovsky;One-Loop Threshold Effects in String Unification
hep-ph/9205225;hep-ph;0;31;;D.Suematsu;Strong CP-Problem in Superstring Theory
hep-th/9205071;hep-th;1;25;hep-th/0209014;H.Grosse,W.Kummer,P.Prešnajder,D.J.Schwarz;Novel Symmetry of Non-Einsteinian Gravity in Two Dimensions
hep-th/9205072;hep-th;0;0;;A.N.Schellekens;Meromorphic c=24 Conformal Field Theories
hep-th/9205073;hep-th;0;28;;J.Ambjorn,C.F.Kristjansen;Non-perturbative 2d quantum gravity and hamiltonians unbounded from below
hep-ph/9205226;hep-ph;0;0;;J.Louis;Recent Developments in Superstring Phenomenology
hep-th/9205074;hep-th,math-ph,math.MP;0;16;;J.W.van Holten,R.H.Rietdijk;Symmetries and Motions in Manifolds
cond-mat/9205010;cond-mat;0;16;;M.Dong,M.C.Marchetti,A.A.Middleton,V.Vinokur;Elastic String in a Random Potential
hep-th/9205075;hep-th;0;0;;W.Siegel;The N=2(4) string is self-dual N=4 Yang-Mills
cond-mat/9205011;cond-mat;0;26;;A.A.Middleton;Thermal Rounding of the Charge Density Wave Depinning Transition
hep-ph/9205227;hep-ph;0;18;;M.Dine,D.A.MacIntire;Supersymmetry, Naturalness, and Dynamical Supersymmetry Breaking
hep-th/9205076;hep-th;0;21;;M.A.Martín-Delgado;The Critical Point of Unoriented Random Surfaces with a Non-Even Potential
hep-th/9205077;hep-th;0;55;;G.Bimonte,K.S.Gupta,A.Stern;Edge Currents and Vertex Operators for Chern-Simons Gravity
hep-lat/9205014;hep-lat,hep-th;0;0;;J.de Lyra,B.DeWitt,S.K.Foong,T.Gallivan,R.Harrington,A.Kapulkin,E.Myers,J.Polchinski;The Quantized $O(1,2)/O(2)×Z_2$ Sigma Model Has No Continuum Limit in Four Dimensions. I. Theoretical Framework
math/9205207;math.FA;0;28;;P.G.Casazza;Some Questions Arising from the Homogeneous Banach Space Problem
math/9205208;math.LO;0;0;;M.Goldstern,S.Shelah;Many simple cardinal invariants
math/9205209;math.DS,math.CV;0;0;;B.Bielefeld,M.Lyubich,L.Carleson,R.Devaney,A.Eremenko,C.McMullen,J.Milnor,F.Przytycki,M.Rees,S.Sutherland;Problems in holomorphic dynamics
hep-lat/9205015;hep-lat;0;29;;W.Wilcox,T.Draper,K.-F.Liu;Chiral Limit of Nucleon Lattice Electromagnetic Form Factors
hep-lat/9205016;hep-lat;0;10;;UKQCD Collaboration,C.R.Allton,H.Duong,C.T.Sachrajda,R.M.Baxter,S.P.Booth,K.C.Bowler,S.Collins,D.S.Henty,R.D.Kenway,C.McNeile,B.J.Pendleton,D.G.Richards,J.N.Simone,A.D.Simpson,B.E.Wilkes,A.Hulsebos,A.C.Irving,A.McKerrell,C.Michael,M.Prisznyak,P.W.Stephenson,G.Martinelli;Quenched Hadrons using Wilson and O(a)-Improved Fermion Actions at beta=6.2
hep-ph/9205228;hep-ph;0;24;;M.Luke,A.V.Manohar;Reparameterisation Invariance Constraints on Heavy Particle Effective Field Theories
hep-th/9205078;hep-th;0;0;;S.Mahapatra;Four Dimensional 2-Brane Solution in Chiral Gauged Wess-Zumino-Witten Model
hep-ph/9205229;hep-ph;0;9;;E.J.Chun,J.E.Kim,H.P.Nilles;Axino Mass
hep-ph/9205230;hep-ph;0;48;;E.Akhmedov,Z.Berezhiani,G.Senjanovic;Planck-Scale Physics and Neutrino Masses
alg-geom/9205007;alg-geom,math.AG;0;15;;S.Nag;On the Tangent Space to the Universal Teichmuller Space
hep-th/9205079;hep-th;0;34;;M.Henningson;Duality of string amplitudes in a curved background
hep-lat/9205017;hep-lat;0;0;;J.de Lyra,B.DeWitt,S.K.Foong,T.Gallivan,R.Harrington,A.Kapulkin,E.Myers,J.Polchinski;The Quantized $O(1,2)/O(2)×Z_2$ Sigma Model Has No Continuum Limit in Four Dimensions. II. Lattice Simulation
hep-lat/9205018;hep-lat,cond-mat,hep-ph,hep-th;0;16;;E.Marinari,G.Parisi;Simulated Tempering: A New Monte Carlo Scheme
hep-th/9205080;hep-th;0;23;;A.Anderson;Canonical Transformations in Quantum Mechanics
hep-th/9205081;hep-th;0;37;;R.R.Khuri;A Heterotic Multimonopole Solution
hep-lat/9205019;hep-lat;0;0;;I.M.Barbour,A.J.Bell,E.G.Klepfish;Critical mass in nonzero temperature QCD with staggered fermions
hep-th/9205082;hep-th;0;48;;S.G.Naculich,H.A.Riggs,H.J.Schnitzer;Simple-Current Symmetries, Rank-Level Duality, and Linear Skein Relations for Chern-Simons Graphs
hep-ph/9205231;hep-ph;0;0;;T.Bhattacharya,A.Gocksch,C.P.Korthals-Altes,R.D.Pisarski;Z(N) interface tension in a hot SU(N) gauge theory
hep-ph/9205232;hep-ph;0;22;;V.Jain;Finite Temperature Scalar Potential from a 1/N Expansion
hep-th/9205083;hep-th;0;18;;H.La;Solitons reduced from Heterotic fivebranes
hep-lat/9205020;hep-lat,hep-ph;0;38;;S.Sharpe;Quenched Chiral Logarithms
hep-th/9205084;hep-th;0;9;;H.Sonoda;Operator Coefficients for Composite Operators in the $(φ^4)_4$ Theory
hep-th/9205085;hep-th;0;6;;H.Sonoda;Composite Operators in QCD
hep-th/9205086;hep-th;0;0;;S.Durand;Fractional Superspace Formulation of Generalized Super-Virasoro Algebras
hep-th/9205087;hep-th;0;35;;T.Kobayashi,T.Uematsu;Differential Calculus on the Quantum Superspace and Deformation of Phase Space
cond-mat/9205012;cond-mat;0;12;;K.Harigaya,S.Abe;Dispersion of the Third-Order Nonlinear Optical Susceptibility in C_{60} Calculated with a Tight-Binding Model
hep-th/9205088;hep-th;0;4;;A.Schwarz;Geometry of Batalin-Vilkovisky quantization
hep-ph/9205233;hep-ph;0;69;;W.Fischler,S.Paban,S.Thomas;Bounds on Microscopic Physics from P and T Violation in Atoms and Molecules
hep-ph/9205234;hep-ph;0;0;;L.E.Ibáñez;Computing the Weak Mixing Angle from Anomaly Cancellation
cond-mat/9205013;cond-mat;0;11;;M.Sun,C.Ebner;Molecular Dynamics Simulation of Compressible Fluid Flow in Two-Dimensional Channels
hep-lat/9205021;hep-lat,hep-th;0;16;;J.Ambjorn,Z.Burda,J.Jurkiewicz,C.F.Kristjansen;3d quantum gravity coupled to matter
hep-lat/9205022;hep-lat;0;35;;J.Ambjørn,K.Farakos,M.E.Shaposhnikov;Parity breaking at high temperature and density
hep-ph/9205235;hep-ph;0;0;;P.V.Landshoff,A.Rebhan;Covariant gauges at finite temperature
hep-lat/9205023;hep-lat;0;34;;I.Montvay;Mirror fermions in chiral gauge theories
hep-lat/9205024;hep-lat;0;0;;I.M.Barbour,E.G.Klepfish;Grand Canonical Partition Function of a 2-dimensional Hubbard Model
hep-ph/9205236;hep-ph;0;0;;R.Oehme;Dispersion Relations in Quantum Chromodynamics
hep-ph/9205237;hep-ph;0;40;;L.Clavelli,P.W.Coulter,K.Yuan;Best Fit to the Gluino Mass
hep-lat/9205025;hep-lat,hep-th;0;0;;S.Aoki;Regularizations, Anomalies and Fermion Number Non-Conservation in Chiral Gauge Theories
hep-th/9205089;hep-th;0;13;;A.Bilal,C.Callan;Liouville Models of Black Hole Evaporation
hep-th/9205090;hep-th,hep-lat;1;34;hep-th/9108006;H.Ooguri;Topological Lattice Models in Four Dimensions
hep-th/9205091;hep-th;0;40;;R.R.Khuri;Monopoles and Instantons in String Theory
hep-th/9205092;hep-th;0;0;;M.Henneaux,C.Teitelboim,J.D.Vergara;Gauge Invariance for Generally Covariant Systems
hep-th/9205093;hep-th;0;24;;G.W.Delius,M.T.Grisaru,P.van Nieuwenhuizen;Induced (N,0) supergravity as a constrained Osp(N,2) WZWN model and its effective action
hep-th/9205094;hep-th;2;24;hep-th/9109053,hep-th/9205068;L.Dolan,J.T.Liu;Running Gauge Couplings and Thresholds in the Type II Superstring
hep-th/9205095;hep-th;0;4;;I.I.Kogan;About some exact solutions for 2+1 gravity coupled to gauge fields
cond-mat/9205014;cond-mat;0;23;;K.Harigaya;Lattice distortion and energy level structures in doped C_{60} and C_{70} studied with the extended Su-Schrieffer-Heeger model: Polaron excitations and optical absorption
hep-th/9205096;hep-th;0;44;;H.Cateau,K.Sumiyoshi;Thermal history of the string universe
hep-th/9205097;hep-th;0;10;;J.L.Montag;The One-Loop Five-Graviton Scattering Amplitude and Its Low-Energy Limit
hep-th/9205098;hep-th;0;23;;R.B.Mann,S.F.Ross;Matching Conditions and Gravitational Collapse in Two-Dimensional Gravity
hep-ph/9205238;hep-ph;0;10;;R.Barbieri,M.Beccaria,P.Ciafaloni,G.Curci,A.Vicere';Radiative Correction Effects of a Very Heavy Top
hep-ph/9205239;hep-ph;0;12;;T.C.Yuan;Anomalous Radiative Decay of Heavy Higgs Boson
cond-mat/9205015;cond-mat;0;23;;K.R.Elder,J.Viñals,M.Grant;Dynamic scaling and quasi-ordered states in the two dimensional Swift-Hohenberg equation
hep-lat/9205026;hep-lat,cond-mat,hep-th;0;13;;K.Yee;Central Charge of the Parallelogram Lattice Strong Coupling Schwinger Model
hep-th/9205099;hep-th;1;14;hep-th/9201019;J.A.Dixon,M.J.Duff;Chern-Simons Forms, Mickelsson-Faddeev Algebras and the P-Branes
hep-th/9205100;hep-th,cond-mat,hep-lat;0;34;;J.Distler;A note on the 3D Ising model as a string theory
hep-ph/9205240;hep-ph;0;23;;S.Dimopoulos,L.Hall,S.Raby;Predictions for neutral K and B meson physics
hep-lat/9205027;hep-lat,cond-mat;0;29;;P.Butera,M.Comi;High-Temperature series for the $RP^{n-1}$ lattice spin model (generalized Maier-Saupe model of nematic liquid crystals) in two space dimensions and with general spin dimensionality n
math/9205210;math.DS;0;0;;E.Bedford,M.Lyubich,J.Smillie;Polynomial diffeomorphisms of C^2, IV: The measure of maximal entropy and laminar currents
math/9205211;math.HO;0;0;;D.E.Knuth;Two notes on notation
hep-th/9205101;hep-th;2;32;hep-th/9108004,hep-th/9109032;N.Ohta,H.Suzuki;Interactions of Discrete States with Nonzero Ghost Number \\in $c=1$ $2D$ Gravity
hep-ph/9205241;hep-ph;0;0;;B.Blok,M.Shifman;Nonleptonic decays of K mesons revisited
hep-th/9205102;hep-th;0;0;;R.Zucchini;Light Cone $W_n$ Geometry and its Symmetries and Projective Field Theory
cond-mat/9205016;cond-mat;0;13;;K.Harigaya;C_{60} with O defects: Localized states in the gap and oxygen clustering
hep-th/9205103;hep-th;0;0;;L.Castellani;Gauge theories of quantum groups
hep-ph/9205242;hep-ph;0;9;;V.Bhansali,H.Georgi;Running Nonlocal Lagrangians
hep-ph/9205243;hep-ph;0;0;;E.Jenkins,A.V.Manohar,M.B.Wise;Baryons Containing a Heavy Quark as Solitons
hep-th/9205104;hep-th;1;28;hep-th/9204058;J.-S.Park;Universal Bundle, Generalized Russian Formula and Non-Abelian Anomaly in Topological Yang-Mills Theory
hep-th/9205105;hep-th;0;0;;J.Schiff;The KdV Action and Deformed Minimal Models
hep-th/9205106;hep-th;0;40;;L.Chekhov;Matrix Model for Discretized Moduli Space
hep-th/9205107;hep-th;8;62;hep-th/9108026,hep-th/9108027,hep-th/9109012,hep-th/9109027,hep-th/9109032,hep-th/9111001,hep-th/9111031,hep-th/9112062;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;The Origin of Space-Time as $W$ Symmetry Breaking in String Theory
hep-th/9205108;hep-th;0;23;;R.R.Khuri;Exact Solutions in Bosonic and Heterotic String Theory
hep-ph/9205244;hep-ph;0;38;;E.Akhmedov;Resonant Spin-Flavor Precession of Neutrinos As a Possible Solution to the Solar Neutrino Problem
hep-th/9205109;hep-th,cond-mat;1;22;hep-th/9108017;R.Cuerno,G.Sierra,C.Gomez;On Integrable Quantum Group Invariant Antiferromagnets
hep-th/9205110;hep-th;0;41;;I.M.Krichever;The $τ$-function of the universal Whitham hierarchy, matrix models and topological field theories
hep-th/9205111;hep-th;0;0;;H.Ikemori;Extended form method of antifield-BRST formalism for BF theories
hep-lat/9205028;hep-lat;0;35;;S.Klessinger,G.Muenster;Numerical Investigation of the Interface Tension in the three-dimensional Ising Model
hep-th/9205112;hep-th;0;7;;A.Anderson;The Global Problem of Time
hep-ph/9205245;hep-ph;0;0;;J.Liu,Y.-P.Yao;QCD Corrections to the Charged-Higgs-Boson Decay of a Heavy Top Quark
hep-th/9205113;hep-th;2;27;hep-th/9109001,hep-th/9110052;P.C.Argyres,E.Lyman,S.-H.H.Tye;Low-Lying States of the Six-Dimensional Fractional Superstring
hep-lat/9205029;hep-lat,hep-th;0;0;;R.L.Renken,S.M.Catterall,J.B.Kogut;Three Dimensional Quantum Gravity Coupled to Ising Matter
hep-lat/9205030;hep-lat;0;0;;V.Azcoiti,G.D.Carlo,A.F.Grillo;Renormalization group and triviality in noncompact lattice QED with light fermions
hep-th/9205114;hep-th;0;22;;A.Peet,L.Susskind,L.Thorlacius;Information Loss and Anomalous Scattering
hep-th/9205115;hep-th;0;17;;H.-C.Kao,K.Lee;Self-Dual Chern-Simons Higgs Systems with an N=3 Extended Supersymmetry
hep-ph/9205246;hep-ph;0;0;;G.R.Goldstein,K.Sliwa,R.H.Dalitz;On Observing Top Quark Production at the Tevatron
hep-ph/9205247;hep-ph;0;0;;A.Pomarol;Higgs sector CP violation in the Minimal Supersymmetric Model
hep-th/9205116;hep-th;0;30;;A.P.Balachandran,P.Teotonio-Sobrinho;The Edge States of the BF System and the London Equations
hep-th/9205117;hep-th;1;24;hep-th/9112009;F.Yu,Y.-S.Wu;An Infinite Number of Commuting Quantum $\hat W_∞$ Charges in the $SL(2,R)/U(1)$ Coset Model
hep-th/9206001;hep-th;0;20;;A.Berkovich,G.Sierra,C.Gomez;q--Magnetism at roots of unity
hep-th/9206002;hep-th;0;24;;O.Babelon,D.Bernard;Affine Solitons: A Relation Between Tau Functions, Dressing and Bäcklund Transformations
hep-ph/9206201;hep-ph,astro-ph;0;0;;S.Ben-Menahem,A.R.Cooper;Baryogenesis from Unstable Domain Walls
hep-th/9206003;hep-th;1;24;hep-th/9206002;O.Babelon,D.Bernard;From Form Factors to Correlation Functions: The Ising Model
math/9206201;math.FA;0;0;;S.J.Dilworth,S.J.Montgomery-Smith;The distribution of vector-valued Rademacher series
hep-ph/9206202;hep-ph;0;31;;T.Elliott,S.F.King;Heavy Axions From Strong Broken Horizontal Gauge Symmetry
hep-th/9206004;hep-th;0;0;;M.Cvetic,S.Griffies,S.-J.Rey;Nonperturbative Stability of Supergravity and Superstring Vacua
hep-th/9206005;hep-th;0;0;;J.Mickelsson;Vacuum Expectation Values of Products of Chiral Currents in $3+1$ Dimensions
hep-ph/9206203;hep-ph;0;22;;J.Ellis,S.Kelley,D.V.Nanopoulos;Constraints From Gauge Coupling Unification On The Scale Of Supersymmetry Breaking
hep-th/9206006;hep-th;4;28;hep-th/9108001,hep-th/9109048,hep-th/9110054,hep-th/9205037;I.Bars,K.Sfetsos;Conformally Exact Metric and Dilaton in String Theory on Curved Spacetime
hep-th/9206007;hep-th;0;68;;G.Giavarini,C.P.Martin,F.R.Ruiz;Chern-Simons Theory as the Large Mass Limit of Topologically Massive Yang-Mills Theory
hep-th/9206008;hep-th;0;23;;K.Huitu;Modular Invariants of $N=2$ Supersymmetric $SU(1,1)$ Models
hep-th/9206009;hep-th;0;0;;J.-M.Shen,Z.-M.Sheng,Z.-H.Wang;Quantum Liouville Theory On The Riemann Sphere With $n>3$ Punctures
hep-lat/9206001;hep-lat;0;38;;F.R.Brown,H.Chen,N.H.Christ,Z.Dong,R.D.Mawhinney,W.Schaffer,A.Vaccarino;Lattice QCD with 8 Light Quark Flavors
alg-geom/9206001;alg-geom,math.AG;0;0;;P.Aluffi,C.Faber;Linear orbits of smooth plane curves
hep-lat/9206002;hep-lat,hep-th;0;3;;A.A.Migdal;Exact Solution of Induced Lattice Gauge Theory at Large $N$
cond-mat/9206001;cond-mat;0;13;;O.Biham,A.A.Middleton,D.Levine;Self Organization and a Dynamical Transition in Traffic Flow Models
hep-th/9206010;hep-th;0;17;;A.Hietamaki,A.J.Niemi;Index Theorems and Loop Space Geometry
hep-th/9206011;hep-th;0;34;;D.C.Cabra;Zamolodchikov's c-function for the Chiral Gross-Neveu Model
hep-ph/9206204;hep-ph;0;16;;M.K.Gaillard;Interpretation of Precision Measurements in the Strongly Interacting Limit of the Standard Electroweak Model
hep-th/9206012;hep-th;5;101;hep-th/9108004,hep-th/9108027,hep-th/9109032,hep-th/9111021,hep-th/9111048;N.Ohta;Discrete States in Two-Dimensional Quantum Gravity
cond-mat/9206002;cond-mat;0;18;;N.Yu,M.Fowler;Twisted Boundary Conditions and the Adiabatic Ground State for the Attractive XXZ Luttinger Liquid
hep-lat/9206003;hep-lat;0;11;;A.C.Irving,C.Michael;Finite size effects and scaling in lattice CP(N-1)
hep-lat/9206004;hep-lat;0;27;;C.R.Gattringer,C.B.Lang;Resonance Scattering Phase Shifts in a 2-d Lattice Model
hep-th/9206013;hep-th;0;9;;S.Majid,M.J.Rodriguez-Plaza;Quantum and super-quantum group related to the Alexander-Conway polynomial
hep-lat/9206005;hep-lat;0;44;;J.L.Alonso,Ph.Boucaud,J.L.Cortes,F.Lesmes,E.Rivas;Massless Decoupled Doublers: Chiral Yukawa Models and Chiral Gauge Theories
alg-geom/9206002;alg-geom,math.AG;0;0;;A.Ruffing,T.Deck,M.Schlichenmaier;String Branchings on Complex Tori and Algebraic Representations of Generalized Krichever-Novikov Algebras
hep-lat/9206006;hep-lat;0;17;;J.C.Vink,U.-J.Wiese;Gauge Fixing on the Lattice without Ambiguity
hep-ph/9206205;hep-ph;0;8;;A.Antaramian,L.J.Hall,A.Rašin;Flavor changing interactions mediated by scalars at the weak scale
hep-ph/9206206;hep-ph,hep-th;2;29;hep-th/9109053,hep-th/9201047;M.K.Gaillard,R.Xiu;Analysis of Running Coupling Constant Unification in String Theory
hep-th/9206014;hep-th;4;46;hep-th/9108004,hep-th/9109005,hep-th/9109032,hep-th/9201005;N.Marcus,Y.Oz;Discrete States of 2D String Theory in Polyakov's Light-Cone Gauge
hep-th/9206015;hep-th;0;6;;V.A.Kazakov,A.A.Migdal;Induced QCD at Large N
hep-th/9206016;hep-th;0;0;;A.Sen;Macroscopic Charged Heterotic String
hep-th/9206017;hep-th;0;0;;S.P.Khastgir,J.Maharana;Symmetries of String Effective Action and Space-Time Geometry
hep-ph/9206207;hep-ph;0;9;;G.B.West;Reply to Comments on ``Asymptotic Estimate of the {\it n}-Loop QCD Contribution to the Total $e^+e^-$ Annihilation Cross Section''
hep-lat/9206007;hep-lat;0;24;;R.Brower,P.Tamayo;Virtual Bond Percolation for Ising Cluster Dynamics
hep-lat/9206008;hep-lat;0;21;;W.Bock,J.Smit,J.C.Vink;Fermion-Higgs model with Reduced Staggered Fermions
hep-lat/9206009;hep-lat;0;11;;D.S.Henty,R.D.Kenway;Hopping Parameter Expansion for Heavy-Light Systems
alg-geom/9206003;alg-geom,math.AG;0;9;;N.M.Kumar;Affine like Surfaces
hep-ph/9206208;hep-ph;0;13;;M.Leurer;Can HERA See an $e u --> e c$ Signal of a Virtual Leptoquark?
hep-th/9206018;hep-th;0;16;;S.Mignemi,N.R.Stewart;Dilaton-Axion hair for slowly rotating Kerr black holes
hep-th/9206019;hep-th;0;20;;L.Baulieu;Transmutation of Pure 2-D Supergravity Into Topological 2-D Gravity and Other Conformal Theories
hep-ph/9206209;hep-ph;0;0;;P.Langacker,J.Liu;Standard Model Contributions to the Neutrino Index of Refraction in the Early Universe
hep-th/9206020;hep-th;0;14;;S.P.de Alwis;Black Hole Physics from Liouville Theory
hep-th/9206021;hep-th,math.QA;0;18;;D.S.Freed;Classical Chern-Simons theory, Part 1
hep-th/9206022;hep-th;1;12;hep-th/9111056;R.B.Mann,S.F.Ross;Gravitation & Cosmology in $(1+1)$-dimensional Dilaton Gravity
hep-ph/9206210;hep-ph;0;50;;D.Choudhury;Discrete Symmetry, Neutrino Magnetic Moment and the 17 Kev Neutrino
hep-th/9206023;hep-th;1;43;hep-th/9109032;A.Giveon;On String Field Theory and Effective Actions
hep-th/9206024;hep-th;0;7;;P.Schupp,P.Watts,B.Zumino;The 2-Dimensional Quantum Euclidean Algebra
hep-lat/9206010;hep-lat;0;0;;M.Golterman,D.Petcher,E.Rivas;Absence of Chiral Fermions in the Eichten--Preskill Model
hep-ph/9206211;hep-ph;0;13;;M.Bander,H.Rubinstein;Hadronic Instabilities in Very Intense Magnetic Fields
hep-lat/9206011;hep-lat;0;0;;T.A.DeGrand,M.W.Hecht;More about orbitally excited hadrons from lattice QCD
hep-th/9206025;hep-th;0;0;;J.S.Dowker,A.Wolski;A finite model of two-dimensional ideal hydrodynamics
hep-th/9206026;hep-th;0;30;;E.Bergshoeff,L.A.J.London,P.K.Townsend;Spacetime Scale-Invariance and the Super p-Brane
hep-th/9206027;hep-th,cond-mat;0;53;;A.Cappelli,C.A.Trugenberger,G.R.Zemba;Infinite Symmetry in the Quantum Hall Effect
math/9206202;math.FA;0;0;;N.J.Kalton,P.Wojtaszczyk;On nonatomic Banach lattices and Hardy spaces
math/9206203;math.CO;0;0;;G.Andrews,S.B.Ekhad,D.Zeilberger;A Short Proof of Jacobi's Formula for the Number of Representations of an Integer as a Sum of Four Squares
math/9206204;math.FA;0;1;;A.Kriegl,P.W.Michor;More smoothly real compact spaces
hep-ph/9206212;hep-ph;0;0;;A.Masiero,A.Riotto;Cosmic $ΔB$ from Lepton Violating Interactions at the Electroweak Phase Transition
hep-th/9206028;hep-th;0;0;;D.Z.Freedman,K.Johnson,R.Munoz-Tapia,X.Vilasis-Cardona;A Cutoff Procedure and Counterterms for Differential Renormalization
hep-th/9206029;hep-th,math.QA;0;17;;P.Schupp,P.Watts,B.Zumino;Differential Geometry on Linear Quantum Groups
hep-th/9206030;hep-th;0;0;;K.Takasaki;W algebra, twistor, and nonlinear integrable systems
hep-lat/9206012;hep-lat;0;31;;C.F.Baillie,D.A.Johnston;An Effective Model for Crumpling in Two Dimensions?
hep-th/9206031;hep-th;0;9;;C.M.Hull,L.Palacios;Singular Contractions of W-algebras
hep-th/9206032;hep-th;0;0;;L.Begin,P.Mathieu,M.A.Walton;su(3)k fusion coefficients
hep-th/9206033;hep-th;0;20;;A.J.Niemi,O.Tirkkonen;Cohomological Partition Functions for a Class of Bosonic Theories
hep-ph/9206213;hep-ph;0;11;;H.Goldberg;Exact Nonperturbative Unitary Amplitudes for 1->N Transitions
hep-th/9206034;hep-th;0;0;;A.Kuniba,T.Nakanishi;Spectra in Conformal Field Theories from the Rogers Dilogarithm
hep-th/9206035;hep-th;0;16;;E.Brézin,J.Zinn-Justin;Renormalization Group Approach to Matrix Models
hep-th/9206036;hep-th;0;0;;J.S.Dowker,P.Chang;Polyhedral Cosmic Strings
hep-th/9206037;hep-th;0;0;;B.Dubrovin;Geometry and Integrability of Topological-Antitopological Fusion
hep-th/9206038;hep-th;0;0;;G.Dunne,N.Rius;A Comment on the Relationship Between Differential and Dimensional Renormalization
hep-th/9206039;hep-th;0;0;;M.Leblanc,G.Lozano,H.Min;Extended Superconformal Galilean Symmetry in Chern-Simons Matter Systems
hep-th/9206040;hep-th;0;0;;F.Martinez-Moras,E.Ramos;Higher Dimensional Classical W-Algebras
hep-th/9206041;hep-th;0;55;;A.LeClair,D.Nemeschansky,N.P.Warner;S-matrices for Perturbed N=2 Superconformal Field Theory from quantum groups
hep-th/9206042;hep-th;0;0;;Y.Imamura,M.Sakamoto,T.Sasada,M.Tabuse;Symmetries between Untwisted and Twisted Strings on Asymmetric Orbifolds
hep-th/9206043;hep-th;1;31;hep-th/9111056;E.Elizalde,S.D.Odintsov;One-loop divergences in two-dimensional Maxwell-dilaton quantum gravity
hep-th/9206044;hep-th;0;21;;R.B.Mann;Conservation Laws and 2D Black Holes in Dilaton Gravity
hep-th/9206045;hep-th;0;18;;H.J.Schnitzer;Concerning the Double Scaling Limit in the $O(N)$ Vector Model in Four-Dimensions
hep-th/9206046;hep-th,cond-mat;1;15;hep-th/9110064;J.A.Minahan,A.P.Polychronakos;Integrable Systems for Particles with Internal Degrees of Freedom
cond-mat/9206003;cond-mat;0;5;;E.Abrahams,A.Balatsky,J.R.Schrieffer,P.B.Allen;Interactions for odd-omega gap singlet superconductors
hep-th/9206047;hep-th;0;0;;L.Mezincescu,R.I.Nepomechie;Addendum to ``Integrability of Open Spin Chains with Quantum Algebra Symmetry''
hep-ph/9206214;hep-ph;0;38;;A.G.Cohen,D.B.Kaplan,A.E.Nelson;Debye Screening and Baryogenesis during the Electroweak Phase Transition
hep-th/9206048;hep-th;6;40;hep-th/9108001,hep-th/9109048,hep-th/9110053,hep-th/9110054,hep-th/9205037,hep-th/9206006;K.Sfetsos;Conformally Exact Results for SL(2,R)×SO(1,1)^{d-2}/SO(1,1) Coset Models
hep-lat/9206013;hep-lat,hep-ph;1;45;hep-lat/9204017;D.B.Kaplan;A Method for Simulating Chiral Fermions on the Lattice
hep-lat/9206014;hep-lat,hep-ph;0;17;;K.Jansen;Chiral Fermions and Anomalies on a Finite Lattice
hep-ph/9206215;hep-ph;0;35;;Y.Ono,D.Suematsu;Neutrino Magnetic Moment Model and Solar Neutrino Problem
hep-th/9206049;hep-th;0;13;;L.Brink,T.H.Hansson,M.A.Vasiliev;Explicit Solution to the N-Body Calogero Problem
hep-th/9206050;hep-th;1;16;hep-th/9111015;R.Munoz-Tapia;A New Approach to Lower Dimensional Gauge Theories
hep-ph/9206216;hep-ph,hep-th;0;12;;J.Preskill;Semilocal Defects
hep-th/9206051;hep-th;4;23;hep-th/9109026,hep-th/9109038,hep-th/9110004,hep-th/9110067;A.Kumar;Gauged String Actions and O($\tilde d$, $\tilde d$) Transformation
hep-ph/9206217;hep-ph;0;27;;F.Close,Z.Li;Effective Heavy Quark Theory
hep-th/9206052;hep-th;0;1;;P.Dorey,F.Ravanini;Staircase Models from Affine Toda Field Theory
hep-ph/9206218;hep-ph;1;134;hep-th/9205068;S.Kelley,J.Lopez,D.Nanopoulos,H.Pois,K.Yuan;Aspects of Radiative Electroweak Symmetry Breaking in Supergravity Models
hep-lat/9206015;hep-lat;0;44;;C.F.Baillie,D.A.Johnston;The XY Model Coupled to Two-Dimensional Quantum Gravity
alg-geom/9206004;alg-geom,math.AG;0;0;;Y.-G.Ye;Extremal Rays and Null Geodesics on a Complex Conformal Manifold
hep-th/9206053;hep-th;2;16;hep-th/9109005,hep-th/9109024;H.Dorn,H.-J.Otto;On Correlation Functions for Non-critical Strings with c<1 but d>1
hep-ph/9206219;hep-ph;0;18;;F.del Aguila,B.Alles,Ll.Ametller,A.Grau;Z' Decays into Four Fermions
hep-th/9206054;hep-th;0;0;;E.Abdalla,M.C.B.Abdalla,D.Dalmazi;On the amplitudes for non-critical n=2 supuerstrings
hep-th/9206055;hep-th,hep-ph;2;30;hep-th/9111056,hep-th/9201061;T.Banks,M.O'Loughlin;Classical and Quantum Production of Cornucopions At Energies Below $10^{18}$ GeV
hep-ph/9206220;hep-ph;0;48;;M.Dine;Electroweak Baryogenesis: An Overview (Where are We Now?)
alg-geom/9206005;alg-geom,math.AG;0;13;;V.Alexeev;Two Two-dimensional Terminations
hep-th/9206056;hep-th,gr-qc;0;0;;M.Srednicki;Is Purity Eternal?
cond-mat/9206004;cond-mat;0;48;;M.-D.Lacasse,J.Vinals,M.Grant;New Dynamic Monte Carlo Renormalization Group Method
hep-th/9206057;hep-th;0;35;;T.Deguchi,Y.Akutsu;Colored Vertex Models, Colored IRF Models and Invariants of Trivalent Colored Graphs
hep-th/9206058;hep-th;0;0;;V.Husain;Ashtekar variables, self-dual metrics and w-infinity
hep-th/9206059;hep-th;0;0;;W.A.Sabra;Hidden Kac-Moody symmetry and 2D Quantum Supergravity
hep-th/9206060;hep-th;0;0;;S.Dalley,C.V.Johnson,T.R.Morris,A.Watterstam;Unitary Matrix Models and 2D Quantum Gravity (Virasoro constraints modified)
hep-ph/9206221;hep-ph;0;0;;J.L.Hewett,T.G.Rizzo;Probing New Gauge Boson Couplings via Three-Body Decays
hep-ph/9206222;hep-ph,hep-lat;1;49;hep-ph/9204220;R.S.Chivukula,M.Dugan,M.Golden;Analyticity, Crossing Symmetry and the Limits of Chiral Perturbation Theory
hep-ph/9206223;hep-ph;0;44;;R.G.Leigh;Infrared Effects and Bubble Propagation at the Electroweak Phase Transition
math/9206205;math.DS;0;14;;J.Graczyk,G.Swiatek;Singular measures in circle dynamics
hep-th/9206061;hep-th;0;0;;H.Ikemori;Extended form method of antifield-BRST formalism for topological quantum field theories
hep-th/9206062;hep-th;1;8;hep-th/9109007;M.Natsuume;Nonlinear Sigma Model for String Solitons
hep-th/9206063;hep-th;0;26;;O.Aharony,J.Sonnenschein,S.Yankielowicz;G/G Models and W_N strings
hep-ph/9206224;hep-ph;0;12;;H.Goldberg,M.T.Vaughn;Exact Nonperturbative Unitary Amplitudes for 1->8 Transitions in a Field Theoretic Model
hep-th/9206064;hep-th;0;0;;R.Lafrance,R.Myers;What unitary matrix models are not?
alg-geom/9206006;alg-geom,math.AG;0;4;;J.-F.Mestre;Corps quadratiques dont le 5-rang du groupe des classes est >=3
astro-ph/9206001;astro-ph,hep-ph;0;0;;R.H.Brandenberger,A.-C.Davis;Electroweak Baryogenesis with Electroweak Strings
alg-geom/9206007;alg-geom,math.AG;0;0;;J.-F.Mestre;Rang de courbes elliptiques d'invariant donne
hep-ph/9206225;hep-ph;0;30;;R.Sundrum,S.D.H.Hsu;Walking Technicolor and Electroweak Radiative Corrections
hep-ph/9206226;hep-ph;0;22;;E.Ma;Fixing the Top-Quark and Higgs-Boson Masses
hep-th/9206065;hep-th;0;0;;T.Altherr,T.Grandou;Thermal Field Theory and Infinite Statistics
hep-th/9206066;hep-th;0;0;;C.V.Johnson,T.R.Morris,P.L.White;The Boundary Cosmological Constant in Stable 2D Quantum Gravity
hep-th/9206067;hep-th;0;0;;A.A.Tseytlin;String cosmology and dilaton
hep-lat/9206016;hep-lat;0;14;;M.G.Perez,A.Gonzalez-Arroyo;Numerical study of Yang-Mills classical solutions on the twisted torus
hep-ph/9206227;hep-ph;0;37;;J.R.Espinosa,M.Quirós,F.Zwirner;On the phase transition in the scalar theory
hep-ph/9206228;hep-ph,astro-ph;0;0;;J.M.Gelb,W.Kwong,S.P.Rosen;Implications of New Gallex Results for the MSW Solution of the Solar Neutrino Problem
hep-ph/9206229;hep-ph,hep-th;0;82;;M.Hindmarsh;Semilocal Topological Defects
alg-geom/9206008;alg-geom,math.AG;0;0;;R.Donagi;The fibers of the Prym map
hep-ph/9206230;hep-ph;0;37;;J.L.Goity;Chiral Perturbation Theory for SU(3) Breaking in Heavy Meson Systems
hep-ph/9206231;hep-ph;0;7;;E.Ma;Accidental Approximate Generation Universality and its Possible Verification
hep-th/9206068;hep-th;0;0;;R.-R.Hsu,G.Huang,W.-F.Lin;Uniqueness of the Axionic Kerr Black Hole
hep-th/9206069;hep-th;0;0;;E.Witten;Two Dimensional String Theory And Black Holes
hep-th/9206070;hep-th;0;16;;J.Russo,L.Susskind,L.Thorlacius;The Endpoint of Hawking Evaporation
hep-ph/9206232;hep-ph,astro-ph;0;0;;R.H.Brandenberger,A.-C.Davis,A.M.Matheson,M.Trodden;Superconducting Cosmc Strings and Primordial Magnetic Fields
hep-th/9206071;hep-th;0;23;;K.Hamada;Quantum Theory of Dilaton Gravity in 1+1 Dimensions
cond-mat/9206005;cond-mat,hep-lat,hep-th;1;37;hep-th/9110046;A.Moroz;Dimensional Reduction of a Generalized Flux Problem
astro-ph/9206002;astro-ph;0;0;;D.Thomas,D.N.Schramm,K.A.Olive,B.D.Fields;Primordial Nucleosynthesis and the Abundances of Beryllium and Boron
cond-mat/9206006;cond-mat;1;31;cond-mat/9204007;R.D.Kamien,D.R.Nelson;Directed Polymer Blends and Quantum Critical Phenomena
hep-th/9206072;hep-th;0;0;;J.R.Anglin,R.C.Myers;Wormholes and Supersymmetry
hep-th/9206073;hep-th,cond-mat;0;0;;T.J.Allen,A.J.Bordner;Charged Vortex Dynamics in Ginzburg-Landau Theory of the Fractional Quantum Hall Effect
hep-ph/9206233;hep-ph,astro-ph;0;0;;D.P.Bennett,A.Stebbins,F.R.Bouchet;The Implications of the COBE-DMR Results for Cosmic Strings
hep-ph/9206234;hep-ph;0;0;;S.H.Rhie,D.P.Bennett;Hopf Textures
hep-ph/9206235;hep-ph;0;66;;C.G.Boyd,D.E.Brahm,S.D.H.Hsu;Corrections to the Electroweak Effective Action at Finite Temperature
hep-ph/9206236;hep-ph;0;62;;J.Bijnens,C.Bruno,E.de Rafael;Nambu Jona-Lasinio Like Models and the Low Energy Effective Action of QCD
hep-th/9206074;hep-th,cond-mat,funct-an,hep-lat,hep-ph,math.FA;0;175;;A.Moroz;Quantum Field Theory as a Problem of Resummation (Short guide to using summability methods)
hep-th/9206075;hep-th;0;0;;Z.Bajnok,L.Palla,G.Takacs;A2 Toda theory in reduced WZNW framework and the representations of the W algebra
hep-th/9206076;hep-th;0;0;;A.Das,E.Sezgin,Z.Khviengia;Self-Duality in 3+3 Dimensions and the KP Equation
hep-th/9206077;hep-th;4;46;hep-th/9109027,hep-th/9111001,hep-th/9111031,hep-th/9112062;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;World-Sheet Duality, Space-Time Foam, and the Quantum Fate of a Stringy Black Hole
cond-mat/9206007;cond-mat;0;14;;A.M.Tsvelik;New Fermionic Description of Quantum S = 1/2 Antiferromargnet
hep-th/9206078;hep-th;1;19;hep-th/9110067;C.R.Nappi,E.Witten;A Closed, Expanding Universe in String Theory
astro-ph/9206003;astro-ph,hep-ph;0;0;;J.H.MacGibbon,R.H.Brandenberger;Gamma Ray Signatures from Ordinary Cosmic Strings
hep-th/9206079;hep-th;0;0;;N.Kaloper;Stringy Cosmic Strings and Axion Cohomology
hep-ph/9206237;hep-ph;0;26;;J.R.Cudell,B.Margolis;Perturbative QCD Corrections to the Soft Pomeron
hep-ph/9206238;hep-ph;0;4;;A.E.Faraggi,B.Grinstein,S.Meshkov;Comment On ``Grand Unification and Supersymmetric Threshold"
hep-th/9206080;hep-th;0;0;;D.Ghoshal,D.P.Jatkar,S.Mukhi;Kleinian Singularities and the Ground Ring of C=1 String Theory
hep-ph/9206239;hep-ph;0;0;;R.Baier,G.Kunstatter,D.Schiff;Gauge Dependence of the Resummed Thermal Gluon Self Energy
hep-th/9206081;hep-th;0;0;;H.Kawai,Y.Kitazawa,M.Ninomiya;Scaling Exponents in Quantum Gravity near Two Dimensions
hep-ph/9206240;hep-ph;0;14;;P.Elmfors;Finite Temperature Renormalization of the $(φ^3)_6$- and $(φ^4)_4$-Models at Zero Momentum
hep-ph/9206241;hep-ph;0;17;;A.F.Falk,M.Luke;Strong Decays of Excited Heavy Mesons In Chiral Perturbation Theory
hep-lat/9206017;hep-lat;0;24;;J.-D.Wang,C.DeTar;Tunneling and the Spectrum of the Potts Model
hep-th/9206082;hep-th;1;11;hep-th/9201019;J.A.Dixon;BRS Operators and Covariant Derivatives in Loop Space for P-Branes Coupled to Yang-Mills
hep-ph/9206242;hep-ph;0;15;;F.Pisano,V.Pleitez;$SU(3)⊗U(1)$ Model for Electroweak Interactions
hep-lat/9206018;hep-lat,hep-ph;0;20;;A.Kocic,J.B.Kogut,M.-P.Lombardo,K.C.Wang;Spectroscopy, Scaling and Critical Indices in Strongly Coupled Quenched QED
hep-ph/9206243;hep-ph;0;0;;D.E.Brahm;Complex Effective Potentials and Critical Bubbles
astro-ph/9206004;astro-ph;0;0;;P.Fischer,D.L.Welch,M.Mateo;Dynamics of the Intermediate-Age Elliptical LMC Cluster NGC 1978
hep-ph/9206244;hep-ph;0;6;;J.Agrawal,P.H.Frampton,D.Ng;Dilepton Production in $e^- p$ and $e^+ e^-$ Colliders
hep-ph/9206245;hep-ph;0;9;;G.W.Anderson;Remarks on the Electroweak Phase Transition
hep-th/9206083;hep-th;2;45;hep-th/9109053,hep-th/9205068;J.A.Casas,F.Gómez,C.Muñoz;Fitting the Quark and Lepton Masses in String Theories
hep-lat/9206019;hep-lat;0;28;;V.Singh,R.W.Haymaker,D.A.Browne;London relation and fluxoid quantization for monopole currents in U(1) lattice gauge theory
hep-th/9206084;hep-th;1;63;hep-th/9202015;B.Zwiebach;Closed String Field Theory: Quantum Action and the BV Master Equation
hep-ph/9206246;hep-ph;0;23;;T.Han,G.Valencia,S.Willenbrock;Structure Function Approach to Vector-Boson Scattering in pp Collisions
hep-th/9206085;hep-th;0;0;;M.Srednicki;A New Construction of the Penner Model
hep-th/9206086;hep-th;0;21;;S.Nojiri;$N=\half $ Superstring in Zero Dimension and the Spontaneous Breakdown of the Supersymmetry
hep-th/9206087;hep-th;0;13;;S.Nojiri,I.Oda;Charged Dilatonic Black Hole and Hawking Radiation in Two Dimensions
hep-ph/9206247;hep-ph;0;18;;K.Choi;Light Quark Masses and Quarkonium Decays
astro-ph/9206005;astro-ph,hep-ph;0;21;;R.Brandenberger,V.Mukhanov,T.Prokopec;Entropy of a Classical Stochastic Field and Cosmological Perturbation
hep-th/9206088;hep-th;0;17;;G.P.Korchemsky;Loops in the Curvature Matrix Model
hep-th/9206089;hep-th;1;33;hep-th/9110073;J.-P.Ader,F.Gieres,Y.Noirot;Relating Weyl and diffeomorphism anomalies on super Riemann surfaces
hep-th/9206090;hep-th,math.QA;0;6;;P.D.Francesco,C.Itzykson,J.-B.Zuber;Polynomial averages in the Kontsevich model
hep-lat/9206020;hep-lat;0;0;;G.Bhanot,M.Creutz,J.Lacki;Low temperature expansion for the 3-d Ising Model
hep-th/9206091;hep-th;0;21;;H.Itoyama;Integrable Superhierarchy of Discretized 2d Supergravity
hep-th/9206092;hep-th;0;0;;R.Jackiw,S.-Y.Pi;Finite and Infinite Symmetries in (2+1)-Dimensional Field Theory
hep-th/9206093;hep-th;0;0;;R.Jackiw;Gauge Theories for Gravity on a Line
hep-th/9206094;hep-th;0;0;;S.Deser,R.Jackiw;Time Travel?
cond-mat/9206008;cond-mat;0;21;;T.Hwa;The Nonequilibrium Dynamics of Driven Line Liquids
hep-th/9206095;hep-th,hep-lat;0;11;;I.I.Kogan,G.W.Semenoff,N.Weiss;Induced QCD and Hidden Local ZN Symmetry
hep-th/9206096;hep-th;1;38;hep-th/9112009;H.Aratyn,L.A.Ferreira,J.F.Gomes,A.H.Zimerman;On Two-Current Realization of KP Hierarchy
hep-lat/9206021;hep-lat,hep-th;0;0;;S.M.Catterall,J.B.Kogut,R.L.Renken;Numerical Study of c>1 Matter Coupled to Quantum Gravity
alg-geom/9206009;alg-geom,math.AG;0;19;;G.Mikhalkin;The complex separation and extensions of Rokhlin congruence for curves on surfaces
hep-th/9206097;hep-th;0;23;;F.D.Jonghe,R.Siebelink,W.Troost,S.Vandoren,P.van Nieuwenhuizen,A.V.Proeyen;The regularized BRST Jacobian of pure Yang-Mills theory
hep-th/9206098;hep-th;0;57;;J.de Boer,J.Goeree;Covariant $W$ Gravity & its Moduli Space from Gauge Theory
hep-th/9206099;hep-th;0;18;;J.Alfaro,P.H.Damgaard;The D=1 Matrix Model and the Renormalization Group
hep-th/9206100;hep-th;0;32;;R.B.Mann;Two Dimensional Quantum Gravity Coupled to Matter
hep-ph/9206248;hep-ph;0;0;;D.Asner,R.B.Mann,J.L.Murison,T.G.Steele;Mass of Pseudoscalar Gluonium: A Higher-Loop QCD Sum-Rule Estimate
hep-lat/9206022;hep-lat;1;32;hep-lat/9107002;B.A.Berg,U.Hansmann,T.Neuhaus;Properties of Interfaces in the two and three dimensional Ising Model
hep-ph/9206249;hep-ph;0;7;;S.G.Naculich,C.-P.Yuan;Inelastic Channels in the Electroweak Symmetry-Breaking Sector
hep-ph/9206250;hep-ph;0;12;;Z.Huang,K.S.Viswanathan;Dynamical Self-mass for Massive Quarks
hep-ph/9206251;hep-ph;0;23;;Z.Huang,K.S.Viswanathan,D.D.Wu;Comments on the Vacuum Orientations in QCD
hep-ph/9206252;hep-ph;0;0;;P.E.Haagensen,J.I.Latorre;A Comprehensive Coordinate Space Renormalization of Quantum Electrodynamics to 2-Loop Order
hep-ph/9206253;hep-ph;0;0;;M.H.Friedman,Y.N.Srivastava,A.Widom;Wightman Functions in QCD
cond-mat/9206009;cond-mat;0;0;;D.M.McAvity,H.Osborn;Quantum Field Theories on Manifolds with Curved Boundaries: Scalar Fields
hep-ph/9206254;hep-ph;0;10;;S.G.Naculich,C.-P.Yuan;Can the Electroweak Symmetry-breaking Sector Be Hidden?
hep-th/9206101;hep-th;0;0;;E.Bergshoeff,E.Sezgin;Self-Dual Supergravity Theories in 2+2 Dimensions
hep-th/9206102;hep-th;0;0;;V.Periwal;Non-analyticity in the large N renormalization group
hep-ph/9206255;hep-ph;1;18;hep-ph/9204220;R.S.Chivukula,M.Golden,D.Kominis,M.V.Ramana;The Phenomenology of a Hidden Symmetry Breaking Sector
cond-mat/9206010;cond-mat;0;20;;D.Coffey,S.A.Trugman;Magnetic Properties of Undoped $C_{60}$
hep-ph/9206256;hep-ph;0;0;;D.C.Kennedy;Seesaw Neutrino Mass Ratios with Radiative Corrections
hep-th/9206103;hep-th;0;26;;S.Carlip;The Sum over Topologies in Three-Dimensional Euclidean Quantum Gravity
hep-th/9206104;hep-th;0;0;;C.S.Aulakh,V.Soni;Topological Soliton Multiplets in 4+1 Dimensional YMCS Theory
cond-mat/9206011;cond-mat;0;7;;D.Coffey,S.A.Trugman;Correlations for the S=1/2 Antiferromagnet on a Truncated Tetrahedron
hep-ph/9206257;hep-ph;0;25;;D.Pierce,A.Papadopoulos;Radiative corrections to the Higgs boson decay rate $Γ(H→ZZ)$ in the minimal supersymmetric model
hep-ph/9206258;hep-ph;0;16;;T.G.Rizzo;Probing New Gauge Boson Couplings at Hadron Supercolliders
hep-th/9206105;hep-th,gr-qc;0;14;;S.P.Braham;Generalized embedding variables for geometrodynamics and spacetime diffeomorphisms: Ultralocal coordinate conditions
hep-lat/9206023;hep-lat;0;22;;M.-P.Lombardo,G.Parisi,A.Vladikas;Lattice QCD Spectroscopy with an Improved Wilson Fermion Action
hep-ph/9206259;hep-ph;1;52;hep-th/9110037;A.Linde;Progress in the Theory of the Electroweak Phase Transition
hep-lat/9206024;hep-lat;0;0;;S.Hands,A.Kocic,J.Kogut;The Four-Fermi Model in Three Dimensions at Non-Zero Density and Temperature
hep-ph/9206260;hep-ph,astro-ph;0;0;;R.H.Brandenberger,A.-C.Davis;Electroweak Baryogenesis with a Second Order Phase Transition
hep-th/9206106;hep-th;0;27;;M.Dubois-Violette,M.Henneaux,M.Talon,CM.Viallet;General Solution of the Consistency Equation
hep-th/9206107;hep-th;5;62;hep-th/9108001,hep-th/9108004,hep-th/9109032,hep-th/9111056,hep-th/9201061;S.Chaudhuri,J.D.Lykken;String Theory, Black Holes, and SL(2,R) Current Algebra
hep-lat/9206025;hep-lat,hep-ph;0;57;;M.Göckeler,H.A.Kastrup,T.Neuhaus,F.Zimmermann;Scaling analysis of the O(4)-symmetric $Φ^4$-theory in the broken phase
hep-ph/9206261;hep-ph;0;0;;J.Bagger,S.Dawson,G.Valencia;Vector-Boson versus Gluon Fusion at Hadron Colliders
hep-th/9206108;hep-th;0;0;;E.Sezgin,K.S.Stelle;Nonlinear Realisations of $w_{1+∞}$
hep-ph/9206262;hep-ph;0;17;;B.Grzadkowski,J.F.Gunion;Using Back-Scattered Laser Beams to Detect CP Violation in the Neutral Higgs Sector
hep-th/9206109;hep-th;0;17;;F.Gieres;Maurer-Cartan forms and equations for two-dimensional superdiffeomorphisms
hep-ph/9206263;hep-ph;0;42;;H.Zhang;Magnetic Monopoles As a New Solution to Strong CP Problem
hep-th/9206110;hep-th;1;38;hep-th/9108005;T.Kawai,T.Uchino,S.-K.Yang;Higher-Rank Supersymmetric Models and Topological Field Theory
hep-th/9206111;hep-th;0;0;;S.Mahapatra,S.Mukherji,A.M.Sengupta;Target Space Interpretation of New Moduli in 2D String Theory
hep-lat/9206026;hep-lat;0;0;;A.Kocic,J.Kogut,S.Hands;The Universlity Class of Monopole Condensation in Non-Compact, Quenched Lattice QED
hep-th/9206112;hep-th,hep-lat;1;13;hep-th/9112007;G.Watts,R.Weston;G_2^1 Affine Toda Field Theory: A Numerical Test of Exact S-Matrix results
hep-ph/9206264;hep-ph,hep-lat;0;84;;R.Shrock;On the Origin of Fermion Masses
hep-ph/9206265;hep-ph;0;60;;H.Zhang;Global Quantization in Gauge Orbit Space with Magnetic Monopoles As a Solution to Strong CP Problem and the Relevance to $U_A(1)$ Problem
hep-lat/9206027;hep-lat,hep-ph;0;0;;J.E.Mandula;Numerical Analysis of the Quark Fraction of the Proton Spin
hep-ph/9206266;hep-ph,astro-ph;0;26;;S.Myint;Baryogenesis Constraints on the Minimal Supersymmetric Model
hep-th/9206113;hep-th;0;0;;I.Tsutsui,L.Feher;On the Lagrangian Realization of the WZNW Reductions
hep-th/9206114;hep-th;2;101;hep-th/9109021,hep-th/9111014;T.R.Klassen,E.Melzer;Sine-Gordon =/= Massive Thirring, and Related Heresies
hep-th/9207001;hep-th;2;17;hep-th/9211054,hep-th/0209014;T.Strobl;All Symmetries of Non-Einsteinian Gravity in $d =2$
hep-th/9207002;hep-th;1;38;hep-th/9109007;M.A.R.Osorio,M.A.Vazquez-Mozo;Duality in Non-Trivially Compactified Heterotic Strings
hep-th/9207003;hep-th;0;0;;E.Fradkin,E.Moreno,F.A.Schaposnik;Ground state wave functionals for $1+1$-dimensional fermion field theories
hep-lat/9207001;hep-lat,hep-th;3;47;hep-th/9109011,hep-th/9110002,hep-th/9111060;M.Caselle,R.Fiore,F.Gliozzi,S.Vinti;The Effective String of 3D Z_2 Gauge Theory as a c=1 compactified CFT
hep-ph/9207201;hep-ph;0;92;;P.Langacker;Particle Physics Summary, Where are We and Where are We Going?
hep-ph/9207202;hep-ph,gr-qc,hep-th;0;22;;H.La;Dilatonic Domain Walls
hep-ph/9207203;hep-ph;0;41;;K.Aoki,S.Peris;Non--decoupling, triviality and the $ρ$ parameter
hep-th/9207004;hep-th;3;42;hep-th/9108004,hep-th/9111048,hep-th/9204085;B.Gato-Rivera,A.M.Semikhatov;d≤1\bigcup d≥25$ and Constrained KP Hierarchy from BRST Invariance in the $c≠3$ Topological Algebra
hep-ph/9207204;hep-ph;0;0;;J.Cleymans,H.Satz;Thermal Hadron Production in High Energy Heavy Ion Collisions
cond-mat/9207001;cond-mat,hep-lat;0;0;;V.Privman;Exact Results for a Three-Body Reaction-Diffusion System
hep-th/9207005;hep-th;0;33;;J.Isberg,U.Lindström,B.Sundborg;Space-Time Symmetries of Quantized Tensionless Strings
hep-th/9207006;hep-th;0;18;;A.Mikovic;Exactly Solvable Models of 2d Dilaton Quantum Gravity
cond-mat/9207002;cond-mat,hep-lat;0;0;;V.Privman;Model of Cluster Growth and Phase Separation: Exact Results in One Dimension
cond-mat/9207003;cond-mat,astro-ph,hep-lat;0;0;;V.Privman;Fluctuating Interfaces, Surface Tension, and Capillary Waves: An Introduction
hep-ph/9207205;hep-ph;0;28;;V.Barger,K.Cheung,R.J.N.Phillips,A.L.Stange;What $e^+e^-$ collider could make a ``no-lose'' search for MSSM Higgs bosons?
hep-ph/9207206;hep-ph;0;0;;W.Kwong,S.P.Rosen;Nonet Symmetry and Two-Body Decays of Charmed Mesons
hep-ph/9207207;hep-ph;0;0;;C.P.Burgess,J.M.Cline;Majorons from Double Beta Decay
hep-ph/9207208;hep-ph,astro-ph,hep-th;0;0;;R.Holman,T.W.Kephart,S.-J.REY;Semiclassical Gravity and Invisible Axions
hep-th/9207007;hep-th;0;0;;F.H.L.Essler,V.E.Korepin;A New Solution of the Supersymmetric TJ Model by Means of the Quantum Inverse Scattering Method
hep-lat/9207002;hep-lat;0;34;;K.Yee;Gauge Dependence of Effective Quark Mass and Matrix Elements in Gaugefixed Large $N$ Strong Coupling Lattice QCD
hep-th/9207008;hep-th;0;29;;A.Blasi,N.Maggiore;Infrared and Ultraviolet Finiteness of Topological BF Theory in Two Dimensions
cond-mat/9207004;cond-mat;0;0;;V.Privman,M.Barma;Random Sequential Adsorption on a Line: Mean-Field Theory of Diffusional Relaxation
hep-th/9207009;hep-th;2;72;hep-th/9201008,hep-th/9202058;K.Ito,J.O.Madsen,J.L.Petersen;Free Field Representations of Extended Superconformal Algebras
hep-th/9207010;hep-th;2;43;hep-th/9201008,hep-th/9202058;K.Ito,J.O.Madsen,J.L.Petersen;Free Field Representations and Screening Operators for the $N=4$ Doubly Extended Superconformal Algebras
hep-ph/9207209;hep-ph;0;0;;Z.Berezhiani,A.Y.Smirnov,J.W.F.Valle;Observable Majoron Emission in Neutrinoless Double Beta Decay
hep-ph/9207210;hep-ph;0;0;;W.R.Greenberg,G.A.Miller;Multiple-Scattering Series For Color Transparency
hep-ph/9207211;hep-ph;0;0;;B.K.Jennings,G.A.Miller;Realistic Hadronic Matrix Element Approach to Color Transparency
hep-lat/9207003;hep-lat;1;39;hep-lat/9204016;M.Grabenstein,K.Pinn;Kinematics of Multigrid Monte Carlo
hep-th/9207011;hep-th;3;31;hep-th/9111021,hep-th/9111028,hep-th/9112052;A.Dhar,G.Mandal,S.R.Wadia;Non-relativistic Fermions, Coadjoint Orbits of \winf  and String Field Theory at $c=1$
hep-th/9207012;hep-th;1;22;hep-th/9206059;W.A.Sabra;Classical Hamiltonian Reduction and Superconformal Algebras
hep-ph/9207212;hep-ph;0;52;;V.Barger,K.Cheung,R.J.N.Phillips,A.L.Stange;Collider discovery limits for supersymmetric Higgs bosons
hep-th/9207013;hep-th;0;0;;J.M.Figueroa-O'Farrill,J.Mas,E.Ramos;On the two-boson picture of the KP hierarchy
hep-ph/9207213;hep-ph,astro-ph;0;39;;S.A.Bludman,N.Hata,D.C.Kennedy,P.G.Langacker;Implication of Combined Solar Neutrino Observation and their Theoretical Uncertainties
hep-ph/9207214;hep-ph;0;19;;I.I.Bigi,N.G.Uraltsev,A.I.Vainshtein;Nonperturbative Corrections to Inclusive Beauty and Charm Decays: QCD versus Phenomenological Models
hep-lat/9207004;hep-lat;0;25;;M.F.L.Golterman,D.N.Petcher;Fermions in Models with Wilson--Yukawa Couplings
hep-lat/9207005;hep-lat;0;24;;M.F.L.Golterman,D.N.Petcher,E.Rivas;On the Eichten--Preskill Proposal for Lattice Chiral Gauge Theories
cond-mat/9207005;cond-mat;0;7;;K.Olaussen;On the Harmonic Oscillator Regularization of Partition Functions
hep-ph/9207215;hep-ph;0;18;;R.E.Cutkosky;Isospin Splitting in the Baryon Octet and Decuplet
hep-th/9207014;hep-th,hep-lat;0;16;;Z.Yang;A Note on ``Anomalous" Chiral Gauge Theories
hep-ph/9207216;hep-ph;0;37;;M.Cvetič,P.Langacker;$V'Z$ and $V'W$ Production as Tests of Heavy Gauge Boson Couplings at Future Hadron Colliders
cond-mat/9207006;cond-mat;0;30;;P.A.Slotte;Phase Diagram of a Lattice Microemulsion Model in Two Dimensions
hep-th/9207015;hep-th;0;16;;N.J.MacKay;The full set of $c_n$-invariant factorized $S$-matrices
cond-mat/9207007;cond-mat;0;19;;F.Guinea,M.Ueda;Low voltage conductance of small tunnel junctions
hep-lat/9207006;hep-lat;0;12;;A.Hasenfratz,K.Jansen,Y.Shen;The Phase Diagram of a U(1) Higgs-Yukawa Model at Finite $λ$
hep-th/9207016;hep-th;6;75;hep-th/9109026,hep-th/9109038,hep-th/9109048,hep-th/9110004,hep-th/9110053,hep-th/9112044;J.Maharana,J.H.Schwarz;Noncompact Symmetries in String Theory
hep-ph/9207217;hep-ph;0;0;;B.Blok,M.Shifman;The Isgur-Wise Function in Small Velocity Limit
hep-th/9207017;hep-th,hep-ph;0;0;;Y.Frishman,J.Sonnenschein;Bosonization and QCD in Two Dimensions
hep-ph/9207218;hep-ph;0;0;;S.P.Martin;Some Simple Criteria for Gauged R-parity
cond-mat/9207008;cond-mat;0;58;;Y.-H.Li,S.Teitel;Vortex Line Fluctuations in Model High Temperature Superconductors
hep-ph/9207219;hep-ph;0;51;;J.Lopez,D.Nanopoulos,A.Zichichi;Troubles with the Minimal SU(5) Supergravity Model
hep-th/9207018;hep-th;0;42;;A.Gualzetti,S.Penati,D.Zanon;Quantum Conserved Currents in Supersymmetric Toda Theories
hep-ph/9207220;hep-ph;0;20;;T.Ohl;KROWIG Version 1.0: Interfacing KRONOS and HERWIG or Higher Order Electromagnetic Radiative Corrections at HERA with Hadronic Final States
hep-ph/9207221;hep-ph;0;47;;H.Dreiner,G.G.Ross;Sphaleron Erasure of Primordial Baryogenesis
hep-lat/9207007;hep-lat;0;0;;U.Hansmann,B.A.Berg,T.Neuhaus;Recent Results of Multimagnetical Simulations of the Ising Model
hep-th/9207019;hep-th;0;0;;M.Flohr;W-Algebras, New Rational Models and Completeness of the c = 1 Classification
hep-lat/9207008;hep-lat,hep-th;0;46;;J.Ambjorn,Irback,J.Jurkiewicz,B.Petersson;The Theory of Dynamical Random Surfaces with Extrinsic Curvature
cond-mat/9207009;cond-mat;0;19;;M.C.Marchetti;Modification of the Magnetic Flux-Line Interaction at a Superconductor's Surface
hep-th/9207020;hep-th;2;11;hep-th/9201033,hep-th/9202006;J.Ambjorn,C.F.Kristjansen,Y.M.Makeenko;Higher Genus Correlators for the Complex Matrix Model
hep-th/9207021;hep-th;0;20;;I.Pesando;Polymers and Topological Field Theory: A 2 Loop Computation
hep-th/9207022;hep-th;0;44;;G.von Gehlen;Phase diagram and two-particle structure of the $Z_3$-chiral Potts model
hep-ph/9207222;hep-ph;0;0;;M.Lu,M.B.Wise,M.J.Savage;Two Photon Contribution to Polarization in $K^+ →π^+ μ^+ μ^-$
hep-ph/9207223;hep-ph;0;0;;J.M.Flynn,N.Isgur;Heavy quark symmetry: ideas and applications
hep-th/9207023;hep-th;0;59;;M.Gunaydin;On the Chiral Rings in N=2 and N=4 Superconformal Algebras
hep-ph/9207224;hep-ph;0;34;;M.Leurer;On the Unmixed 17 keV Neutrino
hep-ph/9207225;hep-ph;0;37;;Y.Nir,U.Sarid;Testing the Standard Model and Schemes for Quark Mass Matrices with CP Asymmetries in B Decays
hep-lat/9207009;hep-lat;0;0;;M.Lüscher,R.Narayanan,P.Weisz,U.Wolff;The Schrödinger Functional - a Renormalizable Probe for Non-Abelian Gauge Theories
hep-lat/9207010;hep-lat;0;0;;M.Lüscher,P.Weisz,R.Sommer,U.Wolff;Computation of the Running Coupling in the SU(2) Yang-Mills Theory
hep-th/9207024;hep-th;2;23;hep-th/9204005,hep-th/9205075;N.Marcus;The N=2 open string
hep-th/9207025;hep-th;1;28;hep-th/9109056;H.W.Braden,H.S.Cho,J.D.Kim,I.G.Koh,R.Sasaki;Singularity analysis in $A_n$ Affine Toda Theories
hep-th/9207026;hep-th;0;0;;M.Karowski,R.Schrader,FU-Berlin;A quantum group version of quantum gauge theories in two dimensions
hep-th/9207027;hep-th;0;9;;F.Delduc,J.-L.Gervais,M.Saveliev;Supersymmetric Black Holes from Toda Theories
hep-th/9207028;hep-th;1;25;hep-th/9201042;J.Greensite;Vanishing of the Cosmological Constant in Stabilized Quantum Gravity
hep-ph/9207226;hep-ph;0;23;;T.Appelquist,G.Triantaphyllou;Technicolor Enhancement of $t \bar t$ Production at TeV-Colliders
cond-mat/9207010;cond-mat;0;33;;O.Biham,M.Kvale;Unstable Periodic Orbits in the Stadium Billiard
hep-lat/9207011;hep-lat,cond-mat,q-bio.QM;0;16;;P.Pliszka,E.Marinari;On Heteropolymer Shape Dynamics
hep-ph/9207227;hep-ph;0;0;;M.Pietroni;The Electroweak Phase Transition in a Nonminimal Supersymmetric Model
hep-th/9207029;hep-th;0;0;;T.A.Larsson;Conformal fields: a class of representations of Vect(N)
hep-ph/9207228;hep-ph;0;28;;A.C.Mattingly,P.M.Stevenson;QCD Perturbation Theory at Low Energies
hep-ph/9207229;hep-ph;0;0;;J.L.Hewett,T.G.Rizzo;The Effects of Detector Descoping and Neutral Boson Mixing on New Gauge Boson Physics at the SSC
hep-th/9207030;hep-th;0;0;;T.A.Larsson;Vect(N) conformal fields and their exterior derivatives
hep-ph/9207230;hep-ph;1;6;hep-ph/9204232;A.Kusenko;Invariants Describing Quark Mixing and Mass Matrices
hep-th/9207031;hep-th;1;34;hep-th/9109042;M.D.Freeman,K.Hornfeck,P.West;Commuting quantities and exceptional W-algebras
hep-th/9207032;hep-th;0;0;;A.Ch.Ganchev,V.B.Petkova;Reduction of the Knizhnik-Zamolodchikov Equation - a Way of Producing Virasoro Algebra Singular Vectors
hep-ph/9207231;hep-ph;0;0;;P.L.White;Discrete Symmetries from Broken $SU(N)$ and the MSSM
hep-th/9207033;hep-th;0;0;;S.Massar,R.Parentani,R.Brout;On the Problem of the Uniformly Accelerated Oscillator
cond-mat/9207011;cond-mat;0;17;;H.-wen.Xi,J.Vinals,J.D.Gunton;Numerical study of pattern formation following a convective instability in non-Boussinesq fluids
hep-ph/9207232;hep-ph;0;28;;Z.Kunszt,Z.Trócsányi;QCD Corrections to Photon Production in Association with Hadrons in $e^+e^-$ Annihilation
hep-ph/9207233;hep-ph;0;14;;M.J.Savage,M.Luke,M.B.Wise;The Rare Decays $\piee $, $\etaee $ and \etamumu $ in Chiral Perturbation Theory
cond-mat/9207012;cond-mat;0;38;;M.Jarrell,T.Pruschke;Magnetic and Dynamic Properties of the Hubbard Model in Infinite Dimensions
math/9207201;math.CV;0;0;;M.Abate,G.Patrizio;Holomorphic curvature of Finsler metrics and complex geodesics
math/9207202;math.CV;0;0;;E.A.Poletsky;Sequences of analytic disks
hep-ph/9207234;hep-ph;0;95;;M.Drees,M.M.Nojiri;The Neutralino Relic Density in Minimal N=1 Supergravity
hep-th/9207034;hep-th;0;30;;S.B.Giddings,A.Strominger;Quantum Theories of Dilaton Gravity
hep-ph/9207235;hep-ph;0;31;;J.F.Amundson,J.L.Rosner,M.A.Kelly,N.Horowitz,S.L.Stone;Meson Decay Constants from Isospin Mass Splittings in the Quark Model
hep-th/9207035;hep-th;0;22;;E.S.Fradkin,V.Ya.Linetsky;Classification of Superconformal Algebras with Quadratic Non-Linearity
hep-th/9207036;hep-th;0;0;;J.Govaerts;Finite Euler Hierarchies And Integrable Universal Equations
hep-th/9207037;hep-th,gr-qc,hep-ph;0;33;;S.M.Carroll,E.Farhi,A.H.Guth;Gott Time Machines Cannot Exist in an Open (2+1)-Dimensional Universe With Timelike Total Momentum
hep-th/9207038;hep-th;0;0;;Y.Shamir;Compensating Fields and Anomalies in Supergravity
hep-th/9207039;hep-th;0;0;;G.Ferretti,S.G.Rajeev;Current Algebra in Three Dimensions
hep-th/9207040;hep-th;4;31;hep-th/9110058,hep-th/9111014,hep-th/9201032,hep-th/9202020;F.Ravanini,R.Tateo,A.Valleriani;Dynkin TBA's
hep-th/9207041;hep-th,math.QA;0;21;;J.C.Baez;Link Invariants of Finite Type and Perturbation Theory
hep-th/9207042;hep-th;0;0;;S.V.Ketov,H.Nishino,S.J.Gates Jr;Self-Dual Supersymmetry and Supergravity in Atiyah-Ward Space-Time
hep-th/9207043;hep-th;0;0;;W.Siegel;Self-Dual N=8 Supergravity as Closed N=2(4) Strings
astro-ph/9207001;astro-ph,hep-ph;0;24;;R.L.Davis,H.M.Hodges,G.F.Smoot,P.J.Steinhardt,M.S.Turner;Cosmic Microwave Background Probes Models of Inflation
hep-th/9207044;hep-th,cond-mat;0;10;;W.Chen,M.Li;Operator content and modular property of Chern-Simons coupled to a massless scalar
astro-ph/9207002;astro-ph,hep-ph;0;14;;R.Crittenden,P.J.Steinhardt;Graceful Exit in Extended Inflation and Implications for Density Perturbations
hep-th/9207045;hep-th,hep-ph;0;47;;M.Dine;Problems of Naturalness: Some Lessons from String Theory
hep-ph/9207236;hep-ph;0;0;;B.Blok,M.Shifman;The Rule of Discarding $1/N_c$ in Inclusive Weak Decays
hep-th/9207046;hep-th;1;39;hep-th/9111056;E.Elizalde,S.D.Odintsov;One-Loop Renormalization in Two-Dimensional Matter-Dilaton Quantum Gravity and Charged Black Holes
cond-mat/9207013;cond-mat;1;2;cond-mat/9206007;A.Moroz;The Majorana Fermions for Quantum S=1/2 Antiferromagnet?
hep-ph/9207237;hep-ph;1;52;hep-ph/9203220;J.Ellis,J.Lopez,D.Nanopoulos;The prospects for CHORUS and NOMAD in the light of COBE and GALLEX
hep-ph/9207238;hep-ph,hep-th;0;27;;A.Zhitnitsky;Quark confinement , topological susceptibility and all that in 4 dimensional gluodynamics
hep-th/9207047;hep-th;0;16;;A.P.Polychronakos,R.Tzani;Schrodinger Equation for Particle with Friction
hep-th/9207048;hep-th;3;48;hep-th/9108004,hep-th/9109032,hep-th/9111028;E.Nissimov,S.Pacheva;$\bf W_∞$ Gravity - a Geometric Approach
hep-ph/9207239;hep-ph,astro-ph;0;39;;M.White;Contribution of Long Wavelength Gravitational Waves to the CMB Anisotropy
hep-th/9207049;hep-th;0;40;;J.Erler,D.Jungnickel,M.Spalinski,S.Stieberger;Higher Twisted Sector Couplings of $Z_N$ Orbifolds
hep-th/9207050;hep-th;1;28;hep-th/9203051;F.Delduc,A.Galperin,P.Howe,E.Sokatchev;A twistor formulation of the heterotic D=10 superstring with manifest (8,0) worldsheet supersymmetry
hep-th/9207051;hep-th;0;18;;B.Sathiapalan;Loop Variables and the Virasoro Group
hep-th/9207052;hep-th;0;17;;O.F.Dayi;Solution of the Master Equation in Terms of the Odd Time Formulation
hep-ph/9207240;hep-ph;0;15;;L.Clavelli,P.W.Coulter,B.Fenyi,C.Hester,P.Povinec,K.Yuan;Squarks Below the Z
hep-th/9207053;hep-th;0;0;;A.Sen;Electric Magnetic Duality in String Theory
cond-mat/9207014;cond-mat;0;0;;B.D.Lubachevsky,V.Privman,S.C.Roy;Morphology of Amorphous Layers Ballistically Deposited on a Planar Substrate
hep-lat/9207012;hep-lat;0;24;;M.Goeckeler,G.Schierholz;A Proposal for Simulating Chiral Fermions
hep-lat/9207013;hep-lat;0;37;;N.Schultka,M.Müller-Preussker;The Topological Susceptibility of the Lattice CP(n-1) Model on the Torus and the Sphere
cond-mat/9207015;cond-mat;0;0;;V.Privman,M.D.Grynberg;Fast-diffusion mean-field theory for k-body reactions in one dimension
cond-mat/9207016;cond-mat;0;16;;M.Troyer,D.Würtz;Ferromagnetism of the 1-D Kondo Lattice Model: A Quantum Monte Carlo Study
hep-th/9207054;hep-th,gr-qc;0;18;;D.G.Boulware;Quantum Field Theory in Spaces with Closed Time-Like Curves
hep-ph/9207241;hep-ph;0;21;;R.Ibanez-Meier,P.M.Stevenson;Autonomous Renormalization of the One-Loop Effective Potential and a 2 Tev Higgs in SU(2)xU(1)
hep-th/9207055;hep-th;0;20;;N.Dorey,P.S.Kurzepa;Vortex condensation in a model of random $φ^4$-graphs
cond-mat/9207017;cond-mat;0;40;;R.J.Troy,A.T.Dorsey;Transport Properties and Fluctuations in Type II Superconductors Near $H_{c2}$
hep-ph/9207242;hep-ph,hep-th;0;8;;J.-R.Cudell,K.R.Dienes;Are There Oscillations in the Baryon/Meson Ratio?
cond-mat/9207018;cond-mat;0;0;;A.T.Dorsey;Vortex motion and the Hall effect in type II superconductors: a time dependent Ginzburg-Landau theory approach
hep-ph/9207243;hep-ph,astro-ph;0;34;;L.M.Krauss;COBE, Inflation, and Light Scalars
hep-th/9207056;hep-th,gr-qc;0;26;;L.N.Chang,C.Soo;Einstein manifolds in Ashtekar variables: explicit examples
hep-th/9207057;hep-th;0;0;;P.Majumdar;Inonu-Wigner Contractions of Kac-Moody Algebras
hep-lat/9207014;hep-lat;0;7;;W.Wilcox;Lattice Charge Overlap: Towards the Elastic Limit
hep-th/9207058;hep-th;0;0;;S.Panda,S.Roy;Remarks on the Additional Symmetries and W-Constraints in the Generalized KdV Hierarchy
hep-th/9207059;hep-th;0;8;;A.Carlini,A.Treves,F.Fucito,M.Martellini;The vacuum polarization around an axionic stringy black hole
hep-th/9207060;hep-th;0;0;;M.J.Duff,J.X.Lu;Type II p-branes: the brane-scan revisited
hep-lat/9207015;hep-lat,hep-th;0;8;;A.A.Migdal;1/N Expansion and Particle Spectrum in Induced QCD
hep-th/9207061;hep-th;1;27;hep-th/9110032;C.P.Constantinidis,L.A.Ferreira,J.F.Gomes,A.H.Zimerman;Connection between the Affine and Conformal Affine Toda Models and their Hirota's Solution
hep-th/9207062;hep-th;0;0;;J.R.Bienkowska,H.Lu;A Note on N=2 Superstrings
hep-ph/9207244;hep-ph,astro-ph;0;0;;D.P.Bennett,S.H.Rhie;COBE's Constraints on the Global Monopole and Texture Theories of Cosmic Structure Formation
hep-ph/9207245;hep-ph,astro-ph;0;0;;F.Adams,J.R.Bond,K.Freese,J.Frieman,A.Olinto;Natural Inflation: Particle Physics Models, Power Law Spectra for Large Scale Structure, and Constraints from COBE
cond-mat/9207019;cond-mat;0;16;;C.Ting;Duality in Multi-layered Quantum Hall Systems
cond-mat/9207020;cond-mat;0;29;;C.Ting;Mutual statistics, braid group, and the fractional quantum Hall effect
hep-lat/9207016;hep-lat;0;25;;T.Kalkreuter;Improving Multigrid and Conventional Relaxation Algorithms for Propagators
cond-mat/9207021;cond-mat;0;18;;S.K.Yip,J.A.Sauls;Nonlinear Meissner Effect in CuO Superconductors
hep-lat/9207017;hep-lat;0;18;;A.Hasenfratz,P.Hasenfratz;The equivalence of the SU(N) Yang Mills Theory with a Purely Fermionic Model
hep-lat/9207018;hep-lat;0;28;;S.Aoki;Fermion Interactions in the Wilson Yukawa Approach for Lattice Chiral Gauge Theories
hep-lat/9207019;hep-lat,cond-mat;0;12;;M.Hasenbusch,M.Marcu,K.Pinn;High Precision Verification of the Kosterlitz Thouless Scenario
cond-mat/9207022;cond-mat,hep-lat;0;21;;M.Hasenbusch,G.Lana,M.Marcu,K.Pinn;Cluster Algorithm for a Solid-On-Solid Model with Constraints
hep-ph/9207246;hep-ph,hep-th;0;20;;I.J.R.Aitchison,N.Dorey,M.Klein-Kreisler,N.E.Mavromatos;Phase Structure of QED3 at Finite Temperature
hep-th/9207063;hep-th;6;28;hep-th/9108004,hep-th/9109032,hep-th/9111021,hep-th/9111028,hep-th/9201005,hep-th/9201056;N.Sakai,Y.Tanii;Physical Degrees of Freedom in 2-D String Field Theories
hep-ph/9207247;hep-ph;0;19;;R.K.Schaefer,Q.Shafi;Inflation and Large Scale Structure Formation After COBE
cond-mat/9207023;cond-mat;0;20;;O.H.Nielsen,J.P.Sethna,P.Stoltze,K.W.Jacobsen,J.K.Norskov;Melting a copper cluster: Critical droplet theory
hep-th/9207064;hep-th;0;29;;D.Kutasov;Irreversibility of the Renormalization Group Flow in Two Dimensional Quantum Gravity
hep-ph/9207248;hep-ph;0;18;;A.Datta;Flavour Democracy Calls for the Fourth Generation
hep-lat/9207020;hep-lat;0;20;;J.Ambjorn,K.Farakos;Topography of the hot sphaleron Transitions
hep-th/9207065;hep-th;1;29;hep-th/9203019;S.Dalley,I.Klebanov;Light-Cone Quantization of the c=2 Matrix Model
hep-th/9207066;hep-th;0;18;;G.Papadopoulos,B.Spence;The Global Phase Space Structure of the Wess-Zumino-Witten Model
cond-mat/9207024;cond-mat;0;0;;S.Hershfield,J.H.Davies,P.Hyldgaard,C.J.Stanton,J.W.Wilkins;Zero Frequency Current Noise for the Double Tunnel Junction Coulomb Blockade
gr-qc/9207001;gr-qc;0;10;;R.Capovilla;Non-Minimally Coupled Scalar Field and Ashtekar Variables
hep-ph/9207249;hep-ph,hep-lat;0;35;;R.S.Chivukula,M.Dugan,M.Golden;Electroweak Corrections in Technicolor Reconsidered
hep-ph/9207250;hep-ph;0;27;;A.Zhitnitsky;Once more on $θ$-vacua in $2+1$ dimensional QED and 3+1 dimensional gluodynamics
hep-lat/9207021;hep-lat;2;27;hep-lat/9206008,hep-lat/9206013;C.Frick,L.Lin,I.Montvay,G.Munster,M.Plagge,T.Trappenberg,H.Wittig;Numerical simulation of heavy fermions in an SU(2)_L x SU(2)_R symmetric Yukawa model
hep-lat/9207022;hep-lat;0;25;;C.F.Baillie,D.A.Johnston;Crossover Between Weakly and Strongly Self-avoiding Random Surfaces
hep-ph/9207251;hep-ph;0;37;;T.Barnes,E.S.Swanson,J.Weinstein;I=3/2 $K π$ Scattering in the Nonrelativisitic Quark Potential Model
hep-lat/9207023;hep-lat,cond-mat;1;25;hep-lat/9202004;B.A.Berg,T.Celik;Multicanonical Spin Glass Simulations
hep-th/9207067;hep-th;0;0;;M.Bershadsky,W.Lerche,D.Nemeschansky,N.P.Warner;A BRST Operator for non-critical W-Strings
hep-th/9207068;hep-th;0;0;;J.Govaerts;A Quantum Anomaly For Rigid Particles
hep-ph/9207252;hep-ph;0;11;;B.Kastening;Renormalization Group Improvement of the Effective Potential in Massive O(N) Symmetric $φ^4$ Theory
hep-th/9207069;hep-th;1;17;hep-th/9202020;F.Ravanini,R.Tateo,A.Valleriani;A New Family of Diagonal Ade-Related Scattering Theories
hep-th/9207070;hep-th,gr-qc;2;20;hep-th/9111045,hep-th/9112008;D.Kastor,J.Traschen;Horizons Inside Classical Lumps
gr-qc/9207002;gr-qc;0;16;;R.Capovilla,T.Jacobson;Remarks on Pure Spin Connection Formulations of Gravity
hep-th/9207071;hep-th;0;58;;M.B.Halpern,N.A.Obers;Ward Identities for Affine-Virasoro Correlators
hep-th/9207072;hep-th,gr-qc;0;0;;R.Blumenhagen,W.Eholzer,A.Honecker,R.Huebel;New N=1 Extended Superconformal Algebras with Two and Three Generators
hep-th/9207073;hep-th;0;0;;J.M.Evans,T.J.Hollowood;Integrable N=2 Supersymmetric Field Theories
hep-ph/9207253;hep-ph;0;38;;S.Kelley,J.Lopez,D.Nanopoulos,H.Pois,K.Yuan;New Constraints on Neutralino Dark Matter in the Supersymmetric Standard Model
hep-th/9207074;hep-th,hep-ph;0;45;;S.G.Naculich;Quantum Kinks: Solitons at Strong Coupling
hep-th/9207075;hep-th,math.QA;0;10;;D.Chang,I.Phillips,L.Rozansky;R-matrix Approach to Quantum Superalgebras su_q(m|n)
hep-ph/9207254;hep-ph;0;13;;L.Clavelli,P.H.Cox,K.Yuan;Supersymmetry and Tau Decay
hep-lat/9207024;hep-lat,hep-ph;0;0;;U.M.Heller,H.Neuberger,P.Vranas;Large $N$ analysis of the Higgs mass triviality bound
hep-lat/9207025;hep-lat;0;0;;C.Bernard,M.C.Ogilvie,T.A.DeGrand,C.DeTar,S.Gottlieb,A.Krasnitz,R.L.Sugar,D.Toussaint;QCD thermodynamics with two flavors of Wilson quarks at N_t=6
gr-qc/9207003;gr-qc;0;48;;T.Damour,S.Deser,J.McCarthy;Nonsymmetric Gravity Theories: Inconsistencies and a Cure
hep-th/9207076;hep-th;0;0;;H.D.Politzer;Simple Quantum Systems in Spacetimes with Closed Timelike Curves
hep-th/9207077;hep-th;0;16;;S.Nojiri,I.Oda;Semi-classical Approach to Charged Dilatonic Black Hole in Two Dimensions
hep-lat/9207026;hep-lat,astro-ph,cond-mat;1;13;hep-lat/9202004;B.Grossmann,M.L.Laursen,T.Trappenberg,U.-J.Wiese;A Multicanonical Algorithm and the Surface Free Energy in SU(3) Pure Gauge Theory
gr-qc/9207004;gr-qc,hep-th;0;0;;D.Cangemi;One Formulation for both Lineal Gravities through a Dimensional Reduction
hep-th/9207078;hep-th;5;34;hep-th/9108004,hep-th/9108027,hep-th/9109032,hep-th/9201005,hep-th/9201071;H.Kanno,M.H.Sarmadi;BRST cohomology ring in 2D gravity coupled to minimal models
gr-qc/9207005;gr-qc;0;11;;T.Jacobson,J.D.Romano;Degenerate Extensions of General Relativity
gr-qc/9207006;gr-qc;0;15;;T.Jacobson,J.D.Romano;The Spin Holonomy Group In General Relativity
hep-ph/9207255;hep-ph;0;16;;L.Perivolaropoulos;Large Scale Structure by Global Monopoles and Cold Dark Matter
alg-geom/9207001;alg-geom,math.AG;0;25;;R.Hain;Completions of mapping class groups and the cycle $C - C^-$
hep-ph/9207256;hep-ph;0;9;;L.Perivolaropoulos;Nontopological Global Field Dynamics
hep-ph/9207257;hep-ph;0;30;;V.Barger,R.J.N.Phillips,K.Whisnant;Long-Wavelength Oscillations and the Gallex Solar Neutrino Signal
cond-mat/9207025;cond-mat,hep-th;0;11;;D.Senechal;Chern-Simons superconductivity
hep-th/9207079;hep-th;0;7;;P.H.Cox,B.Harms,Y.Leblanc;Dilatonic Black Holes, Naked Singularities and Strings
hep-th/9207080;hep-th;0;0;;T.Kimura;Generalized Classical BRST Cohomology and Reduction of Poisson Manifolds
hep-th/9207081;hep-th;0;0;;K.Takasaki,T.Takebe;Quasi-classical limit of KP hierarchy, W-symmetries and free fermions
cond-mat/9207026;cond-mat;0;32;;H.Frahm,A.Schadschneider;Critical exponents of the degenerate Hubbard model
hep-lat/9207027;hep-lat;0;0;;V.Azcoiti,G.D.Carlo,A.F.Grillo;A new approach to noncompact lattice qed with light fermions
hep-ph/9207258;hep-ph;0;0;;J.-M.F.J.M.M.M.T.J.Orloff;LEP1 vs. Future Colliders: Effective Operators And Extended Gauge Group
hep-th/9207082;hep-th,hep-ph;0;23;;P.A.Griffin;The sine-Gordon model and the small k^+ region of light-cone perturbation theory
hep-th/9207083;hep-th,hep-lat;1;41;hep-th/9108009;P.A.Griffin;Staggered fermions and chiral symmetry breaking in transverse lattice regulated QED
hep-ph/9207259;hep-ph;0;0;;R.L.Jaffe;Spin Structure Functions
gr-qc/9207007;gr-qc,astro-ph;0;0;;N.J.Cornish,J.W.Moffat;Comments on Theoretical Problems in Nonsymmetric Gravitational Theory
math/9207203;math.LO;0;25;;T.Bartoszynski,W.Just,M.Scheepers;Covering games and the Banach-Mazur game: k-tactics
hep-lat/9207028;hep-lat,hep-th;0;13;;J.Nishimura;Monte Carlo Calculation of Phase Shift in Four Dimensional O(4) $φ^4$ Theory
hep-th/9207084;hep-th,math.QA;1;28;hep-th/9201016;P.Aschieri,L.Castellani;An introduction to non-commutative differential geometry on quantum groups
hep-th/9207085;hep-th;0;9;;A.Babichenko,S.Elitzur;Deviations from Scale Invariance near a General Conformal Background
hep-ph/9207260;hep-ph,hep-th;0;27;;H.Hata,I.Niigata;Color Confinement, Abelian Gauge and Renormalization Group Flow
hep-th/9207086;hep-th,hep-lat;0;8;;M.Caselle,A.D'Adda,S.Panzeri;Exact solution of d=1 Kazakov-Migdal induced gauge theory
hep-th/9207087;hep-th;0;20;;M.Fabbrichesi,R.Iengo;The Gravitational Field of String Matter When the Dilaton is Massive
hep-lat/9207029;hep-lat,hep-th;0;0;;P.van Baal;Topology of the Yang-Mills Configuration space
hep-th/9207088;hep-th;0;0;;A.Ruffing,T.Deck,M.Schlichenmaier;String branchings and complex tori and algebraic representations of generalized Krichever-Novikov algebras
cond-mat/9207027;cond-mat;0;53;;D.S.Fisher,A.A.Middleton;Critical Behavior of Charge Density Waves Below Threshold: Numerical and Scaling Analysis
hep-th/9207089;hep-th;0;39;;V.Ogievetsky,F.Gursey,M.Evans;From 2D conformal to 4D self-dual theories: quaternionic analyticity
hep-ph/9207261;hep-ph;0;0;;P.Gondolo;Indirect detection of unstable heavy dark matter
hep-ph/9207262;hep-ph;0;17;;C.Escobar,O.L.G.Peres,V.Pleitez,R.Z.Funchal;Comment on $τ$ decay puzzle
hep-ph/9207263;hep-ph;0;17;;C.Escobar,O.L.G.Peres,V.Pleitez,R.Z.Funchal;Three generations mixing and the $τ$ decay puzzle
hep-ph/9207264;hep-ph;1;2;hep-ph/9206242;R.Foot,O.F.Hernandez,F.Pisano,V.Pleitez;Leptons masses in an $SU(3)_L⊗U(1)_N$ Gauge Model
gr-qc/9207008;gr-qc;1;17;hep-th/9112065;A.Lahiri;The No-Hair Theorem for the Abelian Higgs Model
hep-ph/9207265;hep-ph;0;0;;J.C.Collins;Hard Scattering in QCD with Polarized Beams
gr-qc/9207009;gr-qc;0;15;;J.W.Moffat,D.C.Tatarski;Gravitational Waves from an Axi-symmetric Source in the Nonsymmetric Grav. Theory
hep-lat/9207030;hep-lat;0;31;;D.Kusnezov,J.Sloan;Global Demons in Field Theory : Critical Slowing Down in the Xy Model
hep-th/9207090;hep-th,math.QA;0;7;;T.Deguchi,T.Ohtsuki;Invariants of Colored Links and a Property of the Clebsch-Gordan Coefficients of $U_q(g)$
hep-ph/9207266;hep-ph,hep-th;0;0;;C.S.Lam;Navigating Around the Algebraic Jungle of QCD: Efficient Evaluation of Loop Helicity Amplitudes
hep-th/9207091;hep-th;0;12;;B.de Wit,A.V.Proeyen;Broken sigma-model isometries in very special geometry
hep-th/9207092;hep-th;0;0;;J.M.Figueroa-O'Farrill,J.Mas,E.Ramos;A One-Parameter Family of Hamiltonian Structures for the KP Hierarchy and a Continuous Deformation of the Nonlinear $\W _{\rm KP}$ Algebra
gr-qc/9207010;gr-qc;0;31;;İ.Semiz;The Dirac Equation Is Separable On The Dyon Black Hole Metric
hep-th/9207093;hep-th;0;0;;T.J.Allen;Collective Coordinate Action for Charged Sigma-Model Vortices in Finite Geometries
hep-th/9207094;hep-th;0;35;;E.Witten;Chern-Simons Gauge Theory As A String Theory
hep-ph/9207267;hep-ph;0;0;;H.E.Haber,A.Pomarol;Constraints from Global Symmetries on Radiative Corrections to the Higgs Sector
hep-th/9207095;hep-th,gr-qc;1;36;hep-th/9205069;S.P.de Alwis;Quantum Black Holes in Two Dimensions
hep-lat/9207031;hep-lat;0;22;;S.Staniford-Chen;Finite Size Scaling of Probability Distributions in SU(2) Lattice Gauge Theory and Phi^4 Field Theory
hep-ph/9207268;hep-ph,hep-th;2;30;hep-th/9109027,hep-th/9109032;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;Testing Quantum Mechanics in the Neutral Kaon System
hep-th/9207096;hep-th;0;45;;L.Alvarez-Gaume,K.Becker,M.Becker,R.Emparan,J.Manes;Double Scaling Limit of the Supervirasoro Constraints
hep-th/9207097;hep-th;0;33;;J.Alfaro;The Large-$N$ Limit of the Two-Hermitian-matrix model by the hidden BRST method
hep-th/9207098;hep-th,cond-mat;0;11;;F.Illuminati;Semi-Classical Quantization of the Many-Anyon System
hep-th/9207099;hep-th,cond-mat;0;11;;F.Illuminati;Energy Spectrum of Anyons in a Magnetic Field
hep-th/9207100;hep-th,cond-mat;0;9;;F.Illuminati,M.Patriarca;Thermal Reservoir coupled to External Field and Quantum Dissipation
hep-th/9207101;hep-th;0;14;;L.Bonora,V.Bonservizi;Quantum sl_n Toda field theories
hep-th/9207102;hep-th;0;34;;L.Frappat,E.Ragoucy,P.Sorba;W Algebras and Superalgebras from Constrained WZW Models: A Group Theoretical Classification
hep-th/9207103;hep-th,gr-qc,hep-ph;6;59;hep-th/9109005,hep-th/9109027,hep-th/9109032,hep-th/9111001,hep-th/9111031,hep-th/9112062;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;String Theory Modifies Quantum Mechanics
hep-ph/9207269;hep-ph;0;0;;J.Romao,F.de Campos,J.W.F.Valle;New Higgs Signatures in Supersymmetry with Spontraneously Broken R Parity"
hep-ph/9207270;hep-ph;0;0;;M.Neubert;Recent Developments in the Theory of Heavy-Quark Decays
math/9207204;math.LO;0;2;;U.Fuchs;Donder's Version of Revised Countable Support
hep-th/9207104;hep-th;0;0;;M.Schlichenmaier;Degenerations of Generalized Krichever Novikov algebras on Tori
hep-ph/9207271;hep-ph;0;0;;J.Liu;Final-State-Interaction Simulation of T-Violation in the Top-Quark Semileptonic Decay
hep-th/9207105;hep-th;0;0;;S.W.Hawking,J.M.Stewart;Naked and Thunderbolt Singularities in Black Hole Evaporation
hep-ph/9207272;hep-ph;0;0;;B.Holdom;Vector Meson Dominance and Free Quarks
hep-th/9207106;hep-th;0;12;;E.C.Marino;The New Charged Massless States of Quantum Electrodynamics
hep-th/9207107;hep-th;0;0;;J.Avan;$w_∞$-Currents in 3-Dimensional Toda Theory
hep-ph/9207273;hep-ph;0;32;;C.D.Carone,E.H.Simmons;Oblique Corrections in Technicolor with a Scalar
hep-ph/9207274;hep-ph;0;0;;J.M.Olness;The Nucleon ``Tensor Charges'' and the Skyrme Model
hep-th/9207108;hep-th;0;0;;A.Achucarro;Lineal gravity from planar gravity
hep-th/9207109;hep-th;1;24;hep-th/9112033;S.Govindarajan,T.Jayaraman,V.John;Chiral Rings and Physical States in c<1 String Theory
hep-ph/9207275;hep-ph;0;16;;M.S.Berger;Test of an Equivalence Theorem at One-Loop
math/9207205;math.LO;0;0;;A.Landver;Remark on the Failure of Martin's Axiom
math/9207206;math.FA;0;0;;S.A.Argyros,I.Deliyanni;Banach Spaces Of The Type Of Tsirelson
math/9207207;math.FA;0;0;;E.Odell,H.P.Rosenthal,T.Schlumprecht;On Weakly Null FDD's in Banach Spaces
math/9207208;math.FA;0;8;;F.Chaatit;On Uniform Homeomorphisms of the Unit Spheres of Certain Banach Lattices
math/9207209;math.QA,math.FA;0;0;;A.Cap,A.Kriegl,P.W.Michor,J.Vanžura;The Frölicher-Nijenhuis bracket in non-commutative differential geometry
math/9207210;math.NT,math.GR;0;0;;S.S.Abhyankar;Galois theory on the line in nonzero characteristic
math/9207211;math.DG,math.GT;0;0;;A.Basmajian;Generalizing the hyperbolic collar lemma
math/9207212;math.AP;0;0;;M.G.Crandall,H.Ishii,P.-L.Lions;user's guide to viscosity solutions of second order partial differential equations
math/9207213;math.DG,math.RT;0;0;;E.Damek,F.Ricci;A class of nonsymmetric harmonic Riemannian spaces
math/9207214;math.CV;0;11;;A.Erëmenko;A counterexample to the Arakelyan Conjecture
math/9207215;math.DG;0;0;;C.Gordon,D.L.Webb,S.Wolpert;One cannot hear the shape of a drum
math/9207216;math.CV;0;0;;S.L.Krushkal;The Green function of Teichmüller spaces with applications
math/9207217;math.AT,math.GR;0;0;;J.Martino,S.Priddy;A Classification of the Stable Type of $BG$
math/9207218;math.CO,math.CA;0;0;;H.S.Wilf,D.Zeilberger;Rational function certification of multisum/integral/``$q$'' identities
math/9207219;math.DS;0;28;;G.Swiatek;Hyperbolicity is dense in the real quadratic family
math/9207220;math.DS;0;0;;J.W.Milnor;Local connectivity of Julia sets: expository lectures
math/9207221;math.CA;0;0;;D.E.Knuth;Convolution polynomials
math/9207222;math.CA;0;0;;D.E.Knuth;Johann Faulhaber and sums of powers
hep-lat/9207032;hep-lat;0;27;;M.Campostrini,P.Rossi,E.Vicari;Topological susceptibility and string tension in the lattice CP(N) models
hep-th/9207110;hep-th;0;0;;J.Govaerts;Relativistic Rigid Particles: Classical Tachyons and Quantum Anomalies
hep-th/9207111;hep-th;0;36;;J.Erler,A.Klemm;Comment on the Generation Number in Orbifold Compactifications
hep-th/9207112;hep-th;0;0;;A.Bellini;Planckian Vertices on High Genus Riemann Surfaces
hep-th/9207113;hep-th;0;0;;A.Bellini,M.Ademollo,M.Ciafaloni;Gravitino one-loop contribution to Planckian Scattering
hep-th/9207114;hep-th;0;21;;P.H.Damgaard,H.B.Nielsen,R.Sollacher;Smooth Bosonization II: The Massive Case
hep-ph/9207276;hep-ph;0;65;;R.Ibanez-Meier,I.Stancu,P.M.Stevenson;Gaussian Effective Potential for the U(1) Higgs Model
gr-qc/9207011;gr-qc;0;8;;S.Iyer,A.R.Prasanna;Centrifugal force in Kerr geometry
hep-lat/9207033;hep-lat;0;19;;R.V.Gavai,U.M.Heller,F.Karsch,T.Neuhaus,B.Plache;A Lower Bound on $T_{SR}/{m_{\rm H}}$ in the O(4) Model on Anisotropic Lattices
hep-th/9207115;hep-th;0;0;;A.K.Kshirsagar;Towards a path integral for the pure-spin connection formulation of gravity
hep-th/9207116;hep-th;1;24;hep-th/9112067;M.P.Bellon,J.-M.Maillard,G.Rollet,C.-M.Viallet;Deformations of Dynamics Associated to the Chiral Potts Model
hep-th/9207117;hep-th;0;0;;R.C.Myers,V.Periwal;Chiral gravity in two dimensions
hep-ph/9207277;hep-ph;0;22;;C.Grosse-Knetter,D.Schildknecht;Production of Three Vector Bosons in e+e- Annihilation as a Test of W+-, Z, gamma Self-Interactions
hep-ph/9207278;hep-ph;1;10;hep-ph/9207249;H.Georgi;Generalized Dimensional Analysis
hep-lat/9207034;hep-lat,hep-ph;0;0;;G.Bathas,H.Neuberger;Chiral Yukawa models in the planar limit
cond-mat/9207028;cond-mat,hep-th;0;0;;N.D.Mermin;Crystallography Without Periodicity
hep-lat/9207035;hep-lat,hep-th;0;6;;A.Gocksch,Y.Shen;The Phase Diagram of the $N=2$ Kazakov-Migdal Model
hep-ph/9207279;hep-ph;0;66;;J.Hisano,H.Murayama,T.Yanagida;Nucleon Decay in the Minimal Supersymmetric $SU(5)$ Grand Unification
hep-th/9207118;hep-th,hep-ph;3;19;hep-th/9108001,hep-th/9110054,hep-th/9205037;I.Bars;Heterotic String Models in Curved Spacetime
hep-th/9208001;hep-th;5;21;hep-th/9108001,hep-th/9110054,hep-th/9205037,hep-th/9206006,hep-th/9206048;I.Bars,K.Sfetsos;$SL(2,R)xSU(2)/R^2$ string model in curved spacetime and exact conformal results
hep-lat/9208001;hep-lat,cond-mat,q-bio.QM;0;25;;G.Iori,E.Marinari,G.Parisi;Non-Exponential Relaxation Time Scales in Disordered Systems: an Application to Protein Dynamics
hep-th/9208002;hep-th;0;8;;D.J.Gross;Some Remarks About Induced QCD
hep-th/9208003;hep-th;0;17;;J.C.Gaite;Lagrangians for the W-Algebra Models
hep-lat/9208002;hep-lat;0;15;;F.Karsch,M.L.Laursen,T.Neuhaus,B.Plache,U.-J.Wiese;Chern-Simons term in the 4-dimensional SU(2) Higgs model
hep-th/9208005;hep-th;0;23;;S.Majid;Quantum Random Walks and Time Reversal
alg-geom/9208001;alg-geom,hep-th,math.AG;0;14;;S.Nag,P.Sankaran;Open String Diagrams I: Topological Type
hep-th/9208006;hep-th,math.QA;0;25;;S.Majid;Quantum and Braided Linear Algebra
hep-th/9208007;hep-th;0;29;;T.Brzezinski,S.Majid;Quantum group gauge theory on quantum spaces
hep-th/9208008;hep-th,math.QA;0;51;;S.Majid;Braided Matrix Structure of the Sklyanin Algebra and of the Quantum Lorentz Group
hep-th/9208009;hep-th,gr-qc;0;0;;J.M.Evans,P.A.Tuckey;A Geometrical Approach to Time-Dependent Gauge-Fixing
hep-th/9208010;hep-th,math.QA;0;20;;T.Brzezinski,S.Majid;A Class of Bicovariant Differential Calculi on Hopf Algebras
cond-mat/9208001;cond-mat,hep-lat;0;36;;M.J.Mehl;Pressure Dependence of the Elastic Moduli in Aluminum Rich Al-Li Compounds
hep-th/9208011;hep-th;1;54;hep-th/9201032;M.J.Martins;Exact resonance A-D-E S-matrices and their renormalization group trajectories
hep-ph/9208201;hep-ph;0;38;;M.Jamin,M.Muenz;Current correlators to all orders in the quark masses
hep-lat/9208003;hep-lat;0;0;;M.Flanigan,P.Tamayo;A Parallel Cluster Labeling Method for Monte Carlo Dynamics
hep-th/9208012;hep-th;0;18;;I.I.Kogan,A.Morozov,G.W.Semenoff,N.Weiss;Area Law and Continuum Limit in "Induced QCD"
hep-ph/9208202;hep-ph,astro-ph;0;27;;M.Kamionkowski,K.Freese;Instability and Subsequent Evolution of Electroweak Bubbles
hep-ph/9208203;hep-ph;0;14;;X.-G.He,B.H.J.McKellar;Topological phase due to electric dipole moment and magnetic monopole interaction
hep-th/9208013;hep-th;0;25;;M.D.Freeman,P.West;On the quantum KP hierarchy and its relation to the non-linear Schrödinger equation
hep-ph/9208204;hep-ph;0;23;;J.Bijnens,G.Ecker,J.Gasser;Semileptonic Kaon Decays in Chiral Perturbation Theory
hep-th/9208014;hep-th;0;7;;S.P.Gavrilov,D.M.Gitman;Quantization of systems with time-dependent constraints. Example of relativistic particle in plane wave
hep-ph/9208205;hep-ph;0;0;;A.Pomarol;Spontaneous CP violation in Supersymmetric theories
hep-ph/9208206;hep-ph;0;26;;L.Xiong,E.Shuryak,G.E.Brown;Photon production through $A_1$ resonance in high energy heavy ion collisions
hep-th/9208015;hep-th,gr-qc;0;18;;R.Kantowski,C.Marzban;One-loop Vilkovisky-DeWitt Counterterms for 2D Gravity plus Scalar Field Theory
hep-ph/9208207;hep-ph;0;31;;A.Ali,T.Mannel,T.Ohl;Radiative Rare B Decays into Higher K-Resonances
astro-ph/9208001;astro-ph,hep-ph;0;0;;T.Falk,R.Rangarajan,M.Srednicki;The Angular Dependence of the Three-Point Correlation Function of the Cosmic Microwave Background Radiation as Predicted by Inflationary Cosmologies
astro-ph/9208002;astro-ph;0;0;;T.Falk,R.Rangarajan,M.Srednicki;Dependence of Density Perturbations on the Coupling Constant in a Simple Model of Inflation
hep-th/9208016;hep-th;0;32;;C.Imbimbo;SL(2,R) Chern-Simons Theories with Rational Charges and Two-dimensional Conformal Field Theories
gr-qc/9208001;gr-qc,hep-th;0;0;;J.J.Halliwell;The Interpretation of Quantum Cosmological Models
hep-ph/9208208;hep-ph;0;23;;P.Mathews,V.Ravindran;Can Polarised Drell-Yan Shed More Light On The Proton Spin?
hep-lat/9208004;hep-lat;0;0;;Ph.Boucaud,J.-P.Leroy,J.Micheli,O.Pène,G.C.Rossi;A Rigourous Treatment of the Lattice Renormalization Problem of F_B
hep-th/9208017;hep-th;0;18;;D.M.Gitman,A.L.Shelepin;Coherent States of the SU(N) groups
cond-mat/9208002;cond-mat;0;19;;Th.Pruschke,D.L.Cox,M.Jarrell;Transport Properties of the Infinite Dimensional Hubbard Model
hep-ph/9208209;hep-ph;0;24;;J.C.Collins,F.V.Tkachov;Breakdown of Dimensional Regularization in the Sudakov Problem
hep-ph/9208210;hep-ph;0;22;;X.Li,E.Ma;Gauge Model of Generation Nonuniversality Reexamined
hep-th/9208018;hep-th,gr-qc;1;18;hep-th/9110020;S.Deser,A.Steif;Gravity Theories with Lightlike Sources in D=3
hep-th/9208019;hep-th;0;0;;L.Houart;2D Quantum Gravity and The Miura Map
hep-ph/9208211;hep-ph;0;39;;K.Haglin,C.Gale,V.Emel'yanov;Soft dilepton production in relativistic heavy ion collisions
hep-th/9208020;hep-th,hep-lat;0;29;;S.Khokhlachev,Yu.Makeenko;The Problem of Large-N Phase Transition in Kazakov-Migdal Model of Induced QCD
hep-ph/9208212;hep-ph,gr-qc,hep-th;0;22;;J.Garriga,A.Vilenkin;Black Holes from Nucleating Strings
hep-ph/9208213;hep-ph;0;17;;J.Collins;Fragmentation of Transversely Polarized Quarks Probed in Transverse Momentum Distributions
alg-geom/9208002;alg-geom,math.AG;0;0;;K.A.Ribet;Abelian varieties over Q and modular forms
astro-ph/9208003;astro-ph,hep-th;0;25;;S.Åminneborg;The Probability for Formation of Collapsing Textures and Texture Knots
cond-mat/9208003;cond-mat;0;22;;F.Guinea,O.Pla,E.Louis;Complexity and criticality in Laplacian growth models
hep-ph/9208214;hep-ph;0;0;;F.Lucchin,S.Matarrese,S.Mollerach;The gravitational wave contribution to CMB anisotropies and the amplitude of mass fluctuations from COBE results
cond-mat/9208004;cond-mat,hep-th;0;16;;J.González,F.Guinea,M.A.H.Vozmediano;The Electronic Spectrum of Fullerenes from the Dirac Equation
cond-mat/9208005;cond-mat;0;42;;J.Baez,M.Ody,W.Richter;Topological Aspects of Spin and Statistics in Nonlinear Sigma Models
hep-lat/9208005;hep-lat;0;0;;M.Hecht;Comparison of Lattice Coulomb Gauge Wave Functions in Quenched Approximation and with Dynamical Fermions
hep-th/9208021;hep-th;0;0;;L.Mezincescu,R.I.Nepomechie;Models with Quantum Symmetry and their Spectra
hep-ph/9208215;hep-ph,hep-lat,hep-th;0;34;;J.March-Russell;On the Possibility of Second-Order Phase Transitions in Spontaneously Broken Gauge Theories
hep-th/9208022;hep-th;0;0;;A.Marshakov;On string field theory for $C ≤1$
hep-th/9208023;hep-th,hep-ph;0;32;;A.E.Faraggi;Aspects of Nonrenormalizable Terms in a Superstring Derived Standard--like Model
hep-th/9208024;hep-th,hep-ph;0;37;;A.E.Faraggi;Construction of Realistic Standard--like Models in the Free Fermionic Superstring Formulation
hep-ph/9208216;hep-ph;0;16;;D.B.DeLaney,S.Jadach,C.Shio,G.Siopsis,B.F.L.Ward;Multiple photon effects in $pp$ scattering at SSC energies
hep-ph/9208217;hep-ph,astro-ph;0;0;;T.Souradeep,V.Sahni;Density Perturbations,Gravity Waves and the Cosmic Microwave Background
hep-th/9208025;hep-th;0;0;;N.Kaloper;A Closed Bianchi I Universe in String Theory
hep-th/9208026;hep-th;0;51;;L.Alvarez-Gaume,J.L.F.Barbon,C.Crnkovic;A Proposal for Strings at D>1
hep-th/9208027;hep-th;0;22;;E.Witten;On Background Independent Open-String Field Theory
hep-th/9208028;hep-th;3;40;hep-th/9108004,hep-th/9109032,hep-th/9112009;I.I.Kogan;Area Preserving Diffeomorphisms and $W_∞$ Symmetry in a $2+1$ Chern-Simons Theory
hep-ph/9208218;hep-ph;0;0;;M.James,L.Perivolaropoulos,T.Vachaspati;On the Stability of Electroweak Strings (New Version)
hep-th/9208029;hep-th;0;41;;D.Anselmi,P.Fre;Twisted N=2 Supergravity as Topological Gravity in Four Dimensions
hep-ph/9208219;hep-ph,gr-qc;0;0;;T.Souradeep,V.Sahni;Quantum effects near a point mass in 2+1 dimensional gravity
hep-th/9208030;hep-th;2;21;hep-th/9111011,hep-th/9204018;J.Ambjorn,B.Durhuus,T.Jonsson,G.Thorleifsson;Matter fields with c > 1 coupled to 2d gravity
cond-mat/9208006;cond-mat;0;37;;Th.Pruschke,D.L.Cox,M.Jarrell;The Hubbard Model at Infinite Dimensions: Thermodynamic and Transport Properties
hep-th/9208031;hep-th;6;53;hep-th/9108004,hep-th/9109032,hep-th/9111021,hep-th/9111035,hep-th/9201005,hep-th/9201056;R.Dijkgraaf,G.Moore,R.Plesser;The partition function of 2d string theory
hep-ph/9208220;hep-ph;0;44;;M.Herrero,E.Ruiz-Morales;Study of gamma gamma -> W_L W_L and gamma gamma -> Z_L Z_L reactions with Chiral Lagrangians
gr-qc/9208002;gr-qc,hep-th;0;0;;C.R.Nappi,A.Pasquinucci;Thermodynamics of Two-Dimensional Black-Holes
hep-ph/9208221;hep-ph;0;22;;Z.Guralnik,M.Luke,A.V.Manohar;Properties of Baryons Containing a Heavy Quark in the Skyrme Model
gr-qc/9208003;gr-qc,astro-ph;0;0;;T.Souradeep;Generation of seed perturbations from Quantum Cosmology
hep-ph/9208222;hep-ph;0;121;;R.Anderson,G.C.Joshi;Quaternions and the heuristic role of mathematical structures in physics
hep-ph/9208223;hep-ph;0;20;;A.D.Rújula,S.L.Glashow;Neutrino Helioseismology
astro-ph/9208004;astro-ph,hep-ph;0;0;;B.B.Nath;Constraints on radiative decay of the 17-keV neutrino from COBE Measurements
hep-lat/9208006;hep-lat;0;30;;M.Goeckeler,A.S.Kronfeld,G.Schierholz,U.-J.Wiese;Continuum Gauge Fields from Lattice Gauge Fields
hep-th/9208032;hep-th,hep-lat;1;38;hep-th/9108006;J.Ambjorn,J.Jurkiewicz,C.F.Kristjansen;Quantum Gravity, Dynamical Triangulation and Higer Derivative Regularization
hep-lat/9208007;hep-lat,cond-mat,hep-ph;0;0;;C.Bernard,A.Soni,K.Yee;Introduction to Lattice Gaugefixing and Effective Quark and Gluon Masses
cond-mat/9208007;cond-mat;0;22;;D.L.Cox;Selection Rules for Two Channel Kondo Models of U and Ce ions in Metals
hep-lat/9208008;hep-lat,hep-th;0;25;;A.A.Migdal;Phase Transitions in Induced QCD
hep-ph/9208224;hep-ph;0;12;;R.Easther,W.Moreau;Calculating the Critical Temperature for Coleman-Weinberg GUTs
hep-th/9208033;hep-th;0;34;;P.G.O.Freund,A.V.Zabrodin;A Hierarchical Array of Integrable Models
hep-th/9208034;hep-th,gr-qc;0;0;;R.Brooks,D.Cangemi,M.Crescimanno;Einstein Gravity in 2+1 Dimensions from a Gauge Model with Symmetry Breaking
hep-lat/9208009;hep-lat,hep-ph;0;0;;J.E.Mandula,M.C.Ogilvie;A New Technique for Measuring the Strangemess Content of the Proton on the Lattice
hep-lat/9208010;hep-lat;0;26;;M.L.Paciello,C.Parrinello,S.Petrarca,B.Taglienti,A.Vladikas;Gribov Copies and Smeared Correlation Functions in Lattice QCD
hep-lat/9208011;hep-lat;0;5;;R.M.Neal;An Improved Acceptance Procedure for the Hybrid Monte Carlo Algorithm
cond-mat/9208008;cond-mat;0;11;;G.D.Lorenzi,F.Ercolessi;Multiple jumps and vacancy diffusion in a face-centered cubic metal
math/9208201;math.FA;0;16;;H.König,N.J.Nielsen;Vector-valued L_p convergence of orthogonal series and Lagrange interpolation
math/9208202;math.FA;0;0;;H.König;Vector-valued Lagrange interpolation and mean convergence of Hermite series
math/9208203;math.QA;0;3;;A.Cap,P.W.Michor;Towards the Chern-Weil homomormism in non-commutative differential geometry
math/9208204;math.DS;0;0;;A.Poirier;Hubbard forests
hep-th/9208035;hep-th;0;0;;N.Berkovits;Calculation of Green-Schwarz Superstring Amplitudes Using the N=2 Twistor-String Formalism
gr-qc/9208004;gr-qc,hep-th;2;18;hep-th/9111056,hep-th/9203056;R.B.Mann,S.F.Ross;The $D→2$ Limit of General Relativity
hep-th/9208036;hep-th,gr-qc;1;7;hep-th/9204099;S.F.Ross,R.B.Mann;Gravitationally Collapsing Dust in $(2+1)$ Dimensions
gr-qc/9208005;gr-qc;0;27;;S.Habib,H.E.Kandrup;Nonlinear Noise in Cosmology
cond-mat/9208009;cond-mat;0;15;;G.Dev,J.K.Jain;Band Structure of the Fractional Quantum Hall Effect
hep-ph/9208225;hep-ph;2;37;hep-ph/9212291,hep-ph/9303201;G.Cvetič,C.Grosse-Knetter,R.Kögerler;Two- and Three Vector Boson Production in e+ e- Collisions within the BESS Model
hep-th/9208037;hep-th;1;26;hep-th/9201016;P.Aschieri,L.Castellani;Bicovariant differential geometry of the quantum group GL_q(3)
hep-th/9208038;hep-th;0;29;;J.Erler,M.Spalinski;Modular Groups for Twisted Narain Models
hep-th/9208039;hep-th;4;18;hep-th/9108004,hep-th/9109012,hep-th/9109032,hep-th/9111048;E.Smith;Trivial Spectrum of Free 1+1 Light-Cone Strings
gr-qc/9208006;gr-qc;0;40;;S.Habib;Stochastic Inflation:The Quantum Phase Space Approach
hep-th/9208040;hep-th;1;34;hep-th/9111001;O.Aharony,O.Ganor,J.Sonnenschein,S.Yankielowicz;On the twisted G/H topological models
hep-th/9208041;hep-th;0;0;;G.Savvidy,K.Savvidy;String fine tuning
hep-ph/9208226;hep-ph;0;22;;J.R.Espinosa,M.Quirós;Higgs boson bounds in non-minimal supersymmetric standard models
hep-lat/9208012;hep-lat;0;0;;J.Fingberg,U.M.Heller,F.Karsch;Scaling and Asymptotic Scaling in the SU(2) Gauge Theory
hep-th/9208042;hep-th;2;32;hep-th/9109005,hep-th/9112059;I.K.Kostov,M.Staudacher;Strings in Discrete and Continuous Target Spaces: A Comparison
hep-ph/9208227;hep-ph;0;20;;D.Land,E.Carlson;Two Stage Phase Transition in Two Higgs Models
hep-th/9208043;hep-th;2;9;hep-th/9207029,hep-th/9207030;T.A.Larsson;Diffeomorphism group and conformal fields
cond-mat/9208010;cond-mat;0;20;;A.-L.Barabási;Dynamic Scaling of Coupled Nonequilibrium Interfaces
cond-mat/9208011;cond-mat;0;16;;J.von Delft,C.L.Henley;Destructive quantum interference in spin tunneling problems
hep-lat/9208013;hep-lat;0;6;;A.J.van der Sijs;Gauge invariant extremization on the lattice
hep-th/9208044;hep-th;2;37;hep-th/9201010,hep-th/9201013;S.Kharchev,A.Marshakov,A.Mironov,A.Morozov,S.Pakuliak;Conformal Matrix Models as an Alternative to Conventional Multi-Matrix Models
hep-ph/9208228;hep-ph;0;0;;A.Dattta,M.Guchait,D.P.Roy;Prospect of Heavy Right-Handed Neutrino Search at SSC/LHC Energies
hep-th/9208045;hep-th,hep-lat;0;24;;Yu.Makeenko;Large-N Reduction, Master Field and Loop Equations in Kazakov-Migdal Model
hep-ph/9208229;hep-ph;0;8;;T.V.Duong,E.Ma;Decay of the Z Boson into Scalar Particles
hep-lat/9208014;hep-lat;0;0;;A.Nabutovsky,R.Ben-Av;Noncomputability Arising In Dynamical Triangulation Model Of Four-Dimensional Quantum Gravity
hep-ph/9208230;hep-ph;1;83;hep-ph/9203202;E.Akhmedov,Z.B.G.Senjanovic,Z.Tao;Planck scale effects in neutrino physics
hep-ph/9208231;hep-ph,astro-ph,gr-qc;1;34;hep-ph/9203203;M.Gleiser,E.W.Kolb;Critical Behavior in the Electroweak Phase Transition
gr-qc/9208007;gr-qc,hep-th;0;10;;N.Ó.Murchadha,H.Shanahan;There is no $R^3 X S^1$ vacuum gravitational instanton
hep-th/9208046;hep-th;1;17;hep-th/9201013;S.Kharchev,A.Marshakov,A.Mironov,A.Morozov;Landau-Ginzburg Topological Theories in the Framework of GKM and Equivalent Hierarchies
hep-th/9208047;hep-th;0;43;;C.Lucchesi,O.Piguet,S.P.Sorella;Renormalization and finiteness of topological BF theories
hep-ph/9208232;hep-ph;0;25;;V.Koch,G.Bertsch;Effects of Collective Potentials on Pion Spectra in Relativistic Heavy Ion Collisions
cond-mat/9208012;cond-mat;0;18;;D.Loss,D.P.DiVincenzo,G.Grinstein;Suppression of tunneling by interference in half-integer--spin particles
hep-ph/9208233;hep-ph,cond-mat,hep-th;0;0;;M.J.Bowick,L.Chandar,E.A.Schiff,A.M.Srivastava;The Cosmological Kibble Mechanism in the Laboratory: String Formation in Liquid Crystals
gr-qc/9208008;gr-qc,astro-ph;0;0;;E.Malec,N.Ó.Murchadha;Trapped surfaces and spherical closed cosmologies
hep-ph/9208234;hep-ph,hep-th;0;10;;A.P.de Almeida,J.Frenkel;On the Infrared Behavior of the Pressure in Thermal Field Theories
hep-th/9208048;hep-th;0;29;;F.Toppan,Y.-Z.Zhang;Superconformal Affine Liouville Theory
cond-mat/9208013;cond-mat;0;0;;M.R.Norman;Effect of Matrix Elements on the Pairing Kernel in Exchange Mediated Superconductors
hep-th/9208049;hep-th;0;15;;D.M.Gitman,A.V.Saa;Pseudoclassical Model of Spinning Particle with Anomalous Magnetic Momentum
hep-th/9208050;hep-th,hep-lat;0;29;;Y.Meurice;Remarks Concerning Polyakov's Conjecture for the 3D Ising Model and the Hierarchical Approximation
hep-lat/9208015;hep-lat,hep-th;0;22;;Y.Meurice;Duality in Long-Range Ising Ferromagnets
funct-an/9208001;funct-an,math.OA;0;0;;V.G.Pestov;Universal arrows to forgetful functors from categories of topological algebra
gr-qc/9208009;gr-qc,astro-ph,hep-th;0;50;;R.Brandenberger,T.Prokopec,V.Mukhanov;The Entropy of the Gravitational Field
alg-geom/9208003;alg-geom,math.AG;0;0;;A.Garcia,R.F.Lax;Weierstrass weight of Gorenstein singularities with one or two branches
hep-ph/9208235;hep-ph;0;21;;Y.Achiman,A.Lukas;E6 GUT and Large Neutrino Mixing
hep-lat/9208016;hep-lat;1;7;hep-lat/9208003;E.Onofri;Embedding Z(3) in SU(3)
cond-mat/9208014;cond-mat;0;28;;J.Liu,K.Ismail,K.Lee,J.Hong,S.Washburn;Electron focusing, mode spectroscopy and mass enhancement in small GaAs/AlGaAs rings
hep-lat/9208017;hep-lat,hep-ph;1;14;hep-lat/9107001;H.Neuberger,U.M.Heller,M.Klomfass,P.Vranas;The triviality bound on the Higgs mass; its value and what it means
hep-lat/9208018;hep-lat;0;12;;UKQCD Collaboration,C.R.Allton,C.T.Sachrajda,S.P.Booth,K.C.Bowler,D.S.Henty,R.D.Kenway,B.J.Pendleton,D.G.Richards,J.N.Simone,A.D.Simpson,C.Michael,P.W.Stephenson;The Hyperfine Splitting in Charmonium: Lattice Computations Using the Wilson and Clover Fermion Actions
hep-lat/9208019;hep-lat;0;0;;H.Rieger;Fast vectorized algorithm for the Monte Carlo Simulation of the Random Field Ising Model
hep-lat/9208020;hep-lat;1;43;hep-lat/9107002;B.Grossmann,M.L.Laursen,T.Trappenberg,U.-J.Wiese;The confined-deconfined Interface Tension and the Spectrum of the Transfer Matrix
hep-lat/9208021;hep-lat;0;0;;S.J.Hands,A.Kocic,J.B.Kogut,R.L.Renken,D.K.Sinclair,K.C.Wang;Spectroscopy, Equation Of State And Monopole Percolation In Lattice QED With Two Flavors
hep-lat/9208022;hep-lat;0;0;;S.Hands,A.Kocic,J.B.Kogut;Four - Fermi Theories in Fewer Than Four Dimensions
hep-th/9208051;hep-th;0;0;;J.Louis;Differential Equations in Special Kahler Geometry
hep-th/9208052;hep-th,hep-ph;0;0;;M.Carreau;The Functional Integral for a Free Particle on a Half-Plane
hep-ph/9208236;hep-ph;0;15;;W.A.Ponce,A.Zepeda,R.G.Lozano;The Generational Seesaw Mechanism in [SU(6)]$^3×$Z$_3$}
hep-ph/9208237;hep-ph;0;5;;V.Bhansali;Renormalization Group Coefficients for the Un-Truncated Derivative Expansion in Effective Field Theory
hep-ph/9208238;hep-ph;0;10;;E.Jenkins,A.V.Manohar;Hyperfine Splittings of Baryons Containing a Heavy Quark in the Skyrme Model
hep-th/9208053;hep-th;2;18;hep-th/9112059,hep-th/9203019;I.Kostov;Gauge Invariant Matrix Model for the Â-{\^D}-{\^E} Closed Strings
hep-th/9208054;hep-th;1;24;hep-th/9201013;I.I.Kogan,A.Morozov,G.W.Semenoff,N.Weiss;Continuum Limits of ``Induced QCD": Lessons of the Gaussian Model at d=1 and Beyond
hep-th/9208055;hep-th;3;32;hep-th/9110070,hep-th/9112023,hep-th/9201019;J.A.Dixon,M.J.Duff,J.C.Plefka;Putting String/Fivebrane Duality to the Test
hep-ph/9208239;hep-ph,astro-ph;0;0;;James.M.Gelb,B.-A.Gradwohl,J.A.Frieman;Large- and Small-Scale Constraints on Power Spectra in $Ω=1$ Universes
hep-ph/9208240;hep-ph;0;8;;A.Czarnecki,S.Davidson;On the QCD corrections to the charged Higgs decay of a heavy quark
hep-ph/9208241;hep-ph;0;31;;D.Harley,T.Kuo,J.Pantaleone;Solar Neutrinos with Three Flavor Mixings
alg-geom/9208004;alg-geom,math.AG;0;21;;R.Miranda;Torsion Sections of Semistable Elliptic Surfaces
hep-lat/9208023;hep-lat,hep-th;1;16;hep-lat/9208008;A.A.Migdal;Mixed Model of Induced QCD
hep-lat/9208024;hep-lat,cond-mat;0;0;;S.Gupta,A.Irbaeck;Finite-Size Scaling on the Ising Coexistence Line
hep-th/9208056;hep-th;0;15;;Y.Tanii;Semiclassical Quantization of Two-Dimensional Dilaton Gravity
hep-th/9208057;hep-th,nlin.SI,solv-int;0;12;;N.MacKay,W.McGhee;Affine Toda Solitons and Automorphisms of Dynkin Diagrams
hep-th/9208058;hep-th,nlin.SI,solv-int;0;0;;T.Hollowood,J.L.Miramontes;Tau-Functions and Generalized Integrable Hierarchies
hep-th/9208059;hep-th;1;33;hep-th/9112035;F.Bastianelli,P.van Nieuwenhuizen;Trace Anomalies from Quantum Mechanics
hep-ph/9208242;hep-ph;0;17;;J.E.C.Montalvo,O.J.P.Eboli;Composite Vector Leptoquarks in $e^+ e^-$, $γe$, and $γγ$ Colliders
hep-ph/9208243;hep-ph;0;19;;S.Dimopoulos,L.J.Hall,S.Raby;Neutrino masses and mixings in a predictive theory of fermion masses
hep-th/9208060;hep-th,astro-ph,gr-qc;0;12;;S.K.Chakrabarti,P.S.Joshi;Naked Singularities as Possible Candidates for Gamma-ray Bursters
hep-th/9208061;hep-th,nlin.SI,solv-int;0;29;;P.Martin,H.Saleur;On an algebraic approach to higher dimensional statistical mechanics
hep-th/9208062;hep-th;0;50;;E.C.Marino;Duality, Quantum Vortices and Anyons in Maxwell-Chern-Simons-Higgs Theories
hep-ph/9208244;hep-ph;3;29;hep-ph/9203225,hep-ph/9204207,hep-ph/9204237;P.Cho;Heavy Hadron Chiral Perturbation Theory
hep-th/9208063;hep-th;1;20;hep-th/9110066;P.G.O.Freund,A.V.Zabrodin;Excitation Scattering in Integrable Models and Hall-Littlewood-Kerov Polynomials
gr-qc/9208010;gr-qc,hep-th;0;0;;K.Kamimura,T.Fukuyama;Massive Analogue of Ashtekar-CJD Action
astro-ph/9208005;astro-ph,gr-qc;0;42;;C.Cutler,T.A.Apostolatos,L.Bildsten,L.S.Finn,E.E.Flanagan,D.Kennefick,D.M.Markovic,A.Ori,E.Poisson,G.J.Sussman,K.S.Thorne;The Last Three Minutes: Issues in Gravitational Wave Measurements of Coalescing Compact Binaries
cond-mat/9208015;cond-mat;0;15;;H.Rieger;Number of solutions of the TAP equations for p--spin interaction spin glasses
hep-th/9208064;hep-th;4;18;hep-th/9109024,hep-th/9111048,hep-th/9112033,hep-th/9201072;S.Govindarajan,T.Jayaraman,V.John;Genus Zero Correlation Functions in c<1 String Theory
hep-ph/9208245;hep-ph;0;0;;R.Holman,S.D.H.Hsu,T.Vachaspati,R.Watkins;Metastable Cosmic Strings in Realistic Models
cond-mat/9208016;cond-mat,hep-th;1;19;hep-th/9202057;M.Fowler,J.A.Minahan;Invariants of the Haldane-Shastry $SU(N)$ Chain
hep-ph/9208246;hep-ph;0;10;;Z.Lalak,K.Meissner,J.Pawełczyk;Gravitationally Induced Scalar Field Fluctuations in the Radiation Dominated R-W Universe
hep-ph/9208247;hep-ph,astro-ph;0;23;;L.Perivolaropoulos;COBE vs Cosmic Strings: An Analytical Model
cond-mat/9208017;cond-mat;0;14;;Y-h.Taguchi,H.Takayasu;Non-Gaussian distribution in Random advection dynamics
hep-ph/9208248;hep-ph;0;24;;E.Jenkins,A.V.Manohar,M.B.Wise;The Baryon Isgur-Wise Function in the Large $N_c$ Limit
cond-mat/9208018;cond-mat;0;19;;Y-h.Taguchi,H.Takayasu;Homogeneous Isotropic Fluid Turbulence Simulated with the Lattice Vortex Tube Model
cond-mat/9208019;cond-mat;0;0;;K.Harigaya,M.Fujita;Dimerization and Energy-Level Structures in Fullerene Tubules Investigated with an Electron-Phonon Model
hep-ph/9208249;hep-ph;0;15;;S.D.Ellis,Z.Kunszt,D.E.Soper;Large Jets at Hadron Colliders at Order $α_s^3$: A Look Inside
hep-ph/9208250;hep-ph;0;18;;M.A.Doncheski,R.W.Robinett,L.Weinkauf;Spin-Spin Asymmetries in Large Transverse Momentum Higgs Boson Production
hep-ph/9208251;hep-ph;0;14;;S.Mizuta,M.Yamaguchi;Coannihilation Effects and Relic Abundance of Higgsino-Dominant LSPs
cond-mat/9208020;cond-mat;0;34;;T.Hsu;Frequency dependent conductivity of vortex cores in type II superconductors
cond-mat/9208021;cond-mat;0;33;;B.S.Shastry;Mott Transition in the Hubbard model
hep-ph/9208252;hep-ph;0;46;;W.Broniowski,T.D.Cohen;The structure of the pion and effective electroweak currents in soliton models of the nucleon
hep-ph/9208253;hep-ph;0;18;;T.D.Cohen,W.Broniowski;The role of the Delta isobar in chiral perturbation theory and hedgehog soliton models
hep-th/9208065;hep-th;0;0;;S.Roy,S.Panda;The Lax Operator Approach for the Virasoro and the W-Constraints in the Generalized KdV Hierarchy
hep-ph/9208254;hep-ph;0;24;;G.T.Bodwin,E.Braaten,T.C.Yuan,G.P.Lepage;P-Wave Charmonium Production in B-Meson Decays
hep-lat/9208025;hep-lat,hep-ph;0;56;;D.B.Leinweber,T.Draper,R.M.Woloshyn;Decuplet Baryon Structure from Lattice QCD
hep-th/9208066;hep-th;0;0;;M.Idzumi,K.Iohara,M.Jimbo,T.Miwa,T.Nakashima,T.Tokihiro;Quantum affine symmetry in vertex models
hep-th/9208067;hep-th,nlin.SI,solv-int;0;0;;M.Jimbo,T.Miwa,Y.Ohta;Structure of the space of states in RSOS models
hep-th/9208068;hep-th;0;0;;R.Perret;Dual formulation of classical W-algebras
astro-ph/9208006;astro-ph,gr-qc;0;9;;S.K.Chakrabarti;Binary Black Holes in Stationary Orbits
hep-lat/9208026;hep-lat,cond-mat;0;0;;A.Billoire;Numerical Study of Finite Size Scaling for First Order Phase Transitions
hep-th/9208069;hep-th;0;0;;R.Blumenhagen;N=2 supersymmetric W-algebras
hep-lat/9208027;hep-lat,hep-th;0;0;;P.van Baal,R.E.Cutkosky;Non-perturbative analysis, Gribov horizons and the boundary of the fundamental domain
hep-lat/9208028;hep-lat;1;31;hep-lat/9205010;G.S.Bali,K.Schilling;Running Coupling and the Lambda-Parameter from SU(3) Lattice Simulations
hep-ph/9208255;hep-ph,astro-ph;0;39;;M.Urban,A.Bouquet,B.Degrange,P.Fleury,J.Kaplan,A.L.Melchior,E.Paré;Searching for TeV dark matter by atmospheric Cerenkov techniques
astro-ph/9208007;astro-ph,gr-qc,hep-ph;0;46;;D.H.Lyth,A.R.Liddle;COBE, Gravitational Waves, Inflation and Extended Inflation
cond-mat/9208022;cond-mat;0;40;;V.Fiorentini,M.Methfessel,M.Scheffler;Electronic and structural properties of GaN by the full-potential LMTO method : the role of the $d$ electrons
cond-mat/9208023;cond-mat;0;25;;P.L.Doussal,L.Radzihovsky;Self-Consistent Theory of Polymerized Membranes
hep-th/9208070;hep-th;0;31;;B.Harms,Y.Leblanc;Statistical Mechanics of Extended Black Objects
hep-lat/9208029;hep-lat;0;22;;S.Aoki,A.Gocksch,Y.Shen;A Study of the $N=2$ Kazakov-Migdal Model
hep-ph/9208256;hep-ph;0;66;;W.Broniowski,T.D.Cohen;Response of nucleons to external probes in hedgehog models: I. Electromagnetic polarizabilities
hep-ph/9208257;hep-ph;0;57;;W.Broniowski,T.D.Cohen;Response of nucleons to external probes in hedgehog models: II. General formalism
hep-th/9208071;hep-th,hep-lat;0;17;;S.Khokhlachev,Yu.Makeenko;Adjoint Fermions Induce QCD
hep-th/9208072;hep-th;1;34;hep-th/9108003;F.Gieres,S.Theisen;Superconformally covariant operators and super W algebras
hep-th/9208073;hep-th;2;66;hep-th/9112075,hep-th/9202013;V.Spiridonov;Deformation of Supersymmetric and Conformal Quantum Mechanics Through Affine Transformations
hep-th/9208074;hep-th;0;0;;B.de Wit,A.K.Tollsten,H.Nicolai;Locally supersymmetric D=3 non-linear sigma models
hep-lat/9208030;hep-lat;0;0;;M.-C.Chu,J.M.Grandy,S.Huang,J.W.Negele;Lattice Calculation of QCD Vacuum Correlation Functions
hep-ph/9208258;hep-ph;0;7;;J.Chyla,J.Rames;Parton-Hadron duality in event generators
hep-ph/9208259;hep-ph;0;28;;E.H.Simmons,R.S.Chivukula,S.B.Selipsky;Extended Technicolor Corrections to the $Z b\bar b$ Vertex
hep-th/9208075;hep-th;0;24;;G.Weigt;Canonical Quantization of the Liouville Theory, Quantum Group Structures, and Correlation Functions
gr-qc/9208011;gr-qc,astro-ph;0;43;;J.H.Kung;Comparison of the Sachs-Wolfe Effect for Gaussian and Non-Gaussian Fluctuations
hep-th/9208076;hep-th;1;11;hep-th/9112070;A.Giveon,A.Pasquinucci;On Cosmological String Backgrounds with Toroidal Isometries
hep-th/9208077;hep-th;0;0;;J.M.Figueroa-O'Farrill,J.Mas,E.Ramos;The Topography of $\W _∞$-Type Algebras
cond-mat/9208024;cond-mat,hep-th;0;0;;S.Fishmen,Y.Shapir,X.-R.Wang;Localized Electrons on a Lattice with Incommensurate Magnetic Flux
cond-mat/9208025;cond-mat;0;40;;A.Yamagata;Interfacial adsorption phenomena of the three-dimensional three-state Potts model
hep-th/9208078;hep-th;0;19;;T.Ortín;Electric-Magnetic Duality and Supersymmetry in Stringy Black Holes
hep-ph/9208260;hep-ph;0;29;;K.S.Babu,R.R.Volkas;Bounds on mini-charged neutrinos in the minimal standard model
hep-ph/9208261;hep-ph;0;18;;Yu.L.Kalinovsky,L.Kaschluhn;Bilocal Field Approach and Semileptonic Heavy Meson Decays
hep-th/9208079;hep-th;0;0;;A.Matsuo;Free Field Representation of Quantum Affine Algebra U_q(\hat {sl}_2)
hep-ph/9208262;hep-ph;1;14;hep-ph/9203202;C.P.Burgess,J.M.Cline,M.Luty;New Neutrino Physics Without Fine Tuning
cond-mat/9208026;cond-mat;0;34;;B.Janko,J.D.Shore;Electromagnetic response of a static vortex line in a type-II superconductor : a microscopic study
cond-mat/9208027;cond-mat;0;13;;A.V.Balatsky,B.L.Altshuler;Persistent spin and mass currents and Aharonov-Casher effect
hep-th/9208080;hep-th;9;30;hep-th/9108004,hep-th/9109005,hep-th/9109032,hep-th/9111021,hep-th/9201056,hep-th/9201061,hep-th/9202035,hep-th/9203052,hep-th/9203056;Y.Matsumura,N.Sakai,Y.Tanii,T.Uchino;Correlation Functions in Two-Dimensional Dilaton Gravity
hep-th/9208081;hep-th;8;67;hep-th/9108004,hep-th/9109032,hep-th/9111021,hep-th/9111056,hep-th/9201061,hep-th/9203052,hep-th/9203056,hep-th/9207105;N.Sakai;c = 1 Two Dimensional Quantum Gravity
cond-mat/9209001;cond-mat;0;0;;Z.-S.Ma,Z.-B.Su;The Constraint for the Lowest Landau Level and the Effective Field Theory Approach for the Fractional Quantum Hall System
hep-th/9209001;hep-th;0;14;;C.Ahn;Explicit Construction of Spin 4 Casimir Operator in the Coset Model $ \hat {SO} (5)_1 ×\hat {SO} (5)_m / \hat {SO} (5)_{1+m} $
hep-th/9209002;hep-th;0;0;;J.M.Figueroa-O'Farrill,E.Ramos,S.Stanciu;A geometrical interpretation of classical W-transformations
hep-th/9209003;hep-th;0;36;;S.Iso,D.Karabali,B.Sakita;Fermions in the Lowest Landau Level: Bosonization, $W_∞$ Algebra, Droplets, Chiral Boson
hep-th/9209004;hep-th;0;13;;G.Haak;Group Theoretical Symmetries and Generalized Baecklund Transformations for Integrable Systems
hep-ph/9209201;hep-ph;0;0;;H.König;Minimal Supersymmetric Standard Model Extended by One Additional Higgs Singlet and its Influence on the Anomalous Magnetic Moment of the Muon
hep-lat/9209001;hep-lat;0;0;;B.A.Berg,B.Krishnan,M.Katoot;Asymptotic Freedom and Euclidean Quantum Gravity
hep-lat/9209002;hep-lat;0;6;;K.Jansen,M.Schmaltz;Critical Momenta of Lattice Chiral Fermions
hep-th/9209005;hep-th;0;72;;W.Chen,G.W.Semenoff,Y.-S.Wu;Two-Loop Analysis of Non-abelian Chern-Simons Theory
hep-ph/9209202;hep-ph;0;0;;Y.N.Srivstava,A.Widom,M.H.Friedman,O.Panella;Compact Lattice QED and the Coulomb Potential
hep-ph/9209203;hep-ph;0;9;;L.S.Brown;Summing tree graphs at threshold
hep-th/9209006;hep-th;2;38;hep-th/9112009,hep-th/9203062;H.Aratyn,E.Nissimov,S.Pacheva,I.Vaysburd;R-Matrix Formulation of KP Hierarchies and their Gauge Equivalence
hep-ph/9209204;hep-ph;0;30;;M.N.Butler,M.J.Savage;Electromagnetic Polarisability of the Nucleon in Chiral Perturbation Theory
hep-lat/9209003;hep-lat,hep-th;1;13;hep-lat/9209002;M.Golterman,K.Jansen,D.Kaplan;Chern-Simons Currents and Chiral Fermions on the Lattice
hep-lat/9209004;hep-lat;0;14;;K.Jansen;The Finite Temperature Phase Diagram of a U(1) Higgs-Yukawa Model
hep-lat/9209005;hep-lat;1;24;hep-lat/9205001;U.Wolff;High Precision Simulation Techniques for Lattice Field Theory
hep-th/9209007;hep-th;1;20;hep-th/9205018;G.Barnich,R.Constantinescu,P.Gregoire;BRST-anti-BRST Antifield formalism : The Example of the Freedman-Townsend Model
hep-th/9209008;hep-th,gr-qc;4;17;hep-th/9111056,hep-th/9201061,hep-th/9203042,hep-th/9203052;D.A.Lowe;Semiclassical Approach to Black Hole Evaporation
hep-th/9209009;hep-th;0;27;;A.Abada,A.H.bougourzi,M.A.E.Gradechi;Deformation of the Wakimoto construction
hep-th/9209010;hep-th;4;26;hep-th/9108004,hep-th/9109005,hep-th/9109025,hep-th/9109032;G.Aldazabal,M.Bonini,J.M.Maldacena;Factorization and Discrete States in C=1 Superliouville Theory
hep-ph/9209205;hep-ph;0;0;;A.Donnachie,P.V.Landshoff;Total cross sections
hep-ph/9209206;hep-ph;0;66;;E.Akhmedov,Z.Berezhiani,G.Senjanovic,Z.Tao;17 keV neutrino and large magnetic moment solution of the solar neutrino puzzle
hep-ph/9209207;hep-ph;0;41;;T.G.Rizzo;The Production of $Z'$ Associated With Photons or Jets as a Probe of New Gauge Boson Couplings
gr-qc/9209001;gr-qc;0;0;;J.W.Moffat;Quantum Gravity, the Origin of Time and Time's Arrow
math/9209201;math.LO;0;0;;M.Kojman,S.Shelah;Non-existence of Universal Orders in Many Cardinals
hep-lat/9209006;hep-lat,cond-mat;0;8;;U.-J.Wiese;Capillary Waves in Binder's Approach to the Interface Tension
hep-ph/9209208;hep-ph;4;30;hep-th/9109045,hep-th/9202003,hep-ph/9203206,hep-ph/9205229;E.J.Chun,A.Lukas;Discrete Gauge Symmetries in Axionic Extensions of the SSM
hep-lat/9209007;hep-lat;0;17;;UKQCD Collaboration,S.P.Booth,A.Hulsebos,A.C.Irving,A.McKerrell,C.Michael,P.S.Spencer,P.W.Stephenson;SU(2) Potentials from Large Lattices
hep-lat/9209008;hep-lat;1;13;hep-lat/9205016;UKQCD Collaboration,S.P.Booth,D.S.Henty,A.Hulsebos,A.C.Irving,C.Michael,P.W.Stephenson;The Running Coupling from SU(3) Lattice Gauge Theory
hep-ph/9209209;hep-ph;0;0;;V.Sahni;The Large Scale Structure of the Universe: Theory {\it vs.} Observations
hep-ph/9209210;hep-ph,hep-th;0;43;;J.Preskill,A.Vilenkin;Decay of Metastable Topological Defects
hep-ph/9209211;hep-ph;0;0;;D.London,C.P.Burgess;Loop Calculations with Anomalous Gauge Boson Couplings
cond-mat/9209002;cond-mat;0;18;;F.H.L.Essler,V.E.Korepin,K.Schoutens;New Exactly Solvable Model of Strongly Correlated Electrons Motivated by High T_c Superconductivity
hep-th/9209011;hep-th;9;45;hep-th/9108004,hep-th/9109005,hep-th/9109032,hep-th/9111048,hep-th/9112009,hep-th/9201005,hep-th/9201056,hep-th/9201071,hep-th/9201072;Y.-S.Wu,C.-J.Zhu;The Complete Structure of the Cohomology Ring and Associated Symmetries in $D=2$ String Theory
hep-th/9209012;hep-th;0;23;;J.Russo,L.Susskind,L.Thorlacius;Cosmic Censorship in Two-Dimensional Gravity
cond-mat/9209003;cond-mat;0;12;;E.Hernandez-Garcia,T.Ala-Nissila,M.Grant;Interface roughening with a time-varying external driving force
cond-mat/9209004;cond-mat;0;15;;A.J.Schofield,J.M.Wheatley;Combination Rules, Charge Symmetry, and Hall Effect in Cuprates
astro-ph/9209001;astro-ph;0;0;;A.C.Robin,M.Creze,V.Mohan;The Radial Structure of the Galactic Disc
hep-th/9209013;hep-th;7;87;hep-th/9108004,hep-th/9108026,hep-th/9109027,hep-th/9109032,hep-th/9111001,hep-th/9112062,hep-th/9205107;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;The String Universe: High $T_c$ Superconductor or Quantum Hall Conductor?
hep-ph/9209212;hep-ph;0;22;;F.Cooper;Dynamical Approach to Pair Production from Strong Fields
hep-ph/9209213;hep-ph;1;39;hep-ph/9310316;J.Chyla,A.Kataev;Next-to-next-to-leading order QCD analysis of the Gross-Llewellyn Smith sum rule and the higher twist effects
hep-lat/9209009;hep-lat;0;10;;A.Kocic,J.B.Kogut,K.C.Wang;Monopole Percolation and The Universality Class of the Chiral Transition in Four Flavor Noncompact Lattice QED
hep-lat/9209010;hep-lat;0;0;;A.Kocic,J.B.Kogut,M.-P.Lombardo;Universal Properties of Chiral Simmetry Breaking
hep-ph/9209214;hep-ph;0;35;;K.S.Babu,Q.Shafi;From Fermion Mass Matrices to Neutrino Oscillations
hep-ph/9209215;hep-ph;0;29;;K.S.Babu,R.N.Mohapatra;Predictive Neutrino Spectrum in Minimal $SO(10)$ Grand Unification
hep-ph/9209216;hep-ph;0;0;;D.Bowser-Chao,D.L.Dzialo;A Comparison of the Use of Binary Decision Trees and Neural Networks in Top Quark Detection
hep-lat/9209011;hep-lat,cond-mat;0;83;;P.Butera,M.Comi;A quantitative study of the Kosterlitz-Thouless phase transition in a system of two-dimensional plane rotators ( XY model ) by high temperature expansions through $β^{20}$
hep-th/9209014;hep-th;0;14;;J.Shiraishi;Free Boson Representation of $U_q(\hat {sl_2})$
hep-th/9209015;hep-th;0;25;;A.Kato,Y.-H.Quano,J.Shiraishi;Free Boson Representation of $q$-Vertex Operators and their Correlation Functions
hep-th/9209016;hep-th;0;0;;A.Sen;Quantization of Dyon Charge and Electric-Magnetic Duality in String Theory
hep-th/9209017;hep-th;0;33;;G.Papadopoulos;The geometry of supersymmetric coset models and superconformal algebras
gr-qc/9209002;gr-qc;0;0;;D.Garfinkle;Results on exact solutions of low energy string theory
hep-ph/9209217;hep-ph;0;10;;B.Mueller,M.H.Thoma;Vacuum Polarization and the Electric Charge of the Positron
cond-mat/9209005;cond-mat;0;17;;H.Monien;Aspects of Spin Dynamics in the Cuprate Superconductors
cond-mat/9209006;cond-mat;0;39;;A.J.Millis,H.Monien;Spin Gaps and Spin Dynamics in La_{2-x}Sr_xCuO_4 and YBa_2Cu_3O7_δ
hep-th/9209018;hep-th;1;78;hep-th/9112047;R.Schimmrigk;The Construction of Mirror Symmetry
hep-th/9209019;hep-th,cond-mat;0;25;;T.Inami,S.Odake;Continuum Limit of Spin-1 Chain (the only change is added references)
hep-ph/9209218;hep-ph;0;45;;E.Gotsman,E.M.Levin,U.Maor;A Quantitative Investigation of the Pomeron
hep-lat/9209012;hep-lat;1;32;hep-lat/9201004;C.B.Lang,U.Winkler;Rotational Symmetry and Regularization Dependence in the $Φ^4_4$-Model
hep-lat/9209013;hep-lat,cond-mat;0;38;;M.Hasenbusch,K.Pinn;Surface Tension, Surface Stiffness, and Surface Width of the 3-dimensional Ising Model on a Cubic Lattice
hep-th/9209020;hep-th,hep-ph;0;0;;I.Antoniadis,K.Benakli;Fractionally Charged Particles and Supersymmetry Breaking in 4D Strings
hep-ph/9209219;hep-ph;0;50;;J.Blümlein,G.J.van Oldenborgh,R.Rückl;QCD and QED Corrections to Higgs Boson Production in Charged Current $ep$ Scattering
hep-ph/9209220;hep-ph;1;43;hep-ph/9206203;J.Lopez,D.Nanopoulos,H.Pois;Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model
hep-ph/9209221;hep-ph;0;20;;E.Ma;Possible Finiteness of the Higgs-Boson Mass Renormalization
hep-th/9209021;hep-th;4;30;hep-th/9109007,hep-th/9109048,hep-th/9112004,hep-th/9201054;A.A.Bytsenko,E.Elizalde,S.D.Odintsov nd S.Zerbini;Laurent Series Representation for the Open Superstring Free Energy
math/9209202;math.LO;0;0;;R.Dougherty,T.Jech;Finite left-distributive algebras and embedding algebras\endtitle 
math/9209203;math.LO;0;0;;A.Blass;Cardinal Characteristics and the Product of Countably Many Infinite Cyclic Groups
cond-mat/9209007;cond-mat;0;0;;R.J.Gooding,A.Mailhot;Spin texture in weakly doped $Cu0_2$ planes explaining magnetic correlation length and Raman scattering experiments
hep-th/9209022;hep-th;0;0;;S.Hikami,E.Brézin;Perturbative analysis of an n-Ising model on a random surface
hep-th/9209023;hep-th;0;0;;A.A.Tseytlin;String vacuum backgrounds with covariantly constant null Killing vector and 2d quantum gravity
hep-th/9209024;hep-th;0;0;;T.Hollowood;Quantum Soliton Mass Corrections in SL(N) Affine Toda Theory
gr-qc/9209003;gr-qc,hep-th;0;12;;G.Fülöp;Transformations and BRST-Charges in 2+1 Dimensional Gravitation
cond-mat/9209008;cond-mat;0;15;;V.L.Libero,D.L.Cox;A Simple Model for Coupled Magnetic and Quadrupolar Instabilities in Uranium Heavy-Fermion Materials
hep-lat/9209014;hep-lat,hep-ph;0;0;;C.Michael;Glueballs and Hybrid Mesons
hep-th/9209025;hep-th;0;0;;S.R.Das,S.K.Rama;Renormalization of Couplings in Embedded Random Surfaces
hep-th/9209026;hep-th;0;0;;D.Bazeia;Gauge Invariance in Chern-Simons Systems
hep-th/9209027;hep-th;0;0;;P.F.Bedaque,I.Horvath,S.G.Rajeev;Two dimensional baryons in the large N limit
hep-lat/9209015;hep-lat;0;13;;M.L.Laursen;Chern-Simons term and Topological Charge on the Lattice
hep-th/9209028;hep-th;0;30;;P.Menotti,G.Modanese,D.Seminara;The radial gauge propagators in quantum gravity
hep-th/9209029;hep-th;0;0;;A.Honecker;A Note on the Algebraic Evaluation of Correlators in Local Chiral Conformal Field Theory
hep-th/9209030;hep-th;0;0;;W.Eholzer,A.Honecker,R.Huebel;Representations of $N=1$ Extended Superconformal Algebras with Two Generators
hep-ph/9209222;hep-ph;0;0;;D.London,C.P.Burgess;Loops, Cutoffs and Anomalous Gauge Boson Couplings
funct-an/9209001;funct-an,math.FA;0;0;;A.Bressan,G.Crasta;Extremal Selections of Multifunctions Generating a Continuous Flow
hep-ph/9209223;hep-ph;0;0;;E.Nardi;Z', new fermions and flavor changing processes, constraints on E$_6$ models from $μ$ --> eee
math/9209204;math.LO;0;0;;M.Kojman;$μ$-complete Souslin trees on $μ^+$
hep-lat/9209016;hep-lat;0;27;;M.Hasenbusch;Direct Monte Carlo Measurement of the Surface Tension in Ising Models
hep-ph/9209224;hep-ph,hep-th;0;0;;A.H.Chamseddine,G.Felder,J.Fröhlich;Grand Unification in Non-Commutative Geometry
hep-th/9209031;hep-th,gr-qc;0;0;;J.E.Nelson,T.Regge;Invariants of 2+1 Quantum Gravity
hep-th/9209032;hep-th;0;13;;C.Bachas,M.Porrati;Pair Creation of Open Strings in an Electric Field
hep-ph/9209225;hep-ph,astro-ph;0;14;;L.M.Krauss,D.Schramm;Angular Diameters as a Probe of a Cosmological Constant and $Ω$
hep-th/9209033;hep-th;0;11;;R.Brustein,B.Ovrut;Non-perturbative interactions in string theory
hep-th/9209034;hep-th;3;51;hep-th/9108004,hep-th/9112036,hep-th/9201056;P.Bouwknegt,J.McCarthy,K.Pilch;Semi-infinite cohomology in conformal field theory and 2d gravity
hep-th/9209035;hep-th;0;18;;W.Kalau;BRST Quantization of 2d-Yang Mills Theory with Anomalies
gr-qc/9209004;gr-qc,astro-ph;0;0;;E.Malec,N.Ó.Murchadha;A Quasilocal Test of the Finiteness of the Universe
hep-th/9209036;hep-th;0;0;;J.Avan,A.Jevicki;Interacting Theory of Collective and Topological Fields in 2 Dimensions
cond-mat/9209009;cond-mat;0;60;;J.Ferrer;Spin liquid phase for the frustrated Quantum Heisenberg Antiferromagnet on a square lattice
hep-ph/9209226;hep-ph;0;0;;J.Madore;On a Noncommutative Extension of Electrodynamics
hep-ph/9209227;hep-ph;0;19;;V.Jain;The 3d effective field theory of the high temperature abelian Higgs model
hep-ph/9209228;hep-ph;0;0;;K.Kang,A.R.White;Color--Sextet Quark Condensation In QCD
hep-th/9209037;hep-th;2;33;hep-th/9110015,hep-th/9203024;E.Bergshoeff,A.Sevrin,X.Shen;A Derivation of the BRST Operator for Non-Critical W-Strings
hep-th/9209038;hep-th;0;0;;E.F.Moreno;Functional determinant and Green functions for a fermionic gauge theory on the disk
cond-mat/9209010;cond-mat;0;22;;H.-wen.Xi,J.D.Gunton,J.Vinals;Study of spiral pattern formation in Rayleigh-Benard convection
cond-mat/9209011;cond-mat;0;9;;E.J.Mele,S.C.Erwin;Anisotropic Pairing on a Three-Band Fermi Surface for $A_3{\rm C}_{60}$
hep-th/9209039;hep-th;0;4;;J.Rogers,D.Spector;Quantum Mechanics with Explicit Time Dependence
hep-ph/9209229;hep-ph;0;0;;F.C.Adams,K.Freese,J.S.Langer;Baryon Number Diffusion and Instabilities in the Quark/Hadron Phase Transition
hep-lat/9209017;hep-lat;1;28;hep-th/9503230;C.Holm,W.Janke;Finite-Size Scaling Study of the Three-Dimensional Classical Heisenberg Model
cond-mat/9209012;cond-mat;0;21;;F.H.L.Essler,V.E.Korepin,K.Schoutens;Completeness of the SO(4) Extended Bethe Ansatz for the One-Dimensional Hubbard Model
astro-ph/9209002;astro-ph;0;30;;K.Tomisaka,J.N.Bregman;Extended Hot Gas Halos Around Starburst Galaxies
alg-geom/9209001;alg-geom,math.AG;0;0;;R.Brussee;On the $(-1)$-curve conjecture of Friedman and Morgan
hep-th/9209040;hep-th,alg-geom,math.AG;0;0;;B.Dubrovin;Integrable Systems and Classification of 2-dimensional Topological Field Theories
cond-mat/9209013;cond-mat;0;10;;B.Friedman,K.Harigaya;Quantum Lattice Fluctuations and Luminescence in C_60
astro-ph/9209003;astro-ph,gr-qc,hep-ph;0;114;;D.H.Lyth,A.A.Liddle;The Spectral Index in the CDM Cosmogony
hep-th/9209041;hep-th;4;21;hep-th/9109054,hep-th/9112009,hep-th/9204019,hep-th/9206035;L.Bonora,C.S.Xiong;Matrix models without scaling limit
hep-th/9209042;hep-th;0;0;;T.Gannon;Partition Functions for Heterotic WZW Conformal Field Theories
hep-th/9209043;hep-th;0;0;;T.Gannon;WZW Commutants, Lattices, and Level 1 Partition Functions
hep-ph/9209230;hep-ph;0;26;;J.R.Cudell,B.Margolis;Can perturbative QCD predict a substantial part of diffractive LHC/SSC physics?
hep-th/9209044;hep-th,gr-qc;0;0;;A.H.Chamseddine,G.Felder,J.Fröhlich;Gravity in Non-Commutative Geometry
hep-th/9209045;hep-th;2;24;hep-th/9109005,hep-th/9202050;R.Brustein,B.Ovrut;Stringy Instantons
cond-mat/9209014;cond-mat;0;19;;W.Li,G.Vidali;Metal Adatom Induced Corrugation of Cu(001)
cond-mat/9209015;cond-mat;0;14;;W.Li,G.Vidali;Growth of Metastable High-Order Commensurate Overlayers of Pb on Cu(001)
hep-ph/9209231;hep-ph;0;26;;C.Bruno,J.Prades;Rare Kaon Decays in the $1/N_c$-Expansion
hep-ph/9209232;hep-ph;2;119;hep-ph/9203220,hep-ph/9206203;V.Barger,M.S.Berger,P.Ohmann;Supersymmetric Grand Unified Theories: Two Loop Evolution of Gauge and Yukawa Couplings
hep-th/9209046;hep-th;0;0;;A.Polyakov;Conformal Turbulence
hep-th/9209047;hep-th,astro-ph,gr-qc;0;15;;H.J.de Vega,A.V.Mikhailov,N.Sanchez;Exact String Solutions in 2+1-Dimensional De Sitter Spacetime
cond-mat/9209016;cond-mat;0;16;;O.Biham,L.-W.Chen,G.Vidali;Models for Monolayers Adsorbed on a Square Substrate
hep-ph/9209233;hep-ph;2;36;hep-ph/9203201,hep-ph/9203203;M.Carena,C.E.M.Wagner;On the Finite Temperature Effective Potential in Scalar QED with N Flavors
hep-th/9209048;hep-th;0;7;;D.S.Freed;Locality and Integration in Topological Field Theory
hep-ph/9209234;hep-ph;0;16;;Z.Huang;On the Anomalous Discrete Symmetry
hep-ph/9209235;hep-ph;0;59;;Z.Huang;The Measure of Strong CP Violation
gr-qc/9209005;gr-qc,hep-th;0;22;;D.S.Goldwirth,M.J.Perry,T.Piran;The Loss of Unitarity in the Vicinity of a Time Machine
hep-th/9209049;hep-th,hep-lat;2;25;hep-th/9203019,hep-th/9207065;S.Dalley,I.Klebanov;String Spectrum of 1+1-Dimensional Large N QCD with Adjoint Matter
hep-th/9209050;hep-th;0;0;;Al.R.Kavalov;Extrinsic Geometry Sensitive Bosonic String Theory
hep-lat/9209018;hep-lat;0;20;;C.Gong;Lyapunov Exponent of SU(3) Gauge Theory
math/9209205;math.LO;0;0;;J.Brendle,H.Judah;Perfect sets of random reals
math/9209206;math.LO;0;0;;J.Brendle;Amoeba-absoluteness and projective measurability
hep-lat/9209019;hep-lat;0;20;;A.M.Green,C.Michael,J.E.Paton;Multi-quark energies in QCD
hep-ph/9209236;hep-ph;0;0;;P.Gondolo,G.Gelmini,S.Sarkar;Cosmic Neutrinos from Unstable Relic Particles
hep-ph/9209237;hep-ph;0;36;;G.Valencia;Anomalous Gauge-Boson Couplings at Hadron Supercolliders
hep-th/9209051;hep-th;0;17;;S.Govindarajan;On Physical States in c<1 String Theory
hep-th/9209052;hep-th;0;0;;M.Gasperini,J.Maharana,G.Veneziano;Boosting Away Singularities from Conformal String Backgrounds
hep-th/9209053;hep-th;0;0;;E.Carlen,E.Lieb;Optimal Hypercontractivity for Fermi Fields and Related Non-Commutative Integration
hep-ph/9209238;hep-ph,astro-ph;0;19;;W.D.Garretson,G.B.Field,S.M.Carroll;Primordial magnetic fields from pseudo-Goldstone bosons
hep-ph/9209239;hep-ph;1;16;hep-ph/9203225;P.Cho,H.Georgi;Electromagnetic Interactions in Heavy Hadron Chiral Theory
hep-ph/9209240;hep-ph;0;12;;M.B.Voloshin;Summing One-Loop Graphs at Multi-Particle Threshold
hep-ph/9209241;hep-ph;0;16;;J.F.Amundson,C.G.Boyd,E.Jenkins,M.Luke,A.V.Manohar,J.L.Rosner,M.J.Savage,M.B.Wise;Radiative $D^*$ Decay Using Heavy Quark and Chiral Symmetry
hep-ph/9209242;hep-ph;0;13;;R.F.Lebed;Meson Mass Splittings in the Nonrelativistic Model
math/9209207;math.LO;0;0;;A.Landver;Finite Combinations of Baire Numbers
gr-qc/9209006;gr-qc;0;20;;B.Grubisic,V.Moncrief;Asymptotic Behavior of the $T^3 ×R$ Gowdy Spacetimes
hep-th/9209054;hep-th,math.QA,nlin.SI,solv-int;0;0;;P.P.Kulish,E.K.Sklyanin;Algebraic Structures Related to Reflection Equations
hep-th/9209055;hep-th,gr-qc;16;84;hep-th/9203054,hep-th/9203059,hep-th/9203083,hep-th/9204026,hep-th/9204072,hep-th/9205028,hep-th/9205069,hep-th/9205089,hep-th/9206020,hep-th/9206071,hep-th/9206087,hep-th/9207006,hep-th/9207034,hep-th/9207077,hep-th/9207095,hep-th/9207105;J.A.Harvey,A.Strominger;Quantum Aspects of Black Holes
hep-th/9209056;hep-th;0;0;;D.Dalmazi;Tree Amplitudes in Noncritical $N=2$ Strings
gr-qc/9209007;gr-qc;0;52;;E.Calzetta,M.Sakellariadou;Semiclassical Effects and the Onset of Inflation
cond-mat/9209017;cond-mat;0;16;;M.Arjunwadkar,G.Baskaran,R.Basu,V.N.Muthukumar;Numerical Study of the Wheatley-Hsu-Anderson Interlayer Tunneling mechanism of High $T_c$ Superconductivity
hep-ph/9209243;hep-ph;0;0;;J.E.Kim;The $μ$ Problem and the Invisible Axion
hep-ph/9209244;hep-ph;1;18;hep-ph/9207278;H.Georgi;Physics from Vacuum Alignment in A Technicolor Model
hep-th/9209057;hep-th;0;0;;A.Jevicki,J.P.Rodrigues,A.J.van Tonder;Scattering States and Symmetries in the Matrix Model and Two Dimensional String Theory
cond-mat/9209018;cond-mat;0;0;;A.Montorsi,A.Pelizzola;Fermi-linearization scheme for itinerant electrons with Clifford variables
cond-mat/9209019;cond-mat,hep-th;0;25;;Y.-C.Tsai,Y.Shapir;Kinetic Roughening in Surfaces of Crystals Growing on Disordered Substrates
hep-ph/9209245;hep-ph;0;52;;A.Cohen,A.Nelson;Supersymmtric Baryogenesis
hep-th/9209058;hep-th,gr-qc;4;46;hep-th/9111056,hep-th/9201059,hep-th/9201061,hep-th/9203059;J.Preskill;Do Black Holes Destroy Information?
hep-th/9209059;hep-th;1;42;hep-th/9111018;G.Aldazabal,I.Allekotte,E.Andrés,C.Núñez;Nondiagonal $CP_m$ Coset Models and their PoincarÉ Polynomials
hep-th/9209060;hep-th,math.QA;0;0;;P.P.Kulish;Quantum Groups, $q$-Oscillators and Covariant Algebras
hep-ph/9209246;hep-ph,cond-mat;0;0;;S.Chakravarty,A.M.Srivastava;Vortex Production in a First Order Phase-Transition at Finite Temperature
cond-mat/9209020;cond-mat;0;24;;E.Canessa,V.L.Nguyen;Non-Linear I-V Characteristics of Double Schottky Barriers and Polycrystalline Semiconductors
cond-mat/9209021;cond-mat;0;13;;E.Canessa,A.Calmetta;Growth Model of Au Films on Ru(001)
hep-th/9209061;hep-th;2;31;hep-th/9108006,hep-th/9110057;S.Mizoguchi;Rational Conformal Field Theory and Multi-Wormhole Partition Function in 3-dimensional Gravity
hep-ph/9209247;hep-ph;0;22;;R.Casalbuoni,A.Deandrea,N.D.Bartolomeo,R.Gatto,F.Feruglio,G.Nardulli;Estimates with an Effective Chiral Lagrangian for Heavy Mesons
hep-th/9209062;hep-th;0;37;;P.Gregoire,M.Henneaux;Hamiltonian BRST-anti-BRST Theory
hep-ph/9209248;hep-ph;0;34;;R.Casalbuoni,A.Deandrea,N.D.Bartolomeo,R.Gatto,F.Feruglio,G.Nardulli;Light Vector Resonances in the Effective Chiral Lagrangian for Heavy Mesons
hep-ph/9209249;hep-ph;0;13;;P.J.O'Donnell,H.K.K.Tung;Exclusive Rare Decay $B→K^∗γ$
hep-th/9209063;hep-th;0;0;;M.Temple-Raston,D.Alexander;Differential cross-sections and escape plots for low energy $SU(2)$ BPS magnetic monopole dynamics
hep-ph/9209250;hep-ph;1;23;hep-ph/9203220;G.W.Anderson,S.Raby,S.Dimopoulos,L.Hall;Precise predictions for mt, Vcb and tan
hep-th/9209064;hep-th;1;31;hep-th/9112009;X.Shen;Quantum Dilaton Gravity in the Light-cone Gauge
hep-ph/9209251;hep-ph;0;0;;R.M.Godbole,P.Roy,X.Tata;Tau Signals of R-parity breaking at LEP 200
hep-th/9209065;hep-th;0;16;;E.Bergshoeff,H.J.Boonstra,M.de Roo;Realisations of $W_3$ Symmetry
hep-ph/9209252;hep-ph;0;17;;T.S.Evans;A New Time Contour for Equilibrium Real-Time Thermal Field Theories (7 characters altered for email)
hep-ph/9209253;hep-ph;0;23;;T.S.Evans;Thermal Bosonic Green Functions Near Zero Energy (6 characters removed for email)
hep-lat/9209020;hep-lat,hep-th;5;79;hep-th/9111003,hep-th/9205043,hep-lat/9205018,hep-th/9205100,hep-lat/9207008;M.Bowick,P.Coddington,L.Han,G.Harris,E.Marinari;The Phase Diagram of Fluid Random Surfaces with Extrinsic Curvature
cond-mat/9209022;cond-mat;0;0;;A.Pelizzola,C.Topi;Generalized Coherent States for Dynamical Superalgebras
cond-mat/9209023;cond-mat;0;0;;C.Buzano,A.Pelizzola;Multicritical Points And Reentrant Phenomenon In The BEG Model
cond-mat/9209024;cond-mat;0;0;;V.Privman;Discrete to Continuous-Time Crossover due to Anisotropy in Diffusion-Limited Two-Particle Annihilation Reactions
hep-th/9209066;hep-th,cond-mat;0;0;;S.Rao;An Anyon Primer
hep-th/9209067;hep-th;0;0;;C.N.Pope,X.J.Wang;A Note on Representations of the $w_∞$ Algebra
hep-th/9209068;hep-th;9;26;hep-th/9108001,hep-th/9108026,hep-th/9109026,hep-th/9110054,hep-th/9111038,hep-th/9111040,hep-th/9112070,hep-th/9201015,hep-th/9205046;S.Kar,A.Kumar,G.Sengupta;Hidden Isometry in a Chiral Gauged WZW Model
hep-ph/9209254;hep-ph;0;10;;M.H.Austern;Can a strongly interacting Higgs boson rescue SU(5)?
cond-mat/9209025;cond-mat;0;0;;J.T.Gammel,D.K.Campbell;Relaxed Excited State Geometries in a Peierls-Hubbard Model for Polyenes
cond-mat/9209026;cond-mat;0;0;;J.T.Gammel,D.K.Campbell,E.Y.Loh Jr;Extracting Infinite System Properties from Finite Size Clusters: `Phase Randomization/Boundary Condition Averaging'
hep-ph/9209255;hep-ph;0;0;;M.A.Luty,R.Sundrum;Technicolor Theories with Negative S
cond-mat/9209027;cond-mat;0;0;;J.T.Gammel,K.Y.A.Saxena,A.R.Bishop,H.Röder;Electron-Phonon Driven Spin Frustration in Multi-Band Hubbard Models: MX Chains and Oxide Superconductors
cond-mat/9209028;cond-mat;0;17;;L.A.Worl,S.C.Huckett,B.I.Swanson,A.Saxena,A.R.Bishop,J.T.Gammel;Photoinduced charge separation in Q1D heterojunction materials: Evidence for electron-hole pair separation in mixed-halide $MX$ solids
hep-ph/9209256;hep-ph;0;22;;J.Schechter,A.Subbaraman;Role of Light Vector Mesons in the Heavy Particle Chiral Lagrangian
hep-th/9209069;hep-th,alg-geom,gr-qc,math.QA;0;0;;B.Broda;Quantum theory of non-abelian differential forms and link polynomials
hep-th/9209070;hep-th,gr-qc;0;13;;R.Gregory,J.A.Harvey;Black Holes with a Massive Dilaton
hep-th/9209071;hep-th;0;0;;E.F.Moreno;Coset Models in Monopole Backgrounds
cond-mat/9209029;cond-mat;2;24;cond-mat/9205014,cond-mat/9205016;K.Harigaya;Polaron excitations in fullerenes: Theory as pi-conjugated systems
hep-ph/9209257;hep-ph,nucl-th;0;12;;S.Weinberg;Three-Body Interactions Among Nucleons and Pions
hep-ph/9209258;hep-ph;0;8;;G.W.Anderson;Collapsing Sub-Critical Bubbles
hep-ph/9209259;hep-ph;0;47;;R.Foot,H.Lew,R.R.Volkas;Electric Charge Quantization
hep-ph/9209260;hep-ph;0;0;;X.G.He,J.P.Ma,B.H.J.McKellar;CP Violating Form Factors for Three Gauge Boson Vertex in the Two Higgs Doublet and Left-Right symmetric Models
hep-ph/9209261;hep-ph;0;44;;J.Bijnens,G.Ecker,J.Gasser;Radiative Semileptonic Kaon Decays
hep-th/9209072;hep-th;0;16;;M.J.Perry,E.Teo;BRS and Anti-BRS Symmetry in Topological Yang--Mills Theory
hep-th/9209073;hep-th,math.QA;0;33;;L.Rozansky,H.Saleur;Reidemeister torsion, the Alexander polynomial and $U(1,1)$ Chern-Simons theory
hep-th/9209074;hep-th;0;6;;A.Morozov;Pair Correlator in the Itzykson-Zuber Integral
hep-ph/9209262;hep-ph;2;27;hep-ph/9203225,hep-ph/9204207;H.Y.Cheng,C.Y.Cheung,G.L.Lin,Y.C.Lin,T.M.Yan,H.L.Yu;Chiral Lagrangians for Radiative Decays of Heavy Hadrons
hep-lat/9209021;hep-lat;1;14;hep-lat/9204016;M.Baeker,T.Kalkreuter,G.Mack,M.Speh;Neural multigrid for gauge theories and other disordered systems
hep-ph/9209263;hep-ph;0;55;;J.F.Amundson,J.L.Rosner;Heavy Quark Symmetry Violation in Semileptonic Decays of D Mesons
hep-th/9209075;hep-th;6;23;hep-th/9111062,hep-th/9202058,hep-th/9202060,hep-th/9203024,hep-th/9204038,hep-th/9205013;A.Deckmyn;On the generalized Miura transformation
hep-th/9209076;hep-th;0;43;;F.Falceto,K.Gawedzki;Lattice Wess-Zumino-Witten Model and Quantum Groups
hep-th/9209077;hep-th,alg-geom,funct-an,math.AG,math.FA;0;23;;A.Turbiner;On polynomial solutions of differential equations
hep-th/9209078;hep-th;0;7;;F.Gieres;On the holomorphic factorization for superconformal fields
hep-th/9209079;hep-th,alg-geom,funct-an,math.AG,math.FA;0;19;;A.Turbiner;Lie-algebraic approach to the theory of polynomial solutions. I. Ordinary differential equations and finite-difference equations in one variable
hep-th/9209080;hep-th,alg-geom,funct-an,math.AG,math.FA;0;10;;A.Turbiner;Lie-algebraic approach to the theory of polynomial solutions. II. Differential equations in one real and one Grassmann variables and 2x2 matrix differential equations
hep-th/9209081;hep-th;2;39;hep-th/9109005,hep-th/9202050;R.Brustein,B.Ovrut;Non-Perturbative Effects in 2-D String Theory or Beyond the Liouville Wall
hep-th/9209082;hep-th,alg-geom,funct-an,math.AG,math.FA;0;25;;A.Turbiner;Lie-algebraic approach to the theory of polynomial solutions. III. Differential equations in two real variables and general outlook
hep-th/9209083;hep-th;0;9;;S.L.Shatashvili;Correlation Functions in The Itzykson-Zuber Model
hep-th/9209084;hep-th;0;0;;A.Das,C.A.P.Galvao;Self-Duality and the KdV Hierarchy
hep-th/9209085;hep-th;2;66;hep-th/9111016,hep-th/9203066;S.Cecotti,C.Vafa;Ising Model and $N=2$ Supersymmetric Theories
hep-th/9209086;hep-th;0;27;;D.M.Gitman,A.V.Saa;Quantization of Spinning Particle with Anomalous Magnetic Momentum
hep-lat/9209022;hep-lat;0;35;;G.P.Lepage,P.B.Mackenzie;On the Viability of Lattice Perturbation Theory
hep-ph/9209264;hep-ph;0;23;;S.Y.Choi,H.S.Song;Exclusive heavy meson pair production by $γγ$ collision in heavy quark effective theory
hep-ph/9209265;hep-ph;0;0;;F.T.Brandt,J.Frenkel;The 3-graviton vertex function in thermal quantum gravity
hep-ph/9209266;hep-ph;0;8;;P.Labelle;Nrqed in Bound States: Applying Renormalization to an Effective Field Theory
hep-th/9209087;hep-th;0;0;;R.Perret;Three dimensional field theories from infinite dimensional lie algebras
hep-ph/9209267;hep-ph;0;21;;D.Chang,W.-Y.Keung,I.Phillips;CP violation in top pair production at an e^+e^- collider
hep-th/9209088;hep-th,hep-ph;0;33;;M.Hindmarsh,R.Holman,T.W.Kephart,T.Vachaspati;Generalized Semilocal Theories and Higher Hopf Maps
hep-th/9209089;hep-th;0;0;;H.B.Gao;On Renormalization Group Flow In Matrix Model
gr-qc/9209008;gr-qc,hep-th;0;12;;E.E.Donets,D.V.Gal'tsov;Continuous Family of Einstein-Yang-Mills Wormholes
hep-th/9209090;hep-th;0;0;;S.Schrans;Generalised Virasoro Constructions from Affine Inonu-Wigner Contractions
hep-ph/9209268;hep-ph;1;46;hep-ph/9204237;A.F.Falk,M.Neubert;Second Order Power Corrections in the Heavy Quark Effective Theory I. Formalism and Meson Form Factors
hep-ph/9209269;hep-ph;0;33;;A.F.Falk,M.Neubert;Second Order Power Corrections in the Heavy Quark Effective Theory II. Baryon Form Factors
hep-ph/9209270;hep-ph;0;5;;M.B.Voloshin;Comment on "Summing One-Loop Graphs at Multi-Particle Threshold"
hep-th/9209091;hep-th,hep-lat;0;8;;D.V.Boulatov;Local symmetry in the Kazakov-Migdal gauge model
hep-ph/9209271;hep-ph;0;21;;M.Neubert,Z.Ligeti,Y.Nir;QCD Sum Rule Analysis of the Subleading Isgur-Wise Form Factor $χ_2(v\cdot v')$
hep-lat/9209023;hep-lat;0;37;;V.G.Bornyakov,V.K.Mitrjushkin,M.Müller-Preussker;Modified $U(1)$ lattice gauge theory: towards realistic lattice QED
astro-ph/9209004;astro-ph;0;26;;V.Faraoni,S.Sonego;On the Tail Problem in Cosmology
cond-mat/9209030;cond-mat;0;17;;A.H.C.Neto,A.O.Caldeira;An alternative approach for the dynamics of polarons in one dimension
hep-ph/9209272;hep-ph;2;26;hep-ph/9204206,hep-ph/9205228;M.A.Nowak,M.Rho,I.Zahed;Chiral effective action with heavy quark symmetry
hep-ph/9209273;hep-ph,hep-th;0;0;;P.F.Bedaque,A.Das;Feynman Parametrization and the Degenerate Electron Gas
hep-ph/9209274;hep-ph;0;23;;V.Rieckert;Note on Tests of the Factorization Hypothesis and the Determination of Meson Decay Constants
astro-ph/9209005;astro-ph,hep-ph;0;10;;G.Raffelt,G.Sigl;Neutrino Flavor Conversion in a Supernova Core
gr-qc/9209009;gr-qc;0;0;;D.Brill;Euclidean Maxwell-Einstein Theory
hep-th/9209092;hep-th;0;0;;T.A.Larsson;Vect(N) Invariants and Quantum Gravity
hep-th/9209093;hep-th;0;11;;H.G.Kausch;W-algebras arising as chiral algebras of conformal field theory
hep-th/9209094;hep-th;0;15;;B.Durhuus,T.Jonsson;On subdivision invariant actions for random surfaces
hep-th/9209095;hep-th;0;18;;G.Papadopoulos,B.Spence;The phase space of the Wess-Zumino-Witten model
hep-th/9209096;hep-th;0;0;;M.Nolasco,C.Reina;Topological Observables in Semiclassical Field Theories
hep-th/9209097;hep-th,hep-lat;0;8;;B.Rusakov;From hermitian matrix model to lattice gauge theory
hep-ph/9209275;hep-ph;0;25;;D.-P.Min,Y.Oh,B.-Y.Park,M.Rho;Soliton Structure of Heavy Baryons
hep-ph/9209276;hep-ph,astro-ph;0;0;;G.Raffelt,G.Sigl,L.Stodolsky;Non-Abelian Boltzmann Equation for Mixing and Decoherence
gr-qc/9209010;gr-qc,astro-ph;0;26;;L.S.Finn;Detection, Measurement and Gravitational Radiation
hep-th/9209098;hep-th;1;17;hep-th/9203029;K.Haller,E.Lim-Lombridas;Anyonic States in Chern-Simons Theory
hep-th/9209099;hep-th;1;0;hep-th/9201056;T.Lada,J.Stasheff;Introduction to sh Lie algebras for physicists
hep-ph/9209277;hep-ph;2;21;hep-ph/9908362,hep-ph/9908363;E.Bagan,P.Ball,P.Gosdzinsky;The Isgur-Wise Function to $O(α_s)$ from Sum Rules in the Heavy Quark Effective Theory
hep-ph/9209278;hep-ph;0;13;;M.Gronau,S.Wakaizumi;On Testing V-A in Lambda_b Decays
hep-ph/9209279;hep-ph;0;29;;M.Gronau;Large Penguin effects in the CP Asymmetry of B0d ->pi+pi-
hep-ph/9209280;hep-ph;0;0;;J.E.Horvath;Stable diquark matter ?
math/9209208;math.LO;0;8;;M.Scheepers;Meager-nowhere dense games (III): Remainder strategies
math/9209209;math.LO;0;0;;G.Melles;Some Natural Internal Forcing Schemata Extending ZFC
math/9209210;math.LO;0;0;;G.Melles;$^*$Forcing
math/9209211;math.FA;0;0;;N.Gronbaek,B.E.Johnson,G.A.Willis;Amenability of Banach algebras of compact operators
math/9209212;math.FA;0;0;;S.J.Montgomery-Smith;The Distribution of Non-Commutative Rademacher Series
math/9209213;math.FA;0;0;;J.Bastero,J.Buernes,A.Pena;The theorems of Caratheodory and Gluskin for $0<p<1$
math/9209214;math.FA;0;19;;V.D.Milman,N.Tomczak-Jaegermann;Asymptotic $l_p$ spaces and bounded distortions
math/9209215;math.FA;0;0;;W.B.Johnson,G.Schechtman;Computing p-summing norms with few vectors
gr-qc/9209011;gr-qc,hep-th;1;15;hep-th/9109006;S.Carlip;The Modular Group, Operator Ordering, and Time in (2+1)-Dimensional Gravity
hep-ph/9209281;hep-ph,cond-mat;0;0;;A.M.Srivastava;Numerical Study of the Lowest Energy Configurations for Global String-Antistring Pairs
hep-th/9209100;hep-th;1;33;hep-th/9201010;A.Mironov,S.Pakuliak;On the Continuum Limit of the Conformal Matrix Models
hep-lat/9209024;hep-lat;3;22;hep-lat/9202004,hep-lat/9204005,hep-lat/9205018;K.Rummukainen;Multicanonical Cluster Algorithm and the 2-D 7-State Potts Model
hep-th/9209101;hep-th;0;24;;T.Mohaupt;Critical Wilson Lines in Toroidal Compactifications of Heteroric Strings
hep-th/9209102;hep-th;0;0;;J.D.E.Grant;Cosmic Strings and Chronology Protection
hep-ph/9209282;hep-ph;0;13;;P.Elmfors;Temperature Renormalization Group and Resummation
hep-th/9209103;hep-th;0;0;;J.Mickelsson;Current Algebras in $3+1$ dimensions
hep-th/9209104;hep-th;0;9;;C.Burdik,L.Cerny,O.Navratil;The q-Boson Realizations of the Quantum Group $U_q(sl(n+1,C))$
cond-mat/9209031;cond-mat;0;0;;E.Lieb,M.Loss;Fluxes, Laplacians and Kasteleyn's Theorem
hep-th/9209105;hep-th;3;19;hep-th/9204097,hep-th/9206075,hep-th/9207032;P.Bowcock,G.M.T.Watts;Null vectors of the W_3 algebra
math/9209216;math.FA;0;0;;N.J.Kalton;On vector-valued inequalities for Sidon sets and sets of interpolation
math/9209217;math.FA;0;0;;N.J.Kalton;Calderón couples of re-arrangement invariant spaces
math/9209218;math.LO,math.FA;0;0;;D.H.Fremlin,S.Shelah;Pointwise compact and stable sets of measurable functions
math/9209219;math.DG;0;4;;D.Alekseevsky,P.W.Michor;Characteristic classes for $G$-structures
math/9209220;math.DS;0;0;;P.Boyland;Weak disks of Denjoy minimal sets
math/9209221;math.DS;0;0;;J.W.Milnor;Remarks on quadratic rational maps
hep-ph/9209283;hep-ph;0;17;;S.G.Naculich,J.A.Bagger;Quantum Corrections to Deep Bags
hep-th/9209106;hep-th,gr-qc;0;20;;P.Bizon;Saddle point solutions in Yang-Mills-dilaton theory
hep-th/9209107;hep-th;4;59;hep-th/9202061,hep-th/9203051,hep-th/9204071,hep-th/9207050;M.Cederwall,C.Preitschopf;Quaternionic Superconformal Field Theory
hep-th/9209108;hep-th;1;9;hep-th/9201025;J.Laartz,M.Bordemann,M.Forger,U.Schäper;New classical r-matrices from integrable non-linear sigma models
hep-th/9209109;hep-th;0;9;;E.Meinrenken;Maslov indices for periodic orbits
hep-th/9209110;hep-th;0;31;;C.Kim;Self-dual Vortices in the Generalized Abelian Higgs Model with Independent Chern-Simons Interaction
hep-th/9209111;hep-th;0;0;;C.N.Pope,E.Sezgin,K.S.Stelle,X.J.Wang;Discrete States in the $W_3$ String
hep-th/9209112;hep-th;2;24;hep-th/9109005,hep-th/9109024;S.-ichi.Yamaguchi;Correlation Functions of (2k-1, 2) Minimal Matter Coupled to 2D Quantum Gravity
hep-ph/9209284;hep-ph;0;86;;D.Chang,X.-G.He,W.-Y.Keung,B.H.J.McKellar,D.Wyler;Neutron electric dipole moment due to Higgs exchange in Left-Right symmetric models
cond-mat/9209032;cond-mat;0;0;;C.Buzano,A.Pelizzola;Surface reentrance in the semi-infinite spin-1 Ising models
cond-mat/9209033;cond-mat;0;0;;K.Kankaala,T.Ala-Nissila,S.-C.Ying;Theory of adsorbate induced surface reconstruction on W(100)
hep-ph/9209285;hep-ph;0;23;;E.Kh.Akhmedov,Z.G.Berezhiani,R.N.Mohapatra,G.Senjanovic;Planck Scale Effects on the Majoron
hep-lat/9209025;hep-lat;0;24;;E.Vicari;Monte Carlo simulation of lattice ${\rm CP}^{N-1}$ models at large N
hep-ph/9209286;hep-ph;0;11;;G.Siopsis,D.B.DeLaney,S.Jadach,Ch.Shio,B.F.L.Ward;Radiative corrections in processes at the SSC
hep-ph/9209287;hep-ph;0;7;;B.H.Smith;Summing one-loop graphs in a theory with broken symmetry
hep-ph/9209288;hep-ph;0;50;;H.Lew,R.R.Volkas;Discrete quark-lepton symmetry need not pose a cosmological domain wall problem
hep-th/9209113;hep-th,gr-qc;15;44;hep-th/9202004,hep-th/9202075,hep-th/9203042,hep-th/9203052,hep-th/9203054,hep-th/9203059,hep-th/9204072,hep-th/9205028,hep-th/9205069,hep-th/9205089,hep-th/9206020,hep-th/9206070,hep-th/9207034,hep-th/9209012,hep-th/9209058;S.B.Giddings;Toy Models For Black Hole Evaporation
hep-th/9209114;hep-th;0;8;;A.N.Kirillov,P.Mathieu,D.Sénéchal,M.A.Walton;Crystallising the Depth Rule for WZNW Fusion Coefficients
hep-th/9209115;hep-th;2;16;hep-th/9109039,hep-th/9201020;V.Chikalov,A.Pashnev;Twistor-Like Type II Superstring and Bosonic String
hep-ph/9209289;hep-ph;0;14;;B.Blok,M.Shifman;The Rule of Discarding $1/N_c$ in Inclusive Weak Decays. II
hep-th/9209116;hep-th;5;12;hep-th/9201029,hep-th/9201061,hep-th/9202004,hep-th/9202075,hep-th/9205027;R.Kallosh,A.Peet;Dilaton Black Holes Near the Horizon
hep-th/9209117;hep-th,gr-qc;0;6;;M.Cvetic,S.Griffies;Domain Walls in $N=1$ Supergravity
hep-th/9209118;hep-th;0;30;;S.Nojiri,I.Oda;Dilatonic Supergravity in Two Dimensions and the Disappearance of Quantum Black Hole
hep-ph/9209290;hep-ph;0;20;;R.Casalbuoni,A.Deandrea,S.D.Curtis,N.D.Bartolomeo,D.Dominici,F.Feruglio,R.Gatto;The Extended Bess Model: Bounds from Precision Electroweak Measurements
hep-th/9209119;hep-th;0;27;;T.Deguchi,K.Tsurusaki;A New Algorithm for Numerical Calculation of Link Invariants
hep-th/9209120;hep-th;0;0;;Ch.Devchand,V.Ogievetsky;Super Self-Duality as Analyticity in Harmonic Superspace
hep-th/9209121;hep-th,gr-qc;0;0;;G.Kleppe;Transformation Properties of Linearized de Sitter Gravity Solutions
hep-th/9209122;hep-th;3;15;hep-th/9108004,hep-th/9109032,hep-th/9201072;T.Eguchi,H.Kanno,S.-K.Yang;$W_∞ Algebra in Two-Dimensional Black Hole
hep-th/9209123;hep-th;0;19;;L.Frappat,E.Ragoucy,P.Sorba;(SUPER) W Algebras from Non Abelian (SUPER) Toda Theories
hep-th/9209124;hep-th,hep-ph;0;0;;G.Kleppe;Regularization Dependence of Quadratic Divergence Cancellations, VPI-IHEP-92/10
gr-qc/9209012;gr-qc,hep-th;0;0;;J.D.Brown,J.W.York;Quasilocal Energy and Conserved Charges Derived from the Gravitational Action
hep-th/9209125;hep-th;1;53;hep-th/9109045;J.H.Schwarz;Dilaton-Axion Symmetry
hep-lat/9209026;hep-lat,hep-th;2;17;hep-lat/9208008,hep-lat/9208023;A.A.Migdal;Bose Condensation and $Z_N$ Symmetry Breaking in the Mixed Model of Induced QCD
hep-ph/9209291;hep-ph;0;11;;H.Georgi;$D$-$\bar D$ Mixing in Heavy Quark Effective Field Theory
hep-ph/9209292;hep-ph,astro-ph;1;79;hep-ph/9203210;S.A.Abel,S.Sarkar,I.B.Whittingham;Neutralino Dark Matter in a Class of Unified Theories
hep-ph/9209293;hep-ph;0;7;;E.Yehudai;The Vector Equivalence Technique
hep-ph/9209294;hep-ph;0;0;;J.Liu;Particle Width Effect on $CP$-Violating Asymmetries
cond-mat/9209034;cond-mat;0;12;;A.Its,A.Izergin,V.Korepin,N.Slavnov;Temperature Correlations of Quantum Spins
hep-th/9209126;hep-th;0;0;;Z.-H.Wang,H.-Y.Guo;Intrinsic Vertex Regularization and Renormalization in $φ^4$ Field Theory
astro-ph/9209006;astro-ph,hep-ph;0;35;;L.Knox,M.S.Turner;Inflation at the Electroweak Scale
hep-ph/9209295;hep-ph,astro-ph;0;32;;S.-J.Rey;Spontaneous CP Violation, Small Instanton and Invisible Axion
hep-ph/9209296;hep-ph;0;34;;G.F.Giudice,A.Masiero,M.Pietroni,A.Riotto;The Supersymmetric Singlet Majoron
hep-th/9209127;hep-th;2;13;hep-th/9108004,hep-th/9112036;M.H.Sarmadi;The Ring Structure of Chiral Operators for Minimal Models Coupled to 2D Gravity
hep-ph/9209297;hep-ph,hep-th;0;16;;C.J.Fewster,B.S.Kay;Model Dependence of Baryon Decay Enhancement by Cosmic Strings
gr-qc/9209013;gr-qc;0;0;;G.Grignani,G.Nardelli;Poincaré Gauge Theories for Lineal Garvity
hep-th/9209128;hep-th,hep-ph;0;11;;V.Bhansali;How the Little Group Constrains Massless Field Representations in Higher Even Dimensions
hep-lat/9209027;hep-lat;0;15;;F.Karsch,M.L.Laursen,T.Neuhaus,B.Plache;Chern-Simons term in the 4-dimensional SU(2) Higgs Model
gr-qc/9209014;gr-qc,hep-th;0;0;;J.D.Brown,J.W.York;The Microcanonical Functional Integral. I. The Gravitational Field
gr-qc/9209015;gr-qc,hep-th;2;69;hep-th/9109049,hep-ph/9204213;L.J.Garay,J.Garcia-Bellido;Jordan-Brans-Dicke Quantum Wormholes and Coleman's Mechanism
hep-ph/9209298;hep-ph,astro-ph;0;8;;A.H.Jaffe,E.Fenimore,M.S.Turner;Limits on Neutrino Radiative Decay from Sn1987a
hep-th/9209129;hep-th;0;0;;G.Ferretti,S.G.Rajeev,Z.Yang;Three Dimensional Quantum Chromodynamics
hep-th/9209130;hep-th;0;20;;S.Lukyanov,S.L.Shatashvili;Free Field Representation for the Classical Limit of Quantum Affine Algebra
hep-th/9209131;hep-th;0;0;;C.R.Hagen;Comment on Disassembling Anyons
hep-th/9209132;hep-th;0;0;;C.R.Hagen;Comment on Internal Frame Dragging and a Global Analog of the Aharonov-Bohm Effect
hep-ph/9209299;hep-ph;0;28;;C.P.Burgess,J.M.Cline;Majorons Without Majorana Masses and Neutrinoless Double Beta Decay
cond-mat/9210001;cond-mat;0;0;;J.A.Ketoja;Universal criterion for the breakup of invariant tori in dissipative systems
hep-th/9210001;hep-th,astro-ph,gr-qc;0;20;;P.F.Mende;String Theory at Short Distance and the Principle of Equivalence
hep-th/9210002;hep-th,cond-mat;0;0;;J.L.Cardy;Critical Exponents of the Chiral Potts Model from Conformal Field Theory
hep-th/9210003;hep-th;0;27;;G.Cognola,L.Vanzo;Bose-Einstein condensation of scalar fields on hyperbolic manifolds
hep-th/9210004;hep-th;2;45;hep-th/9110073,hep-th/9112060;F.A.Bais,T.Tjin,P.van Driel,J.de Boer,J.Goeree;W Algebras, W Gravities and their Moduli Spaces
hep-th/9210005;hep-th,math.DG;0;0;;C.Nash,D.O.Connor;Ray-Singer Torsion, Topological field theories and the Riemann zeta function at s=3
hep-lat/9210001;hep-lat;1;26;hep-lat/9204010;B.Bruegmann;Non-uniform measure in 4d simplicial quantum gravity
hep-ph/9210201;hep-ph;2;39;hep-th/9109053,hep-th/9205068;M.Cvetic;Stringy Origin of Neutrino Masses within the Minimal Supersymmetric Standard Model
hep-th/9210006;hep-th,gr-qc;2;19;hep-th/9201007,hep-th/9204031;M.Cvetic;Stability of Vacua and Domain Walls in Supergravity and Superstring Theory
hep-th/9210007;hep-th;0;0;;J.Kellendonk,A.Recknagel;Virasoro Representations on Fusion Graphs
hep-th/9210008;hep-th;0;0;;W.Siegel;Green-Schwarz Formulation of Self-Dual Superstring
hep-th/9210009;hep-th;0;38;;A.LeClair,C.Vafa;Quantum Affine Symmetry as Generalized Supersymmetry
hep-th/9210010;hep-th;0;0;;P.Bouwknegt,K.Schoutens;W-symmetry in Conformal Field Theory
hep-lat/9210002;hep-lat,gr-qc,hep-th;1;20;hep-lat/9204010;B.Bruegmann,E.Marinari;4d Simplicial Quantum Gravity with a Non-Trivial Measure
hep-lat/9210003;hep-lat;2;16;hep-lat/9205010,hep-lat/9209022;G.S.Bali,K.Schilling;The Running Coupling from SU(3) Gauge Theory
nucl-th/9210001;nucl-th;0;8;;R.R.Silbar;An Interactive NeXTstep Interface to a Fortran Code for Solving Coupled Differential Equations
hep-th/9210011;hep-th;0;5;;E.Langmann,G.Semenoff;Gauge Theories on a Cylinder
hep-ph/9210202;hep-ph;0;33;;S.P.Rosen;Double Beta Decay
hep-ph/9210203;hep-ph;0;0;;S.P.Rosen;MSW Implications of Solar Neutrino Experiments
nucl-th/9210002;nucl-th;0;14;;F.Wang,G.-han.Wu,L.-jian.Teng,T.Goldman;Quark Delocalization, Color Screening, and Nuclear Intermediate Range Attraction
hep-ph/9210204;hep-ph,nucl-th;0;43;;D.V.Ahluwalia,M.Sawicki;Natural Hadronic Degrees of Freedom for an Effective QCD Action in the Front Form
math/9210201;math.CV;0;0;;E.M.Chirka;Radó theorem and its generalization for CR-mappings
hep-lat/9210004;hep-lat;0;24;;T.Ebihara,K.-I.Kondo;Multicritical Points in a Lattice Yukawa Model with the Wilson-Yukawa Coupling
hep-th/9210012;hep-th,gr-qc;7;21;hep-th/9111038,hep-th/9201061,hep-th/9202014,hep-th/9202037,hep-th/9204046,hep-th/9206055,hep-th/9209055;J.Horne,G.Horowitz;Black Holes Coupled to a Massive Dilaton
cond-mat/9210002;cond-mat,hep-lat;0;0;;V.Privman;Exact Solution of a Phase Separation Model with Conserved Order Parameter Dynamics
hep-lat/9210005;hep-lat,hep-th;0;18;;C.J.Griffin,T.D.Kieu;Fermion Doubling and Gauge Invariance on Random Lattices
hep-th/9210013;hep-th;0;54;;P.Chang,J.S.Dowker;Vacuum energy on orbifold factors of spheres
hep-th/9210014;hep-th;0;19;;M.Talon;Two--poles R-matrices
hep-ph/9210205;hep-ph,hep-th;0;0;;J.Soto,R.Tzani;Anomalies in the effective theory of heavy quarks
hep-th/9210015;hep-th;0;0;;A.S.Schwarz,A.A.Tseytlin;Dilaton shift under duality and torsion of elliptic complex
hep-ph/9210206;hep-ph,hep-th;0;22;;U.Ritschel;Non-Gaussian Corrections to Higgs Mass in Autonomous lambda phi**4
astro-ph/9210001;astro-ph;0;0;;A.C.Robin,M.Creze,V.Mohan;The Edge of the Galactic Disc
hep-lat/9210006;hep-lat;0;5;;T.E.Vaughan;Basis States for Hamiltonian QCD with Dynamical Quarks
nucl-th/9210003;nucl-th,hep-ph;0;0;;K.Maltman,T.Goldman;Modelling the Off-Shell Dependence of $π^o- η$ Mixing with Quark Loops
hep-ph/9210207;hep-ph,hep-th;0;88;;D.J.Gross;Asymptotic Freedom and the Emergence of QCD
hep-th/9210016;hep-th;0;27;;M.J.Bowick;Finite Temperature Strings
hep-th/9210017;hep-th;0;0;;Y.Park,A.Strominger;Supersymmetry and Positive Energy in Classical and Quantum Two-Dimensional Dilaton Gravity
hep-th/9210018;hep-th;0;34;;M.Bowick;The Cosmological Kibble Mechanism in the Laboratory: String Formation in Liquid Crystals
cond-mat/9210003;cond-mat;0;24;;P.T.C.So,S.M.Gruner,S.Erramilli;Pressure Induced Topological Phase Transitions in Membranes
hep-ph/9210208;hep-ph;0;34;;M.Harada,K.Yamawaki;Hidden Local Symmetry at One Loop
nucl-th/9210004;nucl-th;0;22;;C.J.Benesh;Quadrupole Contribution to Two Neutron Removal in Heavy Ion Collisions
hep-th/9210019;hep-th;0;0;;M.Temple-Raston;On the quantisation of SU(2) magnetic monopole dynamics
hep-th/9210020;hep-th,math.GR,math.QA;0;14;;F.Constantinescu,F.Toppan;On the Linearized Artin Braid Representation
gr-qc/9210001;gr-qc;0;0;;I.Bengtsson;Clifford Algebra of Two-Forms, Conformal Structures and Field Equations
gr-qc/9210002;gr-qc;0;7;;R.B.Orellana,H.Vucetich;The Nordtvedt effect in the Trojan asteroids
hep-th/9210021;hep-th,gr-qc;5;47;hep-th/9108001,hep-th/9109038,hep-th/9110053,hep-th/9110065,hep-th/9202092;X.C.de la Ossa,F.Quevedo;Duality Symmetries from Non--Abelian Isometries in String Theories
hep-th/9210022;hep-th;0;0;;C.R.Hagen;Comment on Gauge-Independent Analysis of Chern-Simons Theory with Matter Coupling
hep-th/9210023;hep-th;0;11;;S.Majid;Infinite Braided Tensor Products and 2-D quantum Gravity
hep-th/9210024;hep-th;0;14;;T.Brzezinski,S.Majid;Quantum Group Gauge Theory on Classical Spaces
hep-th/9210025;hep-th;0;0;;A.Kuniba,T.Nakanishi;Rogers dilogarithm in integrable systems
hep-ph/9210209;hep-ph;0;0;;H.-Y.Cheng;Large-$N_c$ Higher Order Weak Chiral Lagrangians for Nonleptonic and Radiative Kaon Decays
hep-ph/9210210;hep-ph,astro-ph;0;18;;J.Hong,J.Kim,P.Sikivie;Wiggly Relativistic Strings
hep-ph/9210211;hep-ph;0;0;;L.E.Ibanez;More About Discrete Gauge Anomalies
hep-ph/9210212;hep-ph;0;0;;G.Mahlon,T.M.Yan,C.Dunn;Generalized Gluon Currents and Applications in QCD
hep-ph/9210213;hep-ph;0;0;;G.Mahlon,T.M.Yan;Multiphoton Production at High Energies in the Standard Model I
hep-ph/9210214;hep-ph;0;0;;G.Mahlon;Multiphoton Production at High Energies in the Standard Model II
hep-th/9210026;hep-th;0;12;;J.París;Faddeev-Popov method for anomalous quasigroups
hep-th/9210027;hep-th;0;0;;C.Destri,P.Maraner,E.Onofri;On the definition of Quantum Free Particle on Curved Manifolds
hep-lat/9210007;hep-lat;2;52;hep-th/9110002,hep-th/9111060;F.Gliozzi;The infrared limit of QCD effective string
hep-th/9210028;hep-th;3;51;hep-th/9108006,hep-th/9110057,hep-th/9112072;H.Ooguri;Schwinger-Dyson equation in three-dimensional simplicial quantum gravity
cond-mat/9210004;cond-mat,hep-th;0;19;;M.Kasner,W.Apel;A new Proposal for a Quasielectron Trial Wavefunction for the FQHE on a Disk
hep-th/9210029;hep-th;0;0;;J.Schiff;The Nonlinear Schrodinger Equation and Conserved Quantities in the Deformed Parafermion and SL(2,R)/U(1) Coset Models
hep-th/9210030;hep-th;0;18;;D.Bailin,A.Love,W.A.Sabra;Twisted Sector Yukawa Couplings for the $Z_3×Z_3$ Orbifold
hep-ph/9210215;hep-ph;0;12;;G.Curci,G.Ricciardi;QCD non-leading corrections to weak decays in the dimensional scheme
hep-ph/9210216;hep-ph;0;0;;M.Chanowitz;Complementarity of Resonant and Nonresonant Strong WW Scattering at SSC and LHC
hep-th/9210031;hep-th;0;8;;D.Waldram;Charged String-like Solutions of Low-energy Heterotic String Theory
alg-geom/9210001;alg-geom,math.AG;0;0;;I.Dolgachev,M.Kapranov;Arrangements of Hyperplanes and Vector Bundles on $P^n$
math/9210202;math.LO;0;0;;W.J.Mitchell;The Complexity of the Core Model
hep-ph/9210217;hep-ph;0;6;;J.T.Gammel,J.L.Gammel;A Non-Standard Quark Model and the Mass Difference $Ξ^- - Ξ^0$
gr-qc/9210003;gr-qc,hep-th;0;13;;A.Ishikawa,H.Ueda;The Wave Function of the Universe by the New Euclidean Path-integral Approach in Quantum Cosmology
hep-th/9210032;hep-th;2;36;hep-th/9108006,hep-th/9202074;D.V.Boulatov;q-deformed lattice gauge theory and 3-manifold invariants
hep-ph/9210218;hep-ph,hep-th;0;56;;D.Kapetanakis,M.Mondragon,G.Zoupanos;Finite Unified Models
hep-ph/9210219;hep-ph;1;42;hep-th/9205068;A.de la Macorra,G.G.Ross;Gaugino condensation in 4-D superstring models
hep-lat/9210008;hep-lat,hep-th;0;14;;A.S.Kronfeld,U.-J.Wiese;SU(N) Gauge Theories with C-Periodic Boundary Conditions: II. Small Volume Dynamics
hep-lat/9210009;hep-lat;0;45;;R.Kenna,C.B.Lang;Renormalization Group Analysis of Finite-Size Scaling in the $Φ^4_4$ Model
alg-geom/9210002;alg-geom,math.AG;0;0;;M.Kapranov;Chow quotients of Grassmannian I
hep-th/9210033;hep-th;4;10;hep-th/9202022,hep-th/9202054,hep-th/9202063,hep-th/9203079;J.Zegwaard;The weaving of curved geometries
cond-mat/9210005;cond-mat,hep-lat;1;20;hep-lat/9202004;B.A.Berg,T.Celik,U.Hansmann;Multicanonical Study of the 3D Ising Spin Glass
hep-th/9210034;hep-th,gr-qc;0;0;;J.R.Anglin;Thermal Equilibrium from the Hu-Paz-Zhang Master Equation
hep-th/9210035;hep-th,gr-qc;0;0;;J.R.Anglin;Influence Functionals and the Accelerating Detector
hep-th/9210036;hep-th,gr-qc;0;0;;D.Cangemi,R.Jackiw;Geometric Gravitational Forces on Particles Moving in a Line
gr-qc/9210004;gr-qc,hep-th,quant-ph;0;48;;J.B.Hartle;The Spacetime Approach to Quantum Mechanics
hep-th/9210037;hep-th,math.QA;0;0;;L.Feher,J.Harnad,I.Marshall;Generalized Drinfeld-Sokolov Reductions and KdV Type Hierarchies
gr-qc/9210005;gr-qc,astro-ph,hep-ph;0;22;;T.Goldman,J.Pérez-Mercader,F.Cooper,M.M.Nieto;The Dark Matter Problem in Light of Quantum Gravity
nucl-th/9210005;nucl-th;0;27;;I.R.Afnan,B.F.Gibson;Resonances in $Λd$ Scattering and the $Σ$-hypertriton
hep-th/9210038;hep-th;0;39;;T.Fujiwara,Y.Igarashi,J.Kubo,K.Maeda;A new insight into BRST anomalies in string theory
hep-th/9210039;hep-th,math.QA;0;15;;L.Freidel,J.M.Maillet;The universal R-matrix and its associated quantum algebra as functionals of the classical r-matrix: the $sl_2$ case
hep-lat/9210010;hep-lat;0;6;;M.Campostrini,P.Rossi,E.Vicari;Scaling and asymptotic scaling in two-dimensional $CP^{N-1}$ models
hep-lat/9210011;hep-lat;0;7;;M.Campostrini,P.Rossi;$1/N$ Expansion of Two-Dimensional Models in the Scaling Region
hep-lat/9210012;hep-lat;0;12;;M.Campostrini,P.Rossi,E.Vicari;Topological susceptibility and string tension in CP(N-1) models
hep-th/9210040;hep-th;0;0;;W.Eholzer;Fusion Algebras Induced by Representations of the Modular Group
hep-th/9210041;hep-th;0;36;;J.Sonnenschein;Physical States in Topological Coset Models
hep-th/9210042;hep-th;0;9;;W.K.Baskerville,S.Majid;The Braided Heisenberg Group
hep-ph/9210220;hep-ph,nucl-th;0;17;;A.Wirzba;The Cheshire Cat Bag Model: Color Anomaly and $η'$ Properties
hep-th/9210043;hep-th;0;21;;T.Tjin;Finite $W$ symmetry in finite dimensional integrable systems
hep-th/9210044;hep-th,math.QA;0;39;;S.Majid;The Quantum Double as Quantum Mechanics
hep-th/9210045;hep-th;1;34;hep-th/9109007;J.Polchinski;Strings and QCD?
hep-th/9210046;hep-th,cond-mat,hep-lat,hep-ph;0;31;;J.Polchinski;Effective Field Theory and the Fermi Surface
hep-ph/9210221;hep-ph,astro-ph;1;24;hep-ph/9203213;L.M.Krauss,E.Gates,M.White;Solar Neutrino Data, Solar Model Uncertainties and Neutrino Oscillations
hep-th/9210047;hep-th,hep-ph;0;0;;M.Dine;String Theory: Lessons for Low Energy Physics
hep-ph/9210222;hep-ph;0;19;;M.Cvetic,P.Langacker;Signatures for Heavy $\bf Z'$ Bosons at Hadron Colliders
hep-lat/9210013;hep-lat;0;23;;T.DeGrand,M.Hecht;Wave functions and their use in spectroscopy and phenomenology
hep-ph/9210223;hep-ph;1;26;hep-ph/9206266;J.Choi,R.R.Volkas;The effective potential at finite temperature in the left-right symmetric model
hep-ph/9210224;hep-ph;0;15;;K.Tsushima,D.O.Riska;Dilatons in the topological soliton model for the hyperons
hep-th/9210048;hep-th,hep-ph,nucl-th;0;18;;H.K.Lee,M.Rho;Rotation Symmetry and Nonabelian Berry Potential
hep-th/9210049;hep-th;2;22;hep-th/9109001,hep-th/9112015;P.H.Frampton,J.T.Liu;Heterotic Parafermionic Superstring
hep-ph/9210225;hep-ph;0;10;;G.Lana,B.Svetitsky;Instability of Bubbles Near the Hadron--Quark-Gluon-Plasma Phase Transition
hep-th/9210050;hep-th,gr-qc;0;0;;A.Sen;Black Holes and Solitons in String Theory
hep-th/9210051;hep-th;0;0;;F.A.Smirnov;Remarks on deformed and undeformed Knizhnik-Zamolodchikov equations
hep-th/9210052;hep-th;0;0;;F.A.Smirnov;Form Factors, deformed Knizhnik-Zamolodchikov equations and finite-gap integration
hep-th/9210053;hep-th;0;31;;J.Fuchs,M.Kreuzer;On the Landau-Ginzburg description of $(A_1^{(1)})^{\oplus N}$ invariants
hep-th/9210054;hep-th;0;63;;B.-S.K.Skagerstam;Localization of Massless Spinning Particles and the Berry Phase
hep-lat/9210014;hep-lat;0;20;;Alonso,Azcoiti,Campos,Ciria,Cruz,Iniguez,lesmes,Piedrafita,Rivero,Tarancon,Badoni,Fernandez,M.Sudupe,R.Lorenzo,G.Arroyo,Martinez,Pech,Tellez;The U(1)-Higgs Model: Critical Behaviour in the Confinig-Higgs region
hep-th/9210055;hep-th;2;32;hep-th/9109027,hep-th/9111031;G.A.Diamandis,B.C.Georgalas,X.Maintas,N.E.Mavromatos;Time-dependent perturbations in two-dimensional String Black Holes
cond-mat/9210006;cond-mat;0;11;;V.M.Yakovenko;Once again about interchain hopping
hep-th/9210056;hep-th;0;17;;H.J.de Vega;Simple Approach to Thermal Bethe Ansatz
hep-th/9210057;hep-th;0;0;;M.Sakamoto;Peculiarity of String Theory on Orbifolds in the Presence of an Antisymmetric Background Field
hep-ph/9210226;hep-ph;0;6;;F.Cooper,C.Lucheroni,H.Shepard,P.Sodano;Variational Method for Studying Solitons in the KdV equation
hep-lat/9210015;hep-lat,hep-ph;0;5;;M.Lombardo,J.B.Kogut,A.Kocic,K.C.Wang;The nature of the continuum limit in strongly coupled quenched QED
hep-ph/9210227;hep-ph;1;15;hep-ph/9204216;S.Jeon;Computing Spectral Densities in Finite Temperature Field Theory
hep-lat/9210016;hep-lat;0;5;;T.Hattori,H.Nakajima;Improvement of efficiency in generating random $U(1)$ variables with Boltzmann distribution
alg-geom/9210003;alg-geom,math.AG;0;0;;A.Tyurin;The simple method of distinguishing the underlying differentiable structures of algebraic surfaces
hep-th/9210058;hep-th;2;41;hep-th/9111032,hep-th/9111054;E.Ivanov,S.Krivonos,R.P.Malik;Boussinesq-type equations from nonlinear realizations of $W_3$
hep-th/9210059;hep-th;0;16;;S.Bellucci,E.Ivanov,S.Krivonos;N=3 Supersymmetric Extension of KdV Equation
cond-mat/9210007;cond-mat,hep-th;0;0;;A.Houghton,J.B.Marston;Bosonization and Fermion Liquids in Dimensions Greater Than One
hep-th/9210060;hep-th;1;26;hep-th/9108007;T.Curtright,C.Zachos;Supersymmetry and the Nonlocal Yangian Deformation Symmetry
hep-th/9210061;hep-th;0;0;;R.Percacci,E.Sezgin;Symmetries of P-Branes
hep-ph/9210228;hep-ph;0;9;;M.Bando,T.Kugo,N.Maekawa,H.Nakano;Improving the Effective Potential
nucl-th/9210006;nucl-th;0;45;;M.K.Liou,D.Lin,B.F.Gibson;Anatomy of the Soft-Photon Approximation in Hadron-Hadron Bremsstrahlung
hep-th/9210062;hep-th;0;0;;R.Schimmrigk;Critical String Vacua from Noncritical Manifolds: A Novel Framework for String Compactification
hep-ph/9210229;hep-ph;0;16;;M.Bando,T.Kugo,N.Maekawa,H.Nakano;Improving the Effective Potential:Multi-Mass-Scale Case
hep-th/9210063;hep-th;0;41;;Y.-hiro.Quano,A.Fujii;Yang-Baxter Equation for $A^{(1)}_{n-1}$ Broken ${\Bf Z}_N $ Models
hep-th/9210064;hep-th;2;8;hep-th/9109001,hep-th/9112015;K.R.Dienes;Fractional Superstrings with Critical Spacetime Dimensions Four and Six: A Status Report
nucl-th/9210007;nucl-th,hep-ph;0;0;;P.M.Gensini,G.Violini;Old Problems in Low-Energy $K N$ Physics and Perspectives Opening Up at New Machines
nucl-th/9210008;nucl-th,hep-ph;0;0;;P.M.Gensini;Low-Energy $KN$ Interactions at a $φ$-Factory
nucl-th/9210009;nucl-th,hep-ph;0;0;;P.M.Gensini;Low-Energy Kaon Interactions and Scattering on Nucleons and Light Nuclei
hep-th/9210065;hep-th;0;4;;E.Witten;Some Computations in Background Independent Open-String Field Theory
hep-th/9210066;hep-th;11;78;hep-th/9109046,hep-th/9110024,hep-th/9110025,hep-th/9112016,hep-th/9112069,hep-th/9201013,hep-th/9203028,hep-th/9206060,hep-th/9208065,hep-th/9209041,hep-th/9210037;T.Hollowood,J.L.Miramontes,J.S.Guillen;Generalized Integrability and two-dimensional Gravitation
nucl-th/9210010;nucl-th;0;26;;G.E.Brown,R.Machleidt;Saturation in the Nuclear Matter Problem
gr-qc/9210006;gr-qc,hep-th,quant-ph;1;22;gr-qc/9210010;J.B.Hartle;The Quantum Mechanics of Closed Systems
hep-th/9210067;hep-th;0;13;;J.Hietarinta;The complete solution to the constant quantum Yang-Baxter equation in two dimensions
gr-qc/9210007;gr-qc,hep-th;1;27;hep-th/9109006;A.Anderson;Unitary Equivalence of the Metric and Holonomy Formulations of 2+1 Dimensional Quantum Gravity on the Torus
hep-th/9210068;hep-th;0;45;;B.de Wit,F.Vanderseypen,A.V.Proeyen;Symmetry structure of special geometries
hep-lat/9210017;hep-lat;0;16;;R.Kenna,C.B.Lang;Lee-Yang Zeroes and Logarithmic Corrections in the $Φ^4_4$ Theory
hep-ph/9210230;hep-ph;0;23;;J.A.Bagger;Observing Electroweak Symmetry Breaking at the SSC
hep-th/9210069;hep-th;0;0;;J.Mickelsson;Hilbert space cocycles as representations of $(3+1)-$ D current algebras
hep-ph/9210231;hep-ph;0;22;;L.Randall;ETC With a GIM Mechanism
hep-ph/9210232;hep-ph;0;35;;L.Randall;Testing ETC Generation of the Top Quark Mass
hep-lat/9210018;hep-lat;2;31;hep-lat/9204011,hep-lat/9205020;Gupta,Daniel,Kilcup,Patel,Sharpe;The Kaon $B$-parameter with Wilson Fermions
hep-th/9210070;hep-th;0;0;;R.Ferraro,M.Henneaux,M.Puchin;On the Quantization of Reducible Gauge Systems
hep-ph/9210233;hep-ph;1;40;hep-ph/9204204;C.T.Hill,D.C.Kennedy,T.Onogi,H.--L.Yu;Spontaneously Broken Technicolor and the Dynamics of Virtual Vector Technimesons
alg-geom/9210004;alg-geom,math.AG;0;0;;O.Debarre,M.Klassen;Points of Low Degree on Smooth Plane Curves
hep-th/9210071;hep-th;0;0;;J.Harnad,M.-.Wisse;Matrix Nonlinear Schrödinger Equations and Moment Maps into Loop Algebras$^\dag $
alg-geom/9210005;alg-geom,math.AG;0;0;;O.Debarre;Degrees of Curves in Abelian Varieties
nucl-th/9210011;nucl-th;0;50;;F.Sammarruca,D.P.Xu,R.Machleidt;Relativistic Corrections to the Triton Binding Energy
cond-mat/9210008;cond-mat,hep-ph;0;11;;A.M.Srivastava;String Defects in Condensed Matter Systems as Optical Fibers
cond-mat/9210009;cond-mat;0;0;;F.Liu,G.F.Mazenko;Phase Ordering Dynamics in the Continuum q-state Clock Model
hep-th/9210072;hep-th;1;26;hep-th/9201013;S.Kharchev,A.Marshakov;Topological versus Non--Topological Theories and $p-q$ Duality in $c ≤1$ 2d Gravity Models
hep-th/9210073;hep-th,cond-mat,math-ph,math.MP,nlin.SI,solv-int;0;39;;C.A.Tracy,H.Widom;Introduction to Random Matrices
hep-th/9210074;hep-th,cond-mat,math-ph,math.MP,nlin.SI,solv-int;0;17;;C.A.Tracy,H.Widom;Level-Spacing Distributions and the Airy Kernel
hep-th/9210075;hep-th;1;34;hep-th/9204089;A.T.Filippov,A.P.Isaev,A.B.Kurdikov;On Paragrassmann Differential Calculus
cond-mat/9210010;cond-mat;1;10;cond-mat/9205014;K.Harigaya,M.Fujita;Dimerization structures on the metallic and semiconducting fullerene tubules with half-filled electrons
astro-ph/9210002;astro-ph;0;0;;S.Cristiani,E.Giallongo,L.M.Buson,C.Gouiffes,F.L.Franca;Coordinated UV-optical observations of quasars: the evolution of the Lyman absorption
cond-mat/9210011;cond-mat;0;0;;L.Bergomi,J.P.Blaizot,Th.Jolicoeur,E.Dagotto;Generalized spin density wave state of the Hubbard model on the C12 and C60 clusters
hep-th/9210076;hep-th;0;0;;M.Billo',P.Fre',L.Girardello,A.Zaffaroni;Gravitational Instantons in Heterotic String Theory: The H-Map and the Moduli Deformations of (4,4) Superconformal Field Theories
hep-th/9210077;hep-th;0;0;;J.Harnad,M.-A.Wisse;Isospectral flow in Loop Algebras and Quasiperiodic Solutions of the Sine-Gordon Equation
hep-ph/9210234;hep-ph;0;12;;F.Cooper,H.Shepard,C.Lucheroni,P.Sodano;Post-Gaussian Varioational Method for the Nonlinear Schrodinger Equation
alg-geom/9210006;alg-geom,math.AG;0;14;;E.Lerman,R.Sjamaar;Reductive group actions on Kähler manifolds
hep-ph/9210235;hep-ph;1;81;hep-ph/9206203;P.Langacker,N.Polonsky;Uncertainties in Coupling Constant Unification
hep-ph/9210236;hep-ph;0;0;;B.Grinstein;The SSC: Programme and Searches for New Particles
gr-qc/9210008;gr-qc,hep-th;0;10;;J.Greensite;Dynamical Origin of the Lorentzian Signature of Spacetime
hep-th/9210078;hep-th;0;34;;J.Kellendonk;On The Algebraic Characterization of Aperiodic Tilings Related To ADE-Root Systems
hep-th/9210079;hep-th;6;36;hep-th/9108001,hep-th/9110054,hep-th/9205037,hep-th/9206006,hep-th/9206048,hep-th/9208001;I.Bars;Superstrings on Curved Spacetimes
hep-th/9210080;hep-th;3;30;hep-th/9204019,hep-th/9207013,hep-th/9210029;D.A.Depireux,J.Schiff;On The Hamiltonian Structures and The Reductions of The KP Hierarchy
hep-th/9210081;hep-th;0;0;;F.Bastianelli;A note on 2D chiral gravity and chiral bosons
hep-ph/9210237;hep-ph;0;26;;J.Chýla,J.Fischer,P.Kolář;On an asymptotic estimate of the $n$-loop correction in perturbative QCD
hep-th/9210082;hep-th;1;28;hep-th/9207117;R.C.Myers,V.Periwal;Chiral Non-Critical Strings
gr-qc/9210009;gr-qc,hep-th;0;0;;R.Hecht,F.W.Hehl,J.D.McCrea,E.W.Mielke,Y.Ne'eman;Improved Energy-Momentum Currents in Metric-Affine Spacetime
hep-th/9210083;hep-th;0;0;;M.A.Wisse;Quasi-Periodic Solutions for matrix nonlinear Schroedinger Equations
hep-ph/9210238;hep-ph;1;48;hep-th/9109053;P.Langacker;Proton Decay
hep-ph/9210239;hep-ph,nucl-th;0;13;;E.J.Eichten,I.Hinchliffe,C.Quigg;Flavor Asymmetry of the Nucleon Sea: Consequences for Dilepton Production
hep-th/9210084;hep-th;0;25;;G.L.Rossini,F.A.Schaposnik;Fermionic Coset Models as Topological Models
hep-ph/9210240;hep-ph;1;25;hep-ph/9206203;L.J.Hall,U.Sarid;Gravitational Smearing of Minimal Supersymmetric Unification Predictions
hep-ph/9210241;hep-ph;0;21;;S.Mizuta,D.Ng,M.Yamaguchi;Phenomenological Aspects of Supersymmetric Standard Models without Grand Unification
hep-th/9210085;hep-th;2;39;hep-th/9109007,hep-th/9201054;A.A.Bytsenko,E.Elizalde,S.D.Odintsov,S.Zerbini;A Novel Representation for the Free Energy in String Theory at Non-Zero Temperature
hep-th/9210086;hep-th;0;0;;T.Takebe;Generalized $XYZ$ Model Associated to Sklyanin Algebra$^*$
hep-th/9210087;hep-th;0;10;;F.Falceto,K.Gawȩdzki;Chern-Simons Theory on the Torus
cond-mat/9210012;cond-mat;0;31;;A.Amengual,E.Hernandez-Garcia,M.S.Miguel;Ordering and finite-size effects in the dynamics of one-dimensional transient patterns
cond-mat/9210013;cond-mat;0;20;;J.A.Støvneng,A.-P.Jauho;Numerical studies of tunneling in a nonharmonic time-dependent potential
hep-th/9210088;hep-th;0;7;;F.Belgiorno,A.S.Cattaneo,M.Martellini,F.Fucito;A Conformal Affine Toda Model of 2D Black Holes: A Quantum Study of the Evaporation End-Point
hep-th/9210089;hep-th;0;0;;M.R.Adams,J.Harnad,J.Hurtubise;Darboux Coordinates and Liouville-Arnold Integration in Loop Algebras
hep-ph/9210242;hep-ph;0;0;;G.L.Kane,C.Kolda,J.D.Wells;Calculable Upper Limit on the Mass of the Lightest Higgs Boson in Any Perturbatively Valid Supersymmetric Theory
hep-lat/9210019;hep-lat,cond-mat;0;11;;U.-J.Wiese;Bosonization and Cluster Updating of Lattice Fermions
hep-th/9210090;hep-th;0;14;;K.Ranganathan;Nearby CFT's in the operator formalism: The role of a connection
hep-th/9210091;hep-th,math.DG;0;17;;O.N.Khudaverdian,A.P.Nersessian;Even and odd symplectic and Kählerian structures on projective superspaces
hep-lat/9210020;hep-lat,cond-mat,hep-th;0;24;;M.Henkel,R.Peschanski;Intermittency Studies in Directed Bond Percolation
hep-th/9210092;hep-th,hep-ph;0;6;;J.A.Dixon;A Natural Mechanism for Supersymmetry Breaking with Zero Cosmological Constant (Minor corrections of some formulae, no substantial change)
hep-th/9210093;hep-th;0;0;;H.Nishino;Exact Solutions for Self--Dual Yang--Mills and Self--Dual Tensor Multiplets on Gravitational Instanton Background
cond-mat/9210014;cond-mat,hep-th;0;16;;Y.-C.Tsai,Y.Shapir;On the Scale-Invariant Distribution of the Diffusion Coefficient for Classical Particles Diffusing in Disordered Media.-
hep-ph/9210243;hep-ph,hep-th;0;0;;S.Dodelson,B.-A.Gradwohl;How Effective is the Effective Potential?
hep-th/9210094;hep-th;1;20;hep-th/9109007;K.Bardakci;A Candidate For The QCD String Based On Non-Backtracking Random Walks
hep-th/9210095;hep-th,math.QA,math.SG;0;0;;J.Harnad,B.A.Kupershmidt;Symplectic Geometries on $T^*\widetilde G$, Hamiltonian Group Actions and Integrable Systems
cond-mat/9210015;cond-mat;0;0;;J.B.Marston,D.R.Andersson,E.R.Behringer,B.H.Cooper,C.A.DiRubio,G.A.Kimmel,C.Richardson;Many Body Theory of Charge Transfer in Hyperthermal Atomic Scattering
hep-th/9210096;hep-th,cond-mat;0;0;;S.Rao,D.Sen;Non-linear Field Theory of a Frustrated Heisenberg Spin Chain
hep-th/9210097;hep-th;2;8;hep-th/9112075,hep-th/9202013;V.Spiridonov;Exactly Solvable Potentials and Quantum Algebras
hep-th/9210098;hep-th;0;19;;A.Sitarz;Noncommutative Geometry and Gauge Theories on Discrete Groups
hep-th/9210099;hep-th;0;55;;M.de Roo,H.Suelmann,A.Wiedemann;The Supersymmetric Effective Action of the Heterotic String in Ten Dimensions
hep-th/9210100;hep-th;0;43;;K.Gawȩdzki;Quantum Group Symmetries in Conformal Field Theory
hep-th/9210101;hep-th;4;17;hep-th/9201061,hep-th/9203042,hep-th/9203052,hep-th/9203054;K.Hamada;Gravitational Collapse in 1+1 Dimensions and Quantum Gravity
cond-mat/9210016;cond-mat;0;12;;M.Fabrizio,A.Parola;Spin-Charge separation in a model of two coupled chains
hep-th/9210102;hep-th,cond-mat,hep-lat;0;0;;M.Henkel;On the Two-Point Correlation Function in Dynamical Scaling and SCHRÖdinger Invariance
astro-ph/9210003;astro-ph;0;0;;Y.Tomozawa;Cosmic Rays, Gamma Rays and Neutrinos from Point Sources
hep-lat/9210021;hep-lat;0;3;;E.Marinari,M.L.Paciello,G.Parisi,B.Taglienti;The String Tension in Gauge Theories: a Suggestion for a New Measurement Method
hep-ph/9210244;hep-ph;0;10;;M.B.Voloshin;Zeros of Tree-Level Amplitudes at Multi-Boson Thresholds
hep-th/9210103;hep-th;0;0;;C.-L.Ho,Y.Hosotani;Operator Algebra in Chern-Simons Theory on a Torus
hep-lat/9210022;hep-lat;0;38;;W.Bock,A.K.De,E.Focht,J.Smit;Fermion-Higgs model with strong Wilson-Yukawa coupling in two dimensions
hep-ph/9210245;hep-ph;0;6;;O.W.Greenberg;Scaling limit of a non-relativistic model
hep-ph/9210246;hep-ph;0;0;;S.Mohanty,S.N.Nayak,S.Sahu;Chern-simon type photon mass from fermion electric dipole moments at finite temperature in 3+1 dimensions
hep-ph/9210247;hep-ph;0;51;;D.A.Morris,R.Rosenfeld;The Perturbative Onset of Multiparticle Production in Weak Interactions
alg-geom/9210007;alg-geom,math.AG;0;24;;M.Thaddeus;Stable pairs, linear systems and the Verlinde formula
hep-th/9210104;hep-th,cond-mat;0;0;;M.Carreau;Four-Parameter Point-Interaction in 1-D Quantum Systems
hep-th/9210105;hep-th;0;0;;I.R.Klebanov,A.Pasquinucci;Infinite symmetry and Ward identities in two-dimensional string theory
nucl-th/9210012;nucl-th;0;28;;G.Rosensteel,A.L.Goodman;Riemann's theorem for quantum tilted rotors
hep-th/9210106;hep-th;0;0;;D.Montano,G.Rivlis;Solving Topological 2D Quantum Gravity Using Ward Identities
hep-ph/9210248;hep-ph;0;29;;T.-S.Park,D.-P.Min,M.Rho;Nuclear Axial-Charge Transitions in Chiral Perturbation Theory
cond-mat/9210017;cond-mat;0;26;;W.Wang,E.Canessa;Biharmonic pattern selection
cond-mat/9210018;cond-mat;0;0;;J.P.Sethna,K.Dahmen,S.Kartha,J.A.Krumhansl,B.W.Roberts,J.D.Shore;Hysteresis and hierarchies: dynamics of disorder-driven first-order phase transformations
nucl-th/9210013;nucl-th;0;19;;T.Nakatsukasa,S.Mizutori,K.Matsuyanagi;Effects of Octupole Vibrations on Quasiparticle Modes of Excitation in Superdeformed $^{193}$Hg
hep-th/9210107;hep-th;0;0;;S.R.Das;Matrix Models and Black Holes
hep-th/9210108;hep-th;0;6;;M.Dubois-Violette;Complex structures and the Elie Cartan approach to the theory of spinors
hep-th/9210109;hep-th,cond-mat;0;0;;A.P.Polychronakos;Lattice Integrable Systems of Haldane-Shastry Type
hep-ph/9210249;hep-ph;0;0;;R.Guida,K.Konishi;Avalanche in the Valley (Fermions, Anomaly and Unitarity in High-Energy Electroweak Interactions)
hep-ph/9210250;hep-ph;0;44;;K.S.Babu;The fermion mass problem
hep-ph/9210251;hep-ph;0;22;;K.S.Babu,Q.Shafi;Heavy top quark from Fritzsch mass matrices
hep-th/9210110;hep-th,gr-qc;0;20;;R.Gambini,J.Pullin;Quantum Einstein-Maxwell Fields: A Unified Viewpoint from the Loop Representation
astro-ph/9210004;astro-ph;0;0;;P.Fischer,D.L.Welch,M.Mateo;Dynamics of the Young Binary LMC Cluster NGC 1850
nucl-th/9210014;nucl-th;0;19;;C.W.Johnson,S.E.Koonin,G.H.Lang,W.E.Ormand;Monte Carlo methods for the nuclear shell model
hep-ph/9210252;hep-ph;0;14;;Z.Berezhiani,R.Rattazzi;Radiative Origin of the Fermion Mass Hierarchy: A Realistic and Predictive Approach
hep-th/9210111;hep-th;0;20;;A.P.Balachandran;Gauge Symmetries,Topology and Quantisation
hep-th/9210112;hep-th;0;0;;Y.Hosotani,C.-L.Ho;Anyons on a Torus
nucl-th/9210015;nucl-th;0;35;;N.R.Walet,R.D.Amado;Skyrmions and the Nuclear Force
hep-ph/9210253;hep-ph,astro-ph,hep-lat;0;35;;K.Rajagopal,F.Wilczek;Static and Dynamic Critical Phenomena at a Second Order QCD Phase Transition
astro-ph/9210005;astro-ph;0;26;;P.Marziani,J.W.Sulentic;Evidence for a Very Broad Line Region in PG 1138+222
math/9210203;math.LO;0;0;;T.LaBerge,A.Landver;Reflection and Weakly Collectionwise Hausdorff Spaces
gr-qc/9210010;gr-qc,hep-th,quant-ph;0;0;;M.Gell-Mann,J.B.Hartle;Classical Equations for Quantum Systems
hep-ph/9210254;hep-ph;0;37;;I.Sarcevic;Intermittency and Particle Correlations: Theory
hep-ph/9210255;hep-ph,hep-th;0;43;;D.J.Broadhurst,A.L.Kataev,O.V.Tarasov;Analytical on-shell QED results: 3-loop vacuum polarization, 4-loop beta-function and the muon anomaly
hep-lat/9210023;hep-lat;0;18;;C.R.Gattringer,I.Hip,C.B.Lang;Scattering in a Simple 2-d Lattice Model
hep-th/9210113;hep-th;1;17;hep-th/9206007;G.Giavarini,C.P.Martin,F.R.Ruiz;Regularization and Renormalization of Chern-Simons Theory
hep-th/9210114;hep-th;0;26;;G.L.Cardoso,B.A.Ovrut;Natural Supergravity Inflation
gr-qc/9210011;gr-qc;0;268;;C.J.Isham;Canonical Quantum Gravity and the Problem of Time
hep-lat/9210024;hep-lat,cond-mat;0;0;;R.Anishetty,S.Cheluvaraja,H.S.Sharatchandra,M.Mathur;Dual of 3-dimensional pure SU(2) Lattice Gauge Theory and the Ponzano-Regge Model
gr-qc/9210012;gr-qc,hep-th;0;20;;S.Deser,A.R.Steif;No Time Machines from Lightlike Sources in 2+1 Gravity
cond-mat/9210019;cond-mat;0;0;;A.Lopez,E.Fradkin;Response functions and Spectrum of Collective Excitations of Fractional Quantum Hall Effect Systems
hep-th/9210115;hep-th,math.DG;0;5;;A.Schwarz;Semiclassical approximation in Batalin-Vilkovisky formalism
hep-th/9210116;hep-th;0;20;;O.A.Mattos,V.O.Rivelles;Non-Perturbative Solutions of String Theory in Gravitational Backgrounds
hep-th/9210117;hep-th;2;52;hep-th/9109027,hep-th/9112009;F.Yu,Y.-S.Wu;On the KP Hierarchy, $\hat W_∞$ Algebra, and Conformal SL(2,R)/U(1) Model: I. The Classical Case
hep-th/9210118;hep-th;2;25;hep-th/9109042,hep-th/9112009;F.Yu,Y.-S.Wu;On the KP Hierarchy, $\hat W_∞$ Algebra, and Conformal SL(2,R)/U(1) Model: II. The Quantum Case
hep-th/9210119;hep-th,gr-qc;24;89;hep-th/9108001,hep-th/9108011,hep-th/9109038,hep-th/9110004,hep-th/9110053,hep-th/9110065,hep-th/9110067,hep-th/9111038,hep-th/9112070,hep-th/9201061,hep-th/9202004,hep-th/9202014,hep-th/9202037,hep-th/9202092,hep-th/9203083,hep-th/9204046,hep-th/9204099,hep-th/9206016,hep-th/9206055,hep-th/9207053,gr-qc/9209004,hep-th/9209055,hep-th/9210012,hep-th/9210050;G.T.Horowitz;The Dark Side of String Theory: Black Holes and Black Strings
hep-th/9210120;hep-th;0;0;;A.Dhar,G.Mandal,S.R.Wadia;Stringy Quantum Effects in 2-Dimensional Black-Hole
hep-ph/9210256;hep-ph,hep-th;0;36;;A.E.Faraggi;Generation Mass Hierarchy in Superstring Derived Models
cond-mat/9210020;cond-mat;0;36;;H.Cruz,F.Piazza,L.Pavesi;Magnetic field effects on non-periodic superlattice structures
hep-th/9210121;hep-th;0;0;;S.F.Hassan,A.Sen;Marginal Deformations of WZNW and Coset Models from O(d,d) Transformation
hep-th/9210122;hep-th;0;0;;D.C.Dunbar,K.G.Joshi;Characters for Coset Conformal Field Theories
hep-ph/9210257;hep-ph;0;0;;L.Clavelli;Tau Decay Puzzles and Possible Light Gluinos
hep-lat/9210025;hep-lat;2;14;hep-lat/9112002,hep-lat/9204016;M.Grabenstein,K.Pinn;Theoretical Analysis of Acceptance Rates in Multigrid Monte Carlo
nucl-th/9210016;nucl-th;0;17;;E.Rost,C.E.Price,J.R.Shepard;Transverse response functions in the $Δ$-resonance region
hep-th/9210123;hep-th,gr-qc;0;0;;M.Cvetič,R.Davis,S.Griffies,H.H.Soleng;Cauchy Horizons, Thermodynamics and Closed Time-like Curves in Planar Supersymmetric Space-times
hep-lat/9210026;hep-lat;0;11;;U.M.Heller,M.Klomfass,H.Neuberger,P.Vranas;Regularization dependence of the Higgs mass triviality bound
alg-geom/9210008;alg-geom,math.AG;0;6;;D.A.Cox;Erratum to "The Homogeneous Coordinate Ring of a Toric Variety", along with the original paper
nucl-th/9210017;nucl-th;0;42;;R.D.Amado,R.Bijker,F.Cannata,J.P.Dedonder,N.R.Walet;Quartets of superdeformed bands and supersymmetry breaking
hep-th/9210124;hep-th;0;36;;J.M.Isidro,J.M.F.Labastida,A.V.Ramallo;Polynomials for Torus Links from Chern-Simons Gauge Theories
hep-th/9210125;hep-th;0;50;;G.von Gehlen,A.Honecker;Multi-particle structure in the Z_n-chiral Potts models
hep-lat/9210027;hep-lat;0;26;;A.Bochkarev,P.de Forcrand;Nonperturbative evaluation of the diffusion rate in field theory at high temperatures
hep-ph/9210258;hep-ph;0;31;;K.Aoki,S.Peris;Non--perturbative evidence for non--decoupling of heavy fermions
hep-lat/9210028;hep-lat,hep-th;0;22;;H.D.Trottier,R.M.Woloshyn;The Savvidy ``ferromagnetic vacuum'' in three-dimensional lattice gauge theory
hep-ph/9210259;hep-ph;0;49;;B.Margolis,J.Ng,M.Phipps,H.D.Trottier;Quark model calculation of $η→l^+ l^-$ to all orders in the bound state relative momentum
cond-mat/9210021;cond-mat;0;0;;F.Dalfovo,S.Stringari;Static Response Function for Longitudinal and Transverse Excitations in Superfluid Helium
cond-mat/9210022;cond-mat;0;35;;C.Q.Wu;Correlaction Effects on the Band Gap of Conducting Polymers
hep-th/9210126;hep-th;0;15;;A.Borzi,A.Koubek;A Multi-Grid Method for the Resolution of Thermodynamic Bethe Ansatz Equations
nucl-th/9210018;nucl-th;0;49;;Y.Umino,F.Myhrer;Electromagnetic Decays of Hyperons (II)
cond-mat/9210023;cond-mat;0;0;;L.Pitaevskii,S.Stringari;Uncertainty Principle and Off-Diagonal Long Range Order in the Fractional Quantum Hall Effect
hep-th/9210127;hep-th;0;0;;A.Sagnotti;A Note on the Green - Schwarz Mechanism in Open - String Theories
hep-lat/9210029;hep-lat;0;13;;R.Altmeyer,K.D.Born,M.Goeckeler,R.Horsley,E.Laermann,G.Schierholz;Renormalisation of lattice currents and the calculation of decay constants for dynamical staggered fermions
hep-th/9210128;hep-th;1;16;hep-th/9206049;J.Avan,M.Talon;Classical R-matrix structure for the Calogero model
gr-qc/9210013;gr-qc;0;20;;W.G.Anderson,P.R.Brady,W.Israel,S.M.Morsink;Quantum Effects in Black Hole Interiors
hep-th/9210129;hep-th,cond-mat;0;40;;R.Kedem,B.M.Mccoy;Construction of Modular Branching Functions from Bethe's Equations in the 3-State Potts Chain
cond-mat/9210024;cond-mat;0;30;;P.De,R.Pelcovits,E.Vogel,J.Vogel;The Supercooling of a Nematic Liquid Crystal
hep-th/9210130;hep-th;0;5;;M.Forger,J.Laartz,U.Schaeper;The Algebra of the Energy-Momentum Tensor and the Noether Currents in Classical Non-Linear Sigma Models
hep-ph/9210260;hep-ph;1;10;hep-ph/9204215;V.Barger,M.S.Berger,P.Ohmann;Universal Evolution of CKM Matrix Elements
hep-th/9210131;hep-th;0;13;;L.Brekke,H.Dykstra,A.F.Falk,T.D.Imbo;Novel Spin and Statistical Properties of Nonabelian Vortices
cond-mat/9210025;cond-mat,hep-lat;0;0;;J.-S.Wang,P.Nielaba,V.Privman;Collective Effects in Random Sequential Adsorption of Diffusing Hard Squares
gr-qc/9210014;gr-qc,astro-ph,hep-th;0;12;;R.H.Brandenberger;A Nonsingular Universe
hep-ph/9210261;hep-ph,astro-ph;0;72;;R.H.Brandenberger;Topological Defect Models of Structure Formation After the COBE Discovery of CMB Anisotropies
hep-th/9210132;hep-th;0;56;;J.L.Vazquez-Bello;The Search for Zoo-Perparticles
hep-th/9210133;hep-th,gr-qc;0;0;;A.M.E.Gradechi,S.D.Bièvre;Phase Space Quantum Mechanics on the Anti-De Sitter Spacetime and its Poincaré Contraction
hep-ph/9210262;hep-ph;0;36;;S.J.Brodsky,P.Hoyer;A Bound on the Energy Loss of Partons in Nuclei
nucl-th/9210019;nucl-th,astro-ph;0;9;;Q.-R.Zhang,B.-Q.Ma,W.Greiner;Finite volume of baryons and the mass limit for neutron stars
hep-lat/9210030;hep-lat;0;16;;P.Cea,L.Cosmai;Dual Superconductor Mechanism of Confinement on the Lattice
hep-th/9210134;hep-th;0;13;;M.D.Freeman,P.West;$W_3$ string scattering
hep-lat/9210031;hep-lat,hep-th;2;20;hep-th/9110002,hep-th/9111060;M.Caselle,F.Gliozzi,S.Vinti;Some universal features of the effective string picture of pure gauge theories
hep-lat/9210032;hep-lat;0;0;;A.C.D.van Enter,R.Fernandez,A.D.Sokal;Regularity Properties and Pathologies of Position-Space Renormalization-Group Transformations
hep-th/9210135;hep-th;0;21;;A.Rogers;Anticommuting Variables, Fermionic Path Integrals and Supersymmetry
gr-qc/9210015;gr-qc;0;0;;K.C.K.Chan,R.B.Mann;Cosmological Models in Two Spacetime Dimensions
hep-th/9210136;hep-th;0;0;;S.Guruswamy,S.G.Rajeev;Two Dimensional Quantum Chromodynamics on a Cylinder
hep-th/9210137;hep-th;0;0;;J.Schiff;Actions for Integrable Systems and Deformed Conformal Theories
hep-ph/9210263;hep-ph;0;34;;I.Sarcevic;Intermittency and Multidimensional Correlations
hep-ph/9210264;hep-ph;0;42;;H.C.Eggers,H.-Th.Elze,I.Sarcevic;Three Dimensional Statistical Field Theory for Density Fluctuations in Heavy-Ion Collsiions
math/9210204;math.LO;0;0;;J.Zapletal;Splitting number and the core model
math/9210205;math.FA;0;0;;H.P.Rosenthal;A characterization of Banach spaces containing $c_0$
math/9210206;math.FA;0;0;;M.Cwikel,N.J.Kalton;Interpolation of compact operators by the methods of Calderón and Gustavsson-Peetre
math/9210207;math.FA;0;35;;A.Koldobsky;Schoenberg's Problem on Positive Definite Functions
hep-th/9210138;hep-th;0;6;;K.Odaka;Comment on $q$-deformation in Second Quantization Procedure
hep-ph/9210265;hep-ph;0;24;;E.Jenkins,M.Luke,A.V.Manohar,M.J.Savage;Weak Radiative Hyperon Decays in Chiral Perturbation Theory
hep-ph/9210266;hep-ph;0;40;;A.Brignole,F.Zwirner;Radiative corrections to the decay H==>hh in the Minimal Supersymmetric Standard Model
hep-ph/9210267;hep-ph;0;63;;P.Hoyer;New QCD Effects at Large x
hep-lat/9210033;hep-lat,hep-ph;0;7;;C.Ford,D.R.T.Jones,P.W.Stephenson,M.B.Einhorn;The effective potential and the renormalisation group
hep-ph/9210268;hep-ph;0;23;;M.Rho;Heavy-Quark Baryons as Skyrmions
hep-th/9210139;hep-th;1;33;hep-th/9110070;A.K.Tollsten;On Anomaly-free Supergravity as an Effective String Theory
hep-th/9210140;hep-th;2;18;hep-th/9111015,hep-ph/9203207;C.Manuel;Differential Renormalization of a Yukawa Model with $γ_5$
hep-ph/9210269;hep-ph;0;14;;B.Blok,M.Shifman;Nonperturbative QCD efects in weak hadronic decays
hep-lat/9210034;hep-lat;1;10;hep-lat/9203001;K.M.Bitar,P.Vranas;The $I=1$, $J=1$ channel of the O(4) $λφ^4_4$ theory
hep-th/9210141;hep-th;0;23;;S.Majid;Braided Momentum Structure of the q-Poincare Group
hep-th/9210142;hep-th;0;0;;A.Klemm,S.Theisen;Recent Efforts in the Computation of String Couplings:
hep-th/9210143;hep-th;1;26;hep-th/9108003;K.Ito;The $W$ algebra structure of $N=2$ $CP_n$ coset models
hep-th/9210145;hep-th,cond-mat;0;0;;S.Randjbar--Daemi,A.Salam,J.Strathdee;Generalized Spin Systems and $σ$--Models
hep-lat/9210035;hep-lat,hep-ph,hep-th;0;4;;G.Bathas,H.Neuberger;A better large $N$ expansion for chiral Yukawa models
cond-mat/9210026;cond-mat;0;14;;J.Casademunt,W.Zhang,J.Vinals,R.F.Sekerka;Narrow band noise as a model of time-dependent accelerations: study of the stability of a fluid surface in a microgravity environment
hep-th/9210146;hep-th,cond-mat;0;38;;R.Kedem;Thermodynamics of the 3-State Potts Spin Chain
hep-th/9210147;hep-th,hep-ph;0;15;;B.van de Sande,S.Pinsky;Renormalization of Tamm-Dancoff Integral Equations
hep-lat/9210036;hep-lat;0;0;;H.R.Fiebig,R.M.Woloshyn;Meson-Meson Scattering in Lattice QED_2+1
hep-lat/9210037;hep-lat,cond-mat;0;0;;G.Gompper,D.M.Kroll;The Shape of Inflated Vesicles
hep-th/9210148;hep-th;0;0;;W.Li,C.-P.Sun,M.-L.Ge;The l-State Boson Algebra as a Non-Standard Quantum Double and its Universal R-Matrix for Yang-Baxer Equation
hep-ph/9210270;hep-ph;0;17;;P.H.Frampton,D.Ng,M.Sher,Y.Yuan;Search for Heavy Leptons at Hadron Colliders
hep-ph/9210271;hep-ph;0;7;;P.H.Frampton,D.Ng,T.W.Kephart,T.C.Yuan;Search for Dileptons in Z decay
hep-th/9210149;hep-th,cond-mat;0;13;;W.Chen,M.Li;Driving Operators Relevant: A Feature of Chern-Simons Interaction
hep-ph/9210272;hep-ph;0;0;;M.Drees,M.M.Nojiri;New Contribution to Coherent neutralino-Nucleus Scattering
gr-qc/9210016;gr-qc;0;23;;E.Seidel,W.-M.Suen;Towards a Singularity-Proof Scheme in Numerical Relativity
gr-qc/9210017;gr-qc;0;0;;I.H.Redmount,W.-M.Suen;Is Quantum Spacetime Foam Unstable?
gr-qc/9210018;gr-qc;0;0;;W.-M.Suen;Self-Consistence of Semi-Classical Gravity
gr-qc/9210019;gr-qc;0;0;;I.H.Redmount,W.-M.Suen;Path integration in relativistic quantum mechanics
hep-th/9210150;hep-th;1;21;hep-th/9206029;P.Schupp,P.Watts,B.Zumino;Bicovariant Quantum Algebras and Quantum Lie Algebras
hep-ph/9210273;hep-ph;0;23;;K.Cahill;A More Effective Potential
hep-lat/9210038;hep-lat;0;7;;A.J.van der Sijs;Gauge invariant extremization
hep-ph/9210274;hep-ph,astro-ph;0;17;;R.S.Chivukula,A.G.Cohen,M.Luke,M.J.Savage;A Comment on the Strong Interactions of Color-Neutral Technibaryons
hep-th/9210151;hep-th;0;14;;J.-S.Park;Zero-Modes, Covariant Anomaly Counterparts and Reducible Connections in Topological Yang-Mills Theory
hep-th/9210152;hep-th;0;15;;L.Hlavaty;Quantum Braided Groups
hep-th/9210153;hep-th;0;9;;A.Galperin,O.Ogievetsky;Harmonic potentials for symmetric quaternionic sigma-models
hep-ph/9210275;hep-ph;1;17;hep-ph/9209248;G.Burdman;Heavy to Light Semileptonic Transitions in the Heavy Quark Effective Theory
hep-ph/9210276;hep-ph,hep-lat;1;31;hep-ph/9204204;R.S.Chivukula,M.Golden,E.H.Simmons;Critical Constraints on Chiral Hierarchies
hep-th/9210154;hep-th;0;21;;A.Kovner,B.Rosenstein;New Look at QED$_4$: the Photon as a Goldstone Boson and the Topological Interpretation of Electric Charge
hep-th/9210155;hep-th;0;0;;L.A.Dickey;Additional symmetries of KP, Grassmannian, and the string equation II
hep-ph/9210277;hep-ph;0;54;;O.J.P.Eboli,M.C.Gonzalez-Garcia,F.Halzen,S.F.Novaes;Threshold Effects on Heavy Quark Production in $γγ$ Interactions
hep-th/9210156;hep-th;1;26;hep-th/9109007;J.D.Cohn,V.Periwal;Quantizing Effective Strings
hep-lat/9210039;hep-lat;0;39;;A.Patel,S.Sharpe;Perturbative Corrections for Staggered Fermion Bilinears
hep-lat/9210040;hep-lat;0;10;;S.V.Zenkin;On reflection positive formulation of chiral gauge theories on a lattice
hep-ph/9210278;hep-ph;3;38;hep-ph/9203201,hep-ph/9203203,hep-ph/9209227;V.Jain,A.Papadopoulos;On the High $T$ Phase Transition in the Gauged $SU(2)$ Higgs Model
hep-th/9210157;hep-th;1;30;hep-th/9205001;T.Kobayashi,T.Uematsu;q-deformed conformal and Poincaré algebras on quantum 4-spinors
hep-lat/9210041;hep-lat;1;12;hep-lat/9202004;B.Grossmann,M.L.Laursen,T.Trappenberg,U.J.Wiese;The Interface Tension in Quenched QCD at the Critical Temperature
cond-mat/9210027;cond-mat;0;12;;P.Benassi,O.Pilla,G.Viliani,G.Ruocco,G.Signorelli,V.Mazzacurati,M.Montagna;Absence of Definite Scaling Laws in Raman Scattering from Fractals
hep-ph/9210279;hep-ph;0;0;;B.Mukhopadhyaya,D.P.Roy;Tevatron Mass Limits for Heavy Quarks Decaying via Flavor Changing Neutral Current
nucl-th/9210020;nucl-th;0;0;;S.D.Gupta,C.Gale,K.Haglin;Coalescence, Percolation and Nuclear Multifragmentation
hep-th/9210158;hep-th;0;13;;H.O.Girotti,M.Gomes,J.L.deLyra,R.S.Mendes,J.R.S.Nascimento,A.J.da Silva;Attractive Forces Between Electrons in QED$_3$
hep-th/9210159;hep-th;3;32;hep-th/9109005,hep-th/9109025,hep-th/9204051;S.Forste;Non critical super strings on world sheets of constant curvature
astro-ph/9210006;astro-ph;0;0;;E.T.Vishniac;On the Origin of the Galactic Magnetic Field
hep-ph/9210280;hep-ph;0;0;;J.Lopez,D.Nanopoulos,A.Zichichi;The Simplest, String-Derivable, Supergravity Model and its Experimental Predictions
hep-ph/9210281;hep-ph;1;38;hep-ph/0501257;G.P.Korchemsky,G.Marchesini;Structure functions for large $x$ and renormalization of Wilson loops
cond-mat/9210028;cond-mat,hep-th;0;25;;J.Myrheim,K.Olaussen;The Third Virial Coefficient of Free Anyons
math/9210208;math.FA;0;6;;J.Wenzel;Mean Convergence of Vector--valued Walsh Series
math/9210209;math.FA;0;16;;P.F.X.Müller;Two Remarks on Marcinkiewicz decompositions by Holomorphic Martingales
math/9210210;math.FA;0;19;;S.A.Argyros;Weakly Lindelof determined Banach spaces not containing $ℓ^1(N)$
math/9210211;math.FA;0;0;;P.K.Lin;Unrestricted products of contractions in Banach spaces
math/9210212;math.DG,math.FA;0;1;;P.W.Michor;Radon transform and curvature
math/9210213;math.MG;0;0;;N.Alon,D.J.Kleitman;Piercing convex sets
math/9210214;math.NT;0;0;;P.D.T.A.Elliott;Additive functions on shifted primes
math/9210215;math.AP,math.SP;0;0;;F.Gesztesy,W.Karwowski,Z.X.Zhao;New types of soliton solutions
math/9210216;math.DG,math.MG;0;0;;K.Grove,S.Markvorsen;Curvature, triameter, and beyond
math/9210217;math.DS;0;0;;S.P.Hastings,W.C.Troy;A shooting approach to the Lorenz equations
math/9210218;math.MG;0;22;;C.D.Hodgson,I.Rivin,W.D.Smith;A characterization of convex hyperbolic polyhedra and of convex polyhedra inscribed in the sphere
math/9210219;math.GR;0;0;;H.-J.Hoehnke,K.W.Johnson;The 1-, 2-, and 3-characters determine a group
math/9210220;math.FA,math.DS;0;33;;B.R.Hunt;Prevalence: a translation-invariant ``almost every'' on infinite-dimensional spaces
math/9210221;math.GR;0;0;;S.V.Ivanov;On the Burnside problem on periodic groups
math/9210222;math.MG,math.CO;0;0;;J.C.Lagarias,P.W.Shor;Keller's cube-tiling conjecture is false in high dimensions
math/9210223;math.DG,math.GT;0;0;;J.Lohkamp;Negatively Ricci curved manifolds
math/9210224;math.GT,math.CV;0;28;;C.McMullen;Riemann surfaces and the geometrization of 3-manifolds
math/9210225;math.CV,math.GN;0;0;;J.T.Rogers Jr;Is the boundary of a Siegel disk a Jordan curve?
math/9210226;math.AP;0;0;;J.Smoller,A.G.Wasserman,S.-T.Yau,J.B.McLeod;Smooth static solutions of the Einstein-Yang/Mills equation
math/9210227;math.OA;0;0;;X.Wang;Voiculescu theorem, Sobolev lemma, and extensions of smooth algebras
math/9210228;math.DS,math.SG;0;0;;C.Golé;Optical Hamiltonians and symplectic twist maps
math/9210229;math.DS;0;0;;C.Liverani,M.P.Wojtkowski;Ergodicity in Hamiltonian systems
gr-qc/9210020;gr-qc;0;0;;F.Dowker;SO(4) Invariant States in Quantum Cosmology
alg-geom/9210009;alg-geom,math.AG;0;0;;I.Dolgachev,M.Gross;Elliptic Three-folds I: Ogg-Shafarevich Theory
hep-th/9210160;hep-th;0;0;;D.Gershon;Coset Models Obtained by Twisting WZW Models and Stringy Charged Black Holes in Four Dimensions
hep-th/9210161;hep-th;0;14;;H.O.Girotti,M.Gomes,J.L.deLyra,R.S.Mendes,J.R.S.Nascimento,A.J.da Silva;Electron--Electron Bound States in QED$_3$
hep-th/9210162;hep-th;0;0;;F.Yu,Y.-S.Wu;On the KP Hierarchy, $\hat W_∞$ Algebra, and Conformal SL(2,R)/U(1) Model --- The Classical and Quantum Cases
hep-th/9210163;hep-th;0;0;;S.J.Gates,Jr.,H.Nishino;Supersymmetric Soluble Systems Embedded in Supersymmetric Self--Dual Yang--Mills Theory
hep-th/9210164;hep-th;1;25;hep-th/9111035;Z.Qiu;Point-Like Interactions in String Theory Induced by 2-D Topological Gravity
hep-th/9210165;hep-th,gr-qc;0;0;;G.Gilbert,E.Raiten;All Or Nothing: On the Small Fluctuations of Two-Dimensional String-Theoretic Black Holes
hep-lat/9210042;hep-lat,hep-ph;0;0;;J.E.Mandula,M.C.Ogilvie;The Isgur-Wise Limit on the Lattice
astro-ph/9210007;astro-ph,hep-ph;0;26;;B.Fields,S.Dodelson,M.S.Turner;Effect of Neutrino Heating on Primordial Nucleosynthesis
hep-th/9211001;hep-th;0;28;;R.Schimmrigk;Noncritical Dimensions for Critical String Theory: Life beyond the Calabi-Yau Frontier
hep-th/9211002;hep-th;0;0;;T.Isse;Unification of Gravity, Gauge and Higgs Fields by Confined Quantum Fields-Mathematical Formulation-
hep-th/9211003;hep-th;0;32;;F.Falceto,K.Gawedzki;Chern-Simons States at Genus One
hep-th/9211004;hep-th;0;18;;J.Chay,D.K.Hong,T.Lee,S.H.Park;$θ$ Effects in Chern-Simons ${\rm QED}_{2+1}$ with a Four-Fermi Interaction
nucl-th/9211001;nucl-th,hep-ph;0;34;;P.Gonzalez,V.Vento;Pionic effects in deep inelastic scattering off nuclei
hep-th/9211005;hep-th;0;0;;U.Bruzzo,J.A.D.Perez;Line Bundles Over Families of (SUPER) Riemann Surfaces. I: The Non-Graded Case
hep-th/9211006;hep-th;0;0;;U.Bruzzo,J.A.D.Perez;Line Bundles Over Families of (SUPER) Riemann Surfaces. II: The Graded Case
hep-th/9211007;hep-th;0;33;;B.R.Greene,S.D.Mathur,C.M.O'Neill;Eluding the no-hair conjecture: Black holes in spontaneously broken gauge theories
hep-th/9211008;hep-th;0;25;;E.Elizalde,S.D.Odintsov;Gravitational Phase Transitions in Infrared Quantum Gravity
hep-th/9211009;hep-th,cond-mat,funct-an,math.FA;5;42;hep-th/9111005,hep-th/9111043,hep-th/9201016,hep-th/9204089,hep-th/9207084;J.U.Petersen;A Quadratic Deformation of the Heisenberg-Weyl and Quantum Oscillator Enveloping Algebras
hep-lat/9211001;hep-lat;4;10;hep-lat/9207010,hep-lat/9208012,hep-lat/9209007,hep-lat/9209022;UKQCD collaboration,presented by P.W.Stephenson;Pure-gauge SU(2) on large lattices
hep-th/9211010;hep-th;0;34;;M.J.Martins;RG flows and resonance scattering amplitudes
hep-lat/9211002;hep-lat;1;13;hep-lat/9205016;UKQCD Collaboration,-presented by Chris Michael;The Running Coupling from SU(3) Potentials
hep-lat/9211003;hep-lat;0;9;;K.M.Bitar;Hadron Spectroscopy with Dynamical Wilson Fermions at beta=5.3
hep-lat/9211004;hep-lat,hep-ph,nucl-th;0;7;;S.Gupta;The Degrees of Freedom in Hot Quenched QCD
hep-ph/9211201;hep-ph,astro-ph;0;7;;L.Roszkowski;On the COBE Discovery - for Pedestrians
hep-ph/9211202;hep-ph,nucl-th;0;27;;B.-Q.Ma,A.Schaefer,W.Greiner;Flavour Distributions in the Nucleons: SU(2) Sea Asymmetry or Isospin Symmetry Breaking?
hep-ph/9211203;hep-ph;0;35;;H.Dreiner;Bell's Inequality and $τ$-Physics at LEP
hep-ph/9211204;hep-ph;0;59;;J.Butterworth,H.Dreiner;R-Parity Violation at HERA
hep-ph/9211205;hep-ph;0;0;;H.König;QCD Corrections to the Light Higgs Boson Decay into a Charm- Anticharm or Bottom- Antibottom Pair within the Minimal Supersymmetric Model
hep-ph/9211206;hep-ph,astro-ph;0;21;;C.-P.Ma;SO(10) Cosmic Strings and Baryon Number Violation
hep-ph/9211207;hep-ph;1;31;hep-ph/9203220;H.Dreiner,G.K.Leontaris,N.D.Tracas;Ansatz for Quark, Charged Lepton, and Neutrino Masses in SUSY GUTS
hep-lat/9211005;hep-lat,hep-ph;2;10;hep-lat/9204007,hep-lat/9205020;S.Sharpe;Problems with the Quenched Approximation in the Chiral Limit
math/9211201;math.LO;0;0;;J.Brendle;Set-theoretic aspects of periodic $FC$-groups --- extraspecial p-groups and Kurepa trees
math/9211202;math.LO;0;0;;J.Brendle,H.Judah,S.Shelah;Combinatorial properties of Hechler forcing
hep-th/9211011;hep-th;5;20;hep-th/9108001,hep-th/9201061,hep-th/9203042,hep-th/9203052,hep-th/9203054;S.P.Trivedi;Semiclassical Extremal Blackholes
hep-th/9211012;hep-th;0;0;;J.Hietarinta;Some Constant Solutions to Zamolodchikov's Tetrahedron Equations
cond-mat/9211001;cond-mat;0;0;;F.H.L.Essler,V.E.Korepin,K.Schoutens;Exact Solution of an Electronic Model of Superconductivity in 1+1 Dimensions
gr-qc/9211001;gr-qc;0;0;;G.Grignani,G.Nardelli;Chern--Simons Gravity from 3+1 Dimensional Gravity
hep-th/9211013;hep-th;1;18;hep-th/9201017;U.H.Danielsson;Black Hole Uncertainties
hep-lat/9211006;hep-lat;0;4;;J.B.Bronzan,T.E.Vaughan;A Gauge-fixed Hamiltonian for Lattice QCD
gr-qc/9211002;gr-qc;0;0;;L.Parker,J.Z.Simon;Einstein Equation with Quantum Corrections Reduced to Second Order
cond-mat/9211002;cond-mat;0;31;;J.von Delft,C.L.Henley;Spin tunneling in the Kagomé antiferromagnet
hep-th/9211014;hep-th;0;0;;A.Das,C.A.P.Galvao;Self-duality and the Supersymmetric KdV Hierarchy
hep-lat/9211007;hep-lat;0;13;;MILC Collaboration,C.Bernard,T.A.DeGrand,C.DeTar,S.Gottlieb,A.Krasnitz;Finite Size Effects on the QCD Spectrum Revisited
astro-ph/9211001;astro-ph;0;0;;J.I.Katz;A Burst of Speculation
nucl-th/9211002;nucl-th;0;0;;L.Frankfurt,W.R.Greenberg,G.A.Miller,M.Strikman;Sum Rule Description of Color Transparency
hep-ph/9211208;hep-ph,astro-ph;0;0;;L.M.Krauss;Cosmology and Astrophysics 1992
cond-mat/9211003;cond-mat,hep-lat;0;12;;A.Mezhlumian,S.A.Molchanov;Infinite-Scale Percolation in a New Type of Branching Diffusion Processes
hep-th/9211015;hep-th;6;13;hep-th/9202014,hep-th/9202037,hep-th/9205027,hep-th/9208078,hep-th/9210012,hep-th/9210123;R.Kallosh,T.Ortin,A.Peet;Entropy and Action of Dilaton Black Holes
cond-mat/9211004;cond-mat;0;23;;T.C.Hsu,J.C.A.d'Auriac;Level repulsion in integrable and almost-integrable quantum spin models
hep-ph/9211209;hep-ph;0;40;;D.S.Shaw,R.R.Volkas;Systematic Study of Fermion Masses and Mixing Angles in Horizontal SU(2) Gauge Theory
hep-ph/9211210;hep-ph;1;34;hep-th/9205068;J.S.Hagelin,S.Kelley;Evidence For SUSY from GUTS? Evidence For GUTS From SUSY!
hep-th/9211016;hep-th;0;0;;R.C.Myers,V.Periwal;Conformally invariant off-shell string physics
hep-th/9211017;hep-th;0;0;;G.B.Cleaver;Comments on Fractional Superstrings
hep-lat/9211008;hep-lat;1;25;hep-lat/9204014;T.Kalkreuter;Multigrid for propagators of staggered fermions in four-dimensional $SU(2)$ gauge fields
hep-lat/9211009;hep-lat;0;8;;B.Grossmann,M.L.Laursen,T.Trappenberg,U.-J.Wiese;The confined-deconfined interface tension, wetting, and the spectrum of the transfer matrix
astro-ph/9211002;astro-ph;0;24;;P.Baillon,A.Bouquet,Y.Giraud-Héraud,J.Kaplan;Detection of brown dwarfs by the micro-lensing of unresolved stars
hep-ph/9211211;hep-ph,hep-th;0;0;;G.Amelino-Camelia,S.-Y.Pi;Self-consistent Improvement of the Finite Temperature Effective Potential
nucl-th/9211003;nucl-th,hep-ph;0;38;;P.C.Tiemeijer,J.A.Tjon;Meson Mass Spectrum from Relativistic Equations in Configuration Space
hep-lat/9211010;hep-lat;0;15;;M.Hasenbusch,K.Pinn;Surface Tension, Surface Stiffness, and Surface Width of the 3-dimensional Ising Model on a Cubic Lattice
hep-lat/9211011;hep-lat;2;8;hep-lat/9205015,hep-lat/9207014;W.Wilcox;Lattice Charge Overlap and the Elastic Limit
gr-qc/9211003;gr-qc,hep-th;0;17;;K.-T.Pirk;Hadamard States and Adiabatic Vacua
hep-th/9211018;hep-th;0;0;;L.Benoit,Y.Saint-Aubin;Fusion and the Neveu-Schwarz Singular Vectors
hep-th/9211019;hep-th;3;77;hep-th/9201008,hep-th/9202058,hep-th/9207010;K.Ito,J.O.Madsen,J.L.Petersen;Extended Superconformal Algebras from Classical and Quantum Hamiltonian Reduction
hep-th/9211020;hep-th;0;0;;J.Gamboa,C.Ramirez;Hamiltonian Approach to $2D$ Supergravity
hep-th/9211021;hep-th;0;0;;M.Gasperini,G.Veneziano;Pre-Big-Bang in String Cosmology
hep-th/9211022;hep-th;0;11;;A.Kempf;Quantum Group Symmetric Bargmann Fock Construction
hep-th/9211023;hep-th;0;0;;A.Kempf;Approach to Quantum Group deformed Quantum Field Theory
hep-th/9211024;hep-th;0;22;;J.Grundberg,U.Lindstrom,H.Nordstrom;Discretization of the Superparticle Path Integral
hep-th/9211025;hep-th;0;0;;N.Berkovits;Lorentz-Covariant Green-Schwarz Superstring Amplitudes
hep-th/9211026;hep-th,math.QA;0;5;;H.Ewen,O.Ogievetsky;Jordanian Solutions of Simplex Equations
hep-th/9211027;hep-th;1;36;hep-th/9202046;S.Stieberger;Moduli and Twisted Sector Dependence of Z_N x Z_M Orbifold Couplings
gr-qc/9211004;gr-qc,hep-th;0;0;;J.Halliwell,M.Ortiz;Sum-over-histories origin of the composition laws of relativistic quantum mechanics and quantum cosmology
gr-qc/9211005;gr-qc;0;17;;M.D.Francia,G.Goya,R.C.Mercader,H.Vucetich;Mößbauer null redshift experiment II
gr-qc/9211006;gr-qc,hep-th;0;0;;D.Hochberg,T.W.Kephart;Wormhole Cosmology and the Horizon Problem
gr-qc/9211007;gr-qc;0;0;;C.Klimčík,P.Kolník;D=3: Singularities in Gravitational Scattering of Scalar Waves
hep-lat/9211012;hep-lat;0;7;;M.-C.Chu,J.M.Grandy,S.Huang,J.W.Negele;Lattice Analysis of Two-Point Hadronic Correlators in the QCD Vacuum
hep-lat/9211013;hep-lat;0;28;;S.Caracciolo,G.Parisi,A.Pelissetto;Random Walks with Long-Range Self-Repulsion on Proper Time
hep-ph/9211212;hep-ph;0;0;;K.Funakubo,S.Otsuki,K.Takenaga,F.Toyoda;Scattering with Baryon Number Violation -- The Case of Higgs Particle Production --
hep-lat/9211014;hep-lat,cond-mat;1;20;hep-lat/9202004;A.Billoire,T.Neuhaus,B.Berg;Observation of FSS for a First Order Phase Transition
hep-lat/9211015;hep-lat;0;14;;B.Alles,M.Campostrini,A.Feo,H.Panagopoulos;Three-Loop Results on the Lattice
hep-ph/9211213;hep-ph;0;0;;A.Abada,D.Kalafatis,B.Moussallam;On the role of vector mesons in topological soliton stability
hep-th/9211028;hep-th;0;41;;J.Kowalski-Glikman;On the Gupta-Bleuler Quantization of the Hamiltonian Systems with Anomalies
gr-qc/9211008;gr-qc,astro-ph;1;16;0809.0927;D.Hochberg,T.W.Kephart;Gauge Field Back-reaction on a Black Hole
gr-qc/9211009;gr-qc;2;16;gr-qc/9209012,gr-qc/9211008;D.Hochberg,T.Kephart,J.W.York;Positivity of Entropy in the Semi-Classical Theory of Black Holes and Radiation
hep-th/9211029;hep-th;0;13;;M.Chaichian,J.F.Gomes,P.Kulish;Operator Formulation of q-Deformed Dual String Model
hep-ph/9211214;hep-ph;0;39;;J.Pantaleone,A.Halprin,C.N.Leung;Neutrino Mixing due to a Violation of the Equivalence Principle
nucl-th/9211004;nucl-th;0;55;;S.J.Pollock,E.N.Fortson,L.Wilets;Atomic Parity Nonconservation: Electroweak Parameters and Nuclear Structure
hep-th/9211030;hep-th;4;23;hep-th/9111038,hep-th/9204090,gr-qc/9208002,hep-th/9209058;T.Banks,M.O'Loughlin,A.Strominger;Black Hole Remnants and the Information Puzzle
nucl-th/9211005;nucl-th;0;36;;G.Rosensteel;Self-consistent anisotropic oscillator with cranked angular and vortex velocities
hep-lat/9211016;hep-lat;0;5;;A.Hasenfratz;Fermion induced SU$(N)$ Yang-Mills Theory
hep-ph/9211215;hep-ph,hep-th;0;36;;H.La;"Vortex Solution in a Multi-Higgs System and Its Physical Implication,"
hep-th/9211031;hep-th;0;0;;T.Isse;Unification of Gravity, Gauge and Higgs Fields by Confined Quantum Fields II -Effective Theory-
hep-th/9211032;hep-th;0;14;;L.Castellani;R matrix and bicovariant calculus for the inhomogeneous quantum groups IGL_q(n)
hep-th/9211033;hep-th;2;52;hep-th/9201067,hep-th/9207073;S.Penati,D.Zanon;Quantum symmetries in supersymmetric Toda theories
hep-lat/9211017;hep-lat;2;12;hep-lat/9204007,hep-lat/9205020;C.Bernard,M.Golterman;The Quenched Approximation in Health and in Sickness
gr-qc/9211010;gr-qc;0;18;;S.Deser;Gauge (In)variance, Mass and Parity in D=3 Revisited
hep-th/9211034;hep-th;0;0;;W.Nahm,A.Recknagel,M.Terhoeven;Dilogarithm Identities in Conformal Field Theory
hep-th/9211035;hep-th;0;28;;Y.Kim,K.Lee;Vortex Dynamics in Self-Dual Chern-Simons Higgs Systems
hep-ph/9211216;hep-ph;0;15;;B.Grinstein,P.F.Mende;On Constraints for Heavy-Meson Form Factors
hep-ph/9211217;hep-ph;0;4;;M.Smizanska,J.Hrivnac;A Possible Measurement of CP-Violation in B0-decays by ATLAS on LHC
hep-ph/9211218;hep-ph;1;25;hep-ph/9203203;G.C.Marques,R.O.Ramos;Quantum Corrections to Nucleation Rates
hep-ph/9211219;hep-ph;3;29;hep-ph/9203203,hep-ph/9204228,hep-ph/9206227;M.Gleiser,R.O.Ramos;Thermal Fluctuations and Validity of the 1-Loop Effective Potential
hep-ph/9211220;hep-ph;0;11;;R.O.Ramos;Critical Temperature for the $\LAMBDA (\PHI ^4)_4$ Theory within the $\DELTA $ -Expansion
hep-ph/9211221;hep-ph;0;29;;M.Anselmino,S.Forte;Small Angle Polarization in High Energy P--P Scattering Through Nonperturbative Chiral Symmetry Breaking
hep-ph/9211222;hep-ph;0;13;;A.F.Falk,M.Luke,M.B.Wise;Analyticity and the Isgur-Wise Function
hep-ph/9211223;hep-ph;3;26;hep-ph/9206222,hep-ph/9206225,hep-ph/9207249;T.Appelquist,J.Terning;On the Limits of Chiral Perturbation Theory
hep-ph/9211224;hep-ph;0;34;;N.G.Deshpande,E.Keith,P.B.Pal;SU(16) grandunification: breaking scales, proton decay and neutrino magnetic moment
hep-ph/9211225;hep-ph;0;44;;J.-L.Basdevant,E.L.Berger,D.Dicus,C.Kao,S.Willenbrock;Final-State Interaction of Longitudinal Vector Bosons
hep-ph/9211226;hep-ph;4;26;hep-ph/9204206,hep-ph/9204229,hep-ph/9209271,hep-ph/9212277;B.Holdom,M.Sutherland;Simply Modeling Meson HQET
astro-ph/9211003;astro-ph;0;0;;F.Ferrini,B.M.Poggianti;Evolution of Elliptical Galaxies: The Multiphase Model
hep-lat/9211018;hep-lat;0;9;;A.Hulsebos;Gribov Copies and Other Gauge Fixing Beasties on the Lattice
astro-ph/9211004;astro-ph,hep-ph;0;0;;A.Kosowsky,M.S.Turner;Gravitational Radiation from Colliding Vacuum Bubbles: Envelope Approximation to Many-Bubble Collisions
hep-ph/9211227;hep-ph;0;19;;S.Forte;Violation of the Bjorken Sum Rule in QCD
hep-ph/9211228;hep-ph;0;0;;J.Lopez,D.Nanopoulos,H.Pois,A.Zichichi;Proposed Tests for Minimal SU(5) Supergravity at Fermilab, Gran Sasso, SuperKamiokande, and LEP
astro-ph/9211005;astro-ph;0;4;;A.Y.Shiekh;Centri`fugal' Force around a Black Hole
hep-th/9211036;hep-th;0;0;;J.M.Figueroa-O'Farrill,E.Ramos;The Algebra of Differential Operators on the Circle and $\Wkpq $
hep-th/9211037;hep-th;0;22;;Q.-H.Park;A Master Equation for Multi-Dimensional Non-Linear Field Theories
hep-ph/9211229;hep-ph;0;27;;B.Moussallam;Casimir Energy in the Skyrme Model
astro-ph/9211006;astro-ph;0;0;;M.Capaccioli,N.Caon,M.D'Onofrio;The ($\log R_e$, $μ_e$) Plane of Hot Stellar Systems
hep-lat/9211019;hep-lat;0;0;;M.-C.Chu,J.M.Grandy,S.Huang,J.W.Negele;Lattice Calculation of Point-to-Point Hadron Current Correlation
alg-geom/9211001;alg-geom,math.AG;0;7;;D.Huybrechts,M.Lehn;Stable pairs on curves and surfaces
astro-ph/9211007;astro-ph,gr-qc;0;18;;M.Kenmoku,Y.Okamoto,K.Shigemoto;Generalized Einstein Theory on Solar and Galactic Scales
hep-th/9211038;hep-th,cond-mat;0;48;;F.David,B.Duplantier,E.Guitter;Renormalization Theory for Interacting Crumpled Manifolds
hep-ph/9211230;hep-ph;0;0;;D.Comelli;Radiatively Corrected Bound on the Light Higgs Mass in a Minimal Non Minimal Supersymmetric Standard Model
hep-ph/9211231;hep-ph;0;0;;A.D.Dolgov,K.Kainulainen;Fermi-Dirac corrections to relic abundances
gr-qc/9211011;gr-qc;0;21;;S.J.Hughes,D.J.M.Manus,M.A.Vandyck;Weak-Field Gravity of Circular Cosmic Strings
hep-lat/9211020;hep-lat;0;10;;C.Bernard,C.Parrinello,A.Soni;The Gluon Propagator in Momentum Space
hep-th/9211039;hep-th;0;12;;R.Ch.Rashkov;2D Supergravity and Integrable Systems
hep-ph/9211232;hep-ph;0;9;;N.G.Deshpande,E.Keith,P.B.Pal;Implications of LEP Results for SO(10) Grandunification with Two Intermediate Stages
hep-th/9211040;hep-th;0;0;;M.Bershadsky,W.Lerche,D.Nemeschansky,N.P.Warner;Extended N=2 Superconformal Structure of Gravity and W-Gravity Coupled to Matter
hep-ph/9211233;hep-ph;0;14;;D.Pierce;Anomalous prompt photon production in hadronic collisions at low-$x_T$
hep-ph/9211234;hep-ph;0;14;;V.Barger,N.G.Deshpande,J.L.Hewett,T.G.Rizzo;A Separate Higgs?
gr-qc/9211012;gr-qc;0;0;;T.A.Roman;Inflating Lorentzian Wormholes
hep-ph/9211235;hep-ph;0;0;;L.Connors,A.J.Deans,J.S.Hagelin;COBE and SUSY
hep-lat/9211021;hep-lat;0;9;;G.T.Bodwin,E.V.Kovacs;A streamlined method for chiral fermions on the lattice
gr-qc/9211013;gr-qc,hep-th;0;0;;D.Cangemi,M.Leblanc,R.B.Mann;Gauge Formulation of the Spinning Black Hole in (2+1)-Dimensional Anti-de Sitter Space
hep-th/9211041;hep-th;0;0;;S.P.Khastgir,J.Maharana;Wormholes and symmetries of string effective action
hep-th/9211042;hep-th;0;0;;H.Nishino;Self--Dual Supergravity and Supersymmetric Yang--Mills Coupled to Green--Schwarz Superstring
hep-lat/9211022;hep-lat,hep-th;0;20;;C.J.Griffin,T.D.Kieu;How Do Fermions Behave on a Random Lattice?
gr-qc/9211014;gr-qc,hep-th;0;19;;P.Peldan;Unification of Gravity and Yang-Mills Theory in (2+1)-Dimensions
gr-qc/9211015;gr-qc,hep-th;0;22;;N.Mohammedi;Discrete Symmetry, Non-Commutative Geometry and Gravity
hep-lat/9211023;hep-lat;0;0;;W.Beirl,E.Gerstenmayer,H.Markum;Quantum-Gravity Path-Integrals on Simplicial Lattices
hep-ph/9211236;hep-ph;0;22;;T.G.Rizzo;Lepton Number Violating Radiative $W$ Decay in Models with R-parity Violation
nucl-th/9211006;nucl-th;0;0;;K.Maltman;$q^2$-Dependence of Meson Mixing in Few-Body Charge Symmetry Breaking: $π^o-η$ Mixing to One Loop in Chiral Perturbation Theory
hep-th/9211043;hep-th;0;0;;C.-P.Sun;The Canonical Quantization in Terms of Quantum Group and Yang-Baxter Equation
hep-th/9211044;hep-th;0;56;;D.Boyanovsky,H.J.de Vega;Quantum Rolling Down out of Equilibrium
astro-ph/9211008;astro-ph,gr-qc,hep-ph;0;0;;K.Freese,J.J.Levin;The Mad Era: A Possible New Resolution to the Horizon, Flatness, and Monopole Problems
hep-lat/9211024;hep-lat;2;15;hep-lat/9207008,hep-lat/9209020;M.Bowick,P.Coddington,L.Han,G.Harris,E.Marinari;Strings with Extrinsic Curvature: An Analysis of the Crossover Regime
cond-mat/9211005;cond-mat;0;16;;N.I.Karchev,T.S.Hristov;Spin-Wave Theory of the Spiral Phase of the t-J Model
hep-th/9211045;hep-th;0;0;;F.Ferrari;Free and Interacting 2-D Maxwell Field Theory on Conformally Flat Space Times
hep-th/9211046;hep-th;0;38;;S.N.Solodukhin;Non-abelian gauge antisymmetric tensor fields
hep-lat/9211025;hep-lat;0;4;;J.B.Bronzan;Hamiltonian lattice gauge theory: wavefunctions on large lattices
hep-lat/9211026;hep-lat;0;7;;S.Aoki,H.Hirose,Y.Kikukawa;Fermion spectrum in the quenched U(1) chiral Wilson-Yukawa model
hep-lat/9211027;hep-lat;3;10;hep-lat/9204008,hep-lat/9204011,hep-lat/9205016;QCDPAX collaboration,Y.Iwasaki,K.Kanaya,S.Sakai,T.Yoshie,T.Hoshino,T.Shirakawa,Y.Oyanagi;Contamination of Excited States in Quenched QCD Hadron Propagators
hep-lat/9211028;hep-lat;0;26;;I.Montvay;Anomalous Fermion Number Non-Conservation on the Lattice
hep-th/9211047;hep-th;0;0;;M.Kreuzer,H.Skarke;All Abelian Symmetries of Landau-Ginzburg Potentials
hep-th/9211048;hep-th,hep-lat;0;46;;M.Asorey,J.G.Esteve,R.F.J.Salas;Rigorous Analysis of Renormalization Group Pathologies in the 4-State Clock Model
hep-lat/9211029;hep-lat;0;7;;F.Zimmermann,J.Westphalen,M.Göckeler,H.A.Kastrup;Unstable particles in finite volume: The broken phase of the $4$-d $O(4)$ non-linear $σ$-model
hep-ph/9211237;hep-ph;0;9;;E.N.Argyres,C.G.Papadopoulos,R.Kleiss;Multiscalar production amplitudes beyond threshold
hep-lat/9211030;hep-lat;0;14;;M.Goeckeler,G.Schierholz;A method for putting chiral fermions on the lattice
nucl-th/9211007;nucl-th;0;48;;V.Stoks,R.Timmermans,J.J.de Swart;On the pion-nucleon coupling constant
hep-lat/9211031;hep-lat;0;7;;M.Baeker,G.Mack,M.Speh;Multigrid meets Neural Nets
hep-ph/9211238;hep-ph;0;7;;B.H.Smith;Properties of perturbative multi-particle amplitudes in $φ^k$ and $O(N)$ theories
hep-ph/9211239;hep-ph;0;0;;J.Schechter,A.Subbaraman,H.Weigel;Effective Hadron Dynamics: From Meson Masses to the Proton Spin Puzzle
hep-lat/9211032;hep-lat;0;0;;K.Yee;Decoupling of Photon Propagator in Compact QED
hep-th/9211049;hep-th;6;23;hep-th/9108019,hep-th/9111035,hep-th/9203060,hep-th/9209033,hep-th/9209045,hep-th/9209081;J.Lee,P.F.Mende;Semiclassical Tunneling in 1+1 Dimensional String Theory
hep-th/9211050;hep-th;0;33;;E.Alvarez;Some General Problems in Quantum Gravity II: The Three Dimensional Case
hep-th/9211051;hep-th;0;0;;C.N.Pope;Physical States in the $W_3$ String
hep-th/9211052;hep-th;0;32;;F.Ferrari;Multivalued Fields on the Complex Plane and Conformal Field Theories
hep-th/9211053;hep-th;0;43;;A.Fring,G.Mussardo,P.Simonetti;Form Factors for Integrable Lagrangian Field Theories, the Sinh-Gordon Model
hep-lat/9211033;hep-lat;0;12;;S.Catterall,F.Devlin,I.Drummond,R.Horgan,A.Simpson;Non-Relativistic QCD for Heavy Quark Systems
nucl-th/9211008;nucl-th,hep-ph;0;0;;S.Kumano;Test of Scalar Meson Structure in $φ$ Radiative Decays
hep-lat/9211034;hep-lat;0;16;;H.-P.Ying,U.-J.Wiese;Blockspin Scheme and Cluster Algorithm for Quantum Spin Systems
hep-lat/9211035;hep-lat;0;9;;Y.Iwasaki,K.Kanaya,S.Sakai,T.Yoshie;Quark Confinement in Multi-Flavor Quantum Chromodynamics
hep-th/9211054;hep-th;0;23;;P.Schaller,T.Strobl;Canonical Quantization of Non-Einsteinian Gravity and the Problem of Time
hep-ph/9211240;hep-ph;0;19;;R.M.Godbole,P.Roy;Debajyoti Choudhury
hep-ph/9211241;hep-ph;0;0;;A.Dolgov;Antimatter in the Universe
hep-th/9211055;hep-th,gr-qc;0;0;;I.Antoniadis;Dynamics of the conformal factor in 4D gravity
hep-th/9211056;hep-th;4;24;hep-th/9205051,hep-th/9205081,hep-th/9207053,hep-th/9209016;J.P.Gauntlett,J.A.Harvey,J.T.Liu;Magnetic Monopoles in String Theory
hep-th/9211057;hep-th;0;2;;J.Russo;Black hole formation in $c=1$ String Field Theory
hep-lat/9211036;hep-lat;0;18;;C.Bernard,T.A.DeGrand,C.DeTar,S.Gottlieb,A.Krasnitz,R.L.Sugar,D.Toussaint;Baryon Density Correlations in the Quark Plasma, MIMD Lattice Calculation
hep-th/9211058;hep-th;3;32;hep-th/9205100,hep-lat/9207008,hep-lat/9209020;M.Bowick,P.Coddington,L.Han,G.Harris,E.Marinari;The Phase Structure of Strings with Extrinsic Curvature
hep-ph/9211242;hep-ph;0;10;;M.B.Voloshin;Some Properties of Amplitudes at Multi Boson Thresholds in Spontaneously Broken Scalar Theory
gr-qc/9211016;gr-qc;0;21;;W.G.Anderson,P.R.Brady,R.Camporesi;Vacuum Polarisation and the Black Hole Singularity
hep-ph/9211243;hep-ph;0;25;;R.V.Gavai,R.M.Godbole,K.Sridhar;Looking for the gluonic EMC effect in associated $J/ψ$ + $γ$ production
hep-th/9211059;hep-th;4;56;hep-th/9112010,hep-th/9204005,hep-th/9205075,hep-th/9207043;N.Marcus;A tour through N=2 strings
hep-th/9211060;hep-th;0;0;;C.Klimčík,E.Klimčík;On Macroscopic Energy Gap for $q$-Quantum Mechanical Systems
hep-ph/9211244;hep-ph;1;30;hep-ph/9207214;P.Ball,V.M.Braun,H.G.Dosch;Semileptonic Inclusive B--Decays and the Determination of $|V_{ub}|$ from QCD Sum Rules
hep-lat/9211037;hep-lat;1;11;hep-lat/9112002;I.T.Drummond,R.R.Horgan;Improved Langevin Methods for Spin Systems
hep-lat/9211038;hep-lat;0;27;;R.Altmeyer,M.Göckeler,R.Horsley,E.Laermann,G.Schierholz;The Spin Content of the Nucleon
hep-lat/9211039;hep-lat;2;10;hep-lat/9204011,hep-lat/9205016;UKQCD Collaboration,-presented by Sara Collins;Gauge Invariant Smearing and Matrix Correlators using Wilson Fermions at beta=6.2
hep-lat/9211040;hep-lat;1;9;hep-lat/9205016;UKQCD Collaboration,presented by Alan D.Simpson;Quenched Light Hadron Spectroscopy: Comparing the Wilson and O(a)-Improved Fermion Actions
astro-ph/9211009;astro-ph;0;0;;T.Piran,A.Shemi;Fireballs in the Galactic Halo and $γ$-Ray Bursts
gr-qc/9211017;gr-qc,astro-ph,hep-th;0;0;;J.D.Bekenstein;The Relation between Physical and Gravitational Geometry
hep-th/9211061;hep-th;0;0;;A.A.Tseytlin;Finite sigma models and exact string solutions with Minkowski signature metric
hep-ph/9211245;hep-ph,nucl-th;0;12;;D.V.Ahluwalia;Intrinsic Parity of the $(j,0)\oplus (0,j)$ Mesons
hep-ph/9211246;hep-ph;0;13;;E.Nardi;New flavor changing interactions in extended gauge models
hep-ph/9211247;hep-ph;0;23;;M.Butler,M.Savage,R.Springer;Strong and Electromagnetic Decays of the Baryon Decuplet
hep-th/9211062;hep-th,gr-qc;0;7;;W.M.Pezzaglia;Clifford Algebra Derivation of the Characteristic Hypersurfaces of Maxwell's Equations
gr-qc/9211018;gr-qc,hep-th;0;12;;W.M.Pezzaglia Jr;Generalized Fierz Identities and the Superselection Rule for Geometric Multispinors
hep-th/9211063;hep-th;0;35;;M.J.Perry,E.Teo;Topological Conformal Gravity in Four Dimensions
hep-th/9211064;hep-th;0;22;;D.V.Boulatov;Infinite Tension Strings at D>1
hep-th/9211065;hep-th,math.QA;0;20;;B.M.Zupnik;Minimal deformations of the commutative algebra and the linear group GL(n)
gr-qc/9211019;gr-qc;2;80;hep-th/9202054,hep-th/9203079;L.Smolin;What can we learn from the study of non-perturbative quantum general relativity?
hep-th/9211066;hep-th,nlin.SI,solv-int;1;10;hep-th/9205055;M.Jimbo,T.Miwa,A.Nakayashiki;Difference equations for the correlation functions of the eight vertex model
cond-mat/9211006;cond-mat,hep-lat;0;17;;H.G.Evertz,G.Lana,M.Marcu;Cluster Algorithm for Vertex Models
hep-ph/9211248;hep-ph;1;45;hep-ph/9209248;R.Casalbuoni,A.Deandrea,N.D.B.F.Feruglio,R.Gatto,G.Nardulli;Effective Lagrangian for Heavy and Light Mesons: Semileptonic Decays
cond-mat/9211007;cond-mat;0;21;;E.Canessa;Singularity spectrum of self-organized criticality
hep-lat/9211041;hep-lat;0;0;;C.Alexandrou,S.Guesken,F.Jegerlehner,K.Schilling,R.Sommer;Results in the static approximation
hep-lat/9211042;hep-lat;0;55;;C.Alexandrou,S.Guesken,F.Jegerlehner,K.Schilling,R.Sommer;The Static Approximation of Heavy-Light Quark-Systems - A Systematic Lattice Study
hep-ph/9211249;hep-ph;0;40;;U.Ellwanger,M.Lindner;Constraints on New Physics from the Higgs and Top Masses
cond-mat/9211008;cond-mat,hep-th;0;36;;P.Nelson,T.Powers;Rigid Chiral Membranes
hep-ph/9211250;hep-ph;0;59;;N.G.Stefanis,M.Bergmann;On the Nucleon Distribution Amplitude: The Heterotic Solution
hep-ph/9211251;hep-ph;0;52;;N.G.Stefanis,M.Bergmann;Analysis of $Δ^+(1232)$ Isobar Observables, with Improved Quark Distribution Amplitudes
hep-ph/9211252;hep-ph;0;16;;S.Jadach,B.F.L.Ward,S.A.Yost;Exact Results on e+ e- --> e+ e- + 2 Photons at SLC/LEP Energies
hep-th/9211067;hep-th;0;0;;J.-S.Park;BRST and Anti-BRST Quantization of Topological Yang-Mills Theory
hep-th/9211068;hep-th;1;108;hep-th/9108017;C.Gomez,G.Sierra;A brief history of hidden quantum symmetries in Conformal Field Theories
hep-th/9211069;hep-th;0;31;;M.P.Tuite;Monstrous Moonshine and the uniqueness of the Moonshine module
hep-th/9211070;hep-th;0;0;;J.Schiff;Self-Dual Yang-Mills and the Hamiltonian Structures of Integrable Systems
hep-th/9211071;hep-th,cond-mat;0;58;;A.Cappelli,G.V.Dunne,C.A.Trugenberger,G.R.Zemba;Conformal Symmetry and Universal Properties of Quantum Hall States
hep-th/9211072;hep-th;3;36;hep-th/9108004,hep-th/9111048,hep-th/9201056;B.H.Lian,G.J.Zuckerman;New Perspectives on the BRST-algebraic Structure of String Theory
hep-th/9211073;hep-th;0;0;;G.B.Cleaver,D.C.Lewellen;On Modular Invariant Partition Functions for Tensor Products of Conformal Field Theories
hep-th/9211074;hep-th;0;24;;F.Ferrari;Multivalued Fields on the Complex Plane and Braid Group Statistics
hep-lat/9211043;hep-lat;0;13;;A.S.Kronfeld;The Charm Quark on the Lattice
gr-qc/9211020;gr-qc,astro-ph,hep-th;0;21;;J.W.Moffat;Superluminary Universe: A Possible Solution to the Initial Value Problem in Cosmology
hep-ph/9211253;hep-ph;0;14;;G.T.Bodwin,E.Braaten,G.P.Lepage;Rigorous QCD Predictions for Decays of P-Wave Quarkonia
hep-ph/9211254;hep-ph;0;0;;H.J.Lu,S.J.Brodsky;Relating Physical Observables in QCD without Scale-Scheme Ambiguity
hep-ph/9211255;hep-ph,nucl-th;0;94;;F.Schlumpf;Relativistic Constituent Quark Model for Baryons
hep-ph/9211256;hep-ph;0;16;;J.L.Hewett;Can $b→sγ$ Close the Supersymmetric Higgs Production Window?
hep-th/9211075;hep-th;0;35;;S.Hwang,P.Roberts;Interaction and modular invariance of strings on curved manifolds
hep-ph/9211257;hep-ph,astro-ph;0;35;;L.Nellen,K.Mannheim,P.L.Biermann;Neutrino production through hadronic cascades in AGN accretion disks
hep-th/9211076;hep-th,hep-ph;1;28;hep-ph/9205205;D.G.C.McKeon,A.Rebhan;Thermal Green's Functions from Quantum Mechanical Path Integrals
hep-lat/9211044;hep-lat;1;10;hep-lat/9204010;W.Beirl,E.Gerstenmayer,H.Markum,J.Riedler;Gravitational Action Versus Entropy on Simplicial Lattices in Four Dimensions
hep-lat/9211045;hep-lat;2;9;hep-lat/9205016,hep-lat/9208018;UKQCD Collaboration,presented by David Richards;Charmed Meson Spectroscopy and Matrix Elements with an O(a)-Improved Clover Fermion Action
hep-ph/9211258;hep-ph;1;25;hep-ph/9207269;J.C.Romão,J.L.Diaz-Cruz,F.de Campos,J.W.F.Valle;Detection of Intermediate Mass Higgs Bosons from Spontaneously Broken R Parity Supersymmetry
hep-ph/9211259;hep-ph;0;79;;H.Weigel;Vector mesons in the collective approach to SU(3)
astro-ph/9211010;astro-ph;0;49;;T.Piran;Gamma-Ray Bursts and Neutron Star Mergers - Possibly the Strongest Explosions in the Universe
hep-ph/9211260;hep-ph;0;38;;V.Barger,M.S.Berger,R.J.N.Phillips;Implications of $b→sγ$ decay measurements in testing the MSSM Higgs sector
hep-th/9211077;hep-th,math.QA;3;16;hep-th/9201002,hep-th/9203048,hep-th/9204054;E.Celeghini;Quantum algebras and Lie groups
astro-ph/9211011;astro-ph,gr-qc,hep-ph;0;0;;J.J.Levin,K.Freese;A Possible Solution to the Horizon Problem: The Mad Era for Massless Scalar Theories of Gravity
hep-ph/9211261;hep-ph;0;30;;T.E.Clark,B.Haeri,S.T.Love;Wilson Renormalization Group Analysis of Theories with Scalars and Fermions
hep-th/9211078;hep-th;0;0;;R.C.Myers,V.Periwal;Off-shell string physics
hep-ph/9211262;hep-ph;0;36;;K.Cheung;Associated production of Intermediate Higgs or Z-boson with $t \bar t$ pair in $γγ$ collision
hep-ph/9211263;hep-ph,hep-lat;0;14;;A.Duncan,E.Eichten,A.X.El-Khadra,J.M.Flynn,B.R.Hill,H.Thacker;Properties of Low-Lying Heavy-Light Mesons
hep-ph/9211264;hep-ph;0;35;;A.Ferrando,V.Vento;About the realization of chiral symmetry in QCD2
hep-ph/9211265;hep-ph;0;18;;A.Ferrando,V.Vento;Dynamical confinement in bosonized QCD2
hep-ph/9211266;hep-ph,hep-th;3;56;hep-th/9201047,hep-th/9202046,hep-th/9205068;B.de Carlos,J.A.Casas,C.Muñoz;Soft SUSY Breaking Terms in Stringy Scenarios: Computation and Phenomenological Viability
cond-mat/9211009;cond-mat,hep-lat;0;0;;G.G.Batrouni,P.de Forcrand;The fermion sign problem: A new decoupling transformation, and a new simulation algorithm
hep-lat/9211046;hep-lat,hep-ph;0;11;;A.X.El-Khadra;The Charmonium Spectrum on the Lattice: A Status Report
gr-qc/9211021;gr-qc,hep-th;0;0;;M.Gasperini,M.Giovannini;Dilaton Contributions to the Cosmic Gravitational Wave Background
astro-ph/9211012;astro-ph;0;34;;V.Faraoni;On the rotation of polarization by a gravitational lens
nucl-th/9211009;nucl-th;0;11;;H.Mishra,S.P.Misra,P.K.Panda,B.K.Parida;Hot Nuclear Matter : A Variational Approach
hep-lat/9211047;hep-lat,cond-mat;0;10;;H.G.Evertz,M.Marcu;The Loop-Cluster Algorithm for the Case of the 6 Vertex Model
hep-lat/9211048;hep-lat;0;17;;C.Bernard,J.Labrenz,A.Soni;Quenched Lattice Results for $f_B$ and $f_D$
hep-th/9211079;hep-th;4;34;hep-th/9108004,hep-th/9109032,hep-th/9110021,hep-th/9112052;T.Yoneya;Matrix Models and 2D Critical String Theory --2D Black Hole by c=1 Matrix Model--
gr-qc/9211022;gr-qc;2;63;hep-th/9202054,hep-th/9203079;H.Kodama;Quantum Gravity by the Complex Canonical Formulation
hep-lat/9211049;hep-lat,cond-mat;3;15;hep-lat/9202001,hep-lat/9202004,hep-lat/9204005;K.Rummukainen;Multicanonical Cluster Algorithm
hep-lat/9211050;hep-lat;0;12;;H.Gausterer,S.Lee;The Mechanism of Complex Langevin Simulations
hep-th/9211080;hep-th;0;9;;H.Ishikawa,M.Kato;Equivalence of BRST cohomologies for 2-d black hole and c=1 Liouville theory
cond-mat/9211010;cond-mat;0;0;;A.Pelizzola;The half-filled Hubbard model in the pair approximation of the Cluster Variation Method
hep-th/9211081;hep-th;15;56;hep-th/9108011,hep-th/9109038,hep-th/9110004,hep-th/9110053,hep-th/9110065,hep-th/9110067,hep-th/9112044,hep-th/9112070,hep-th/9203039,hep-th/9204046,hep-th/9205046,hep-th/9206077,hep-th/9206078,hep-th/9209052,hep-th/9210015;E.Kiritsis;Exact Duality Symmetries in CFT and String Theory
hep-th/9211082;hep-th,gr-qc;2;21;hep-th/9201021,hep-th/9201061;A.Mikovic;Two-dimensional dilaton gravity in a unitary gauge
hep-th/9211083;hep-th;1;23;hep-th/9110028;I.Bakas,E.Kiritsis;Target Space Description of W-Infinity Symmetry in Coset Models
cond-mat/9211011;cond-mat;0;0;;H.J.Herrmann;On the Thermodynamics of Granular Media
hep-ph/9211267;hep-ph;1;12;hep-ph/9204207;L.Randall,E.Sather;Heavy Meson Hyperfine Splittings: A Puzzle for Heavy Quark Chiral Perturbation Theory
hep-ph/9211268;hep-ph;0;20;;L.Randall,E.Sather;The QCD Scale in the Heavy Quark Expansion
hep-th/9211084;hep-th;0;0;;G.Pradisi,A.Sagnotti;New Developments in Open - String Theories
hep-ph/9211269;hep-ph;0;0;;S.M.Bilenky,C.Giunti;See-Saw Type Mixing and $ ν_μ →ν_τ $ Oscillations
hep-ph/9211270;hep-ph;0;0;;V.Jain;Leading Higgs Mass Dependent Corrections to the Standard Model Lagrangian and its Two Higgs Doublet Extension
hep-ph/9211271;hep-ph;0;3;;F.Borzumati;Resolved Virtual Photon Contributions to inelastic $e-p$ Scattering
hep-ph/9211272;hep-ph;0;0;;G.A.Ladinsky,C.-P.Yuan;A Probe of New Physics in Top Quark Pair Production at $e^-e^+$ Colliders
hep-ph/9211273;hep-ph;0;11;;F.Borzumati;$b →s γ$ and Minimal Supersymmetry
hep-ph/9211274;hep-ph;0;18;;M.Rafecas,V.Vento;Nucleon and delta masses in QCD
gr-qc/9211023;gr-qc;0;6;;N.J.Cornish,J.W.Moffat,D.C.Tatarski;Gravitational Waves in the Nonsymmetric Gravitational Theory
hep-lat/9211051;hep-lat,hep-ph;0;8;;F.Butler,H.Chen,A.Vaccarino,J.Sexton,D.Weingarten;Infinite Volume, Continuum Limit of Valence Approximation Hadron Masses
hep-ph/9211275;hep-ph;2;75;hep-ph/9206249,hep-ph/9206254;C.-P.Yuan;Proposals for Studying TeV $W_L W_L →W_L W_L$ Interactions Experimentally
hep-ph/9211276;hep-ph;0;13;;X.-G.He,J.P.Ma,B.McKellar;CP violation in $J/ψ→Λ\bar Λ$
hep-th/9211085;hep-th;0;0;;S.R.Das;The One Dimensional Matrix Model and String Theory
hep-th/9211086;hep-th;0;0;;S.Randjbar-Daemi,J.Strathdee;The Renormalization Group for Flag Manifolds
hep-lat/9211052;hep-lat;1;7;hep-lat/9206020;C.Vohwinkel;Yet another way to obtain low temperature expansions for discrete spin systems
hep-th/9211087;hep-th;2;22;hep-th/9109019,hep-th/9205002;H.Awata;Exchange Relations for the q-Vertex Operators of $U_q(\widehat {sl2})$
hep-th/9211088;hep-th;0;26;;J.-L.Gervais,L.O'Raifeartaigh,A.V.Razumov,M.V.Saveliev;Gauge Conditions for the Constrained-WZNW--Toda Reductions
hep-th/9211089;hep-th;0;0;;R.Schimmrigk;Novel Flows beteen N=2 Landau-Ginzburg Theories: New Directions in Moduli Space via c=0 Theories
gr-qc/9211024;gr-qc;0;0;;R.Mansouri,M.Mohazzab;Tunneling in Anisotropic Cosmological Models
hep-lat/9211053;hep-lat;0;17;;C.Holm,W.Janke;High precision single-cluster Monte Carlo measurement of the critical exponents of the classical 3D Heisenberg model
gr-qc/9211025;gr-qc;0;19;;L.E.Kidder,C.M.Will,A.G.Wiseman;Spin effects in the inspiral of coalescing compact binaries
hep-ph/9211277;hep-ph;0;15;;M.Y.Wang,E.D.Carlson;Will discrete symmetries help solve the hierarchy problem ?
hep-ph/9211278;hep-ph;0;30;;M.Praszalowicz;Strangeness in the Skyrme and in Nambu-Jona Lasinio Models
hep-ph/9211279;hep-ph;0;12;;E.D.Carlson,M.Y.Wang;Trinification and the Strong P Problem
hep-ph/9211280;hep-ph,astro-ph;0;0;;J.N.Bahcall;Recent Work on Standard Solar Models
hep-th/9211090;hep-th;0;19;;A.Lossev;Descendants constructed from matter fields in topological Landau-Ginzburg theories coupled to topological gravity
hep-ph/9211281;hep-ph;0;20;;W.T.A.ter Veldhuis;Mass of the Lightest Higgs Boson in the Minimal Supersymmetric Standard Model with an Additional Singlet
astro-ph/9211013;astro-ph,hep-ph;0;0;;J.R.Primack;Particle Astrophysics after COBE: Blois92 Summary Talk
hep-ph/9211282;hep-ph;0;0;;K.L.Kowalski,C.C.Taylor;Disoriented Chiral Condensates: A White Paper for the Full Acceptance Detector at the SSC
hep-th/9211091;hep-th,hep-ph;0;13;;N.J.MacKay;On the bootstrap structure of Yangian-invariant factorized S-matrices
hep-ph/9211283;hep-ph;0;46;;R.Alkofer;The Chiral Soliton of the Nambu-Jona-Lasinio Model
cond-mat/9211012;cond-mat,hep-lat;0;0;;P.-M.Binder,V.Privman;Second-Order Dynamics in the Collective Evolution of Coupled Maps and Automata
hep-ph/9211284;hep-ph;0;0;;T.Vachaspati,R.Watkins;Bound States Can Stabilize Electroweak Strings
hep-ph/9211285;hep-ph;0;31;;M.Tanaka;Chiral Structure of the $b→c$ Charged Current and the Semileptonic $Λ_b$ Decay
nucl-th/9211010;nucl-th,hep-ph;0;0;;B.Mueller;Physics of the Quark-Gluon Plasma
hep-ph/9211286;hep-ph;1;18;hep-ph/9207219;J.Lopez,D.Nanopoulos,X.Wang,A.Zichichi;Supersymmetry Tests at Fermilab: A Proposal
hep-ph/9211287;hep-ph;0;7;;R.Foot,H.Lew,R.R.Volkas;Quark-Lepton Symmetry
hep-ph/9211288;hep-ph;0;27;;C.D.Carone,R.T.Hamilton;Flavor Changing Neutral Currents in a Realistic Composite Technicolor Model
gr-qc/9211026;gr-qc,astro-ph;0;15;;P.R.Brady,D.Nunez,S.Sinha;Cauchy horizon singularity without mass inflation
hep-ph/9211289;hep-ph;0;25;;D.O.Carlson,C.-P.Yuan;Studying the Top Quark via the W-Gluon Fusion Process
hep-ph/9211290;hep-ph,hep-th;1;33;hep-th/0509223;F.Wilczek;QCD and Asymptotic Freedom: Perspectives and Prospects
hep-ph/9211291;hep-ph,astro-ph;0;0;;J.N.Bahcall;What Do Solar Models Tell Us About Solar Neutrino Experiments?
cond-mat/9211013;cond-mat,hep-lat;0;35;;T.Poeschel;Granular Material Flowing Down an Inclined Chute: A Molecular Dynamics Simulation
hep-ph/9211292;hep-ph;0;0;;S.P.Martin;Self-Breaking Technicolor
hep-ph/9211293;hep-ph;0;0;;P.I.Krastev;Time Variations of Solar Neutrino Signals and the RSFCN Hypothesis
hep-ph/9211294;hep-ph;0;0;;J.Schechter;Symmetry Breaking in a Generalized Skyrme Model
cond-mat/9211014;cond-mat;0;24;;H.Roeder,A.R.Bishop,J.T.Gammel;Spin-Peierls ground states and frustration in a multi-band Peierls-Hubbard model
cond-mat/9211015;cond-mat;0;0;;P.Ossadnik;Cellular automaton for the fracture of disordered media
hep-th/9211092;hep-th,hep-ph;3;26;hep-th/9109007,hep-th/9201054,hep-th/9205043;Z.Yang;Asymptotic Freedom and Dirichlet String Theory, UR-1288, ER-40685-737
hep-th/9211093;hep-th;0;28;;A.P.Isaev,P.N.Pyatov;GLq(N)-Covariant Quantum Algebras and Covariant Differential Calculus
hep-th/9211094;hep-th;0;0;;L.Feher;Generalized Drinfeld-Sokolov Hierarchies and W-Algebras
hep-th/9211095;hep-th,gr-qc;4;35;hep-th/9109048,hep-th/9201021,hep-th/9201061,hep-th/9203042;F.D.Mazzitelli,J.G.Russo;Dilaton Quantum Cosmology in Two Dimensions
hep-th/9211096;hep-th;0;26;;I.A.Batalin,I.V.Tyutin;On possible generalizations of field--antifield formalism
hep-lat/9211054;hep-lat;0;4;;P.de Forcrand,K.-F.Liu;Glueball wavefunctions
funct-an/9211001;funct-an,math.OA;0;0;;R.Exel;Circle Actions on C*-Algebras, Partial Automorphisms and a Generalized Pimsner-Voiculescu Exact Sequence
funct-an/9211002;funct-an,math.OA;0;0;;W.Arveson;C*-algebras and numerical linear algebra
funct-an/9211003;funct-an,math.OA;0;0;;W.Arveson;Improper filtrations for C*-algebras: spectra of unilateral tridiagonal operators
cond-mat/9211016;cond-mat;0;0;;J.Lee,H.J.Herrmann;Angle of Repose and Angle of Marginal Stability: Molecular Dyanmics of Granular Particles
hep-ph/9211295;hep-ph,nucl-th;0;53;;A.Wirzba;Nuclear Matter Aspects of Skyrmions
hep-lat/9211055;hep-lat;0;9;;S.Gupta,A.Irbaeck;Finite-Size Scaling on the Ising Coexistence Line
hep-lat/9211056;hep-lat;0;14;;G.Muenster,M.Plagge;Study of the complex fermion determinant in a $\rm U(1)_L ⊗U(1)_R$ symmetric Yukawa model
hep-th/9211097;hep-th;3;67;hep-th/9111014,hep-th/9111016,hep-th/9203066;S.Cecotti,C.Vafa;On Classification of N=2 Supersymmetric Theories, (e-mail uncorrupted version)
gr-qc/9211027;gr-qc;0;0;;E.Calzetta,C.E.Hasi;Chaotic Friedmann-Robertson-Walker Cosmology
hep-th/9211098;hep-th;1;11;hep-th/9204019;C.S.Xiong;The generalized KP hierarchy
nucl-th/9211011;nucl-th,hep-ph;0;0;;T.S.Biro,B.Mueller;Magnetic Screening in Thermal Yang-Mills Theories
hep-ph/9211296;hep-ph;0;22;;P.Ball,H.G.Dosch,M.A.Shifman;Remarks on the Heavy-Quark Symmetry in the Complex Plane
nucl-th/9211012;nucl-th;0;19;;N.K.Glendenning,D.Von-Eiff,M.Haft,H.Lenske,M.K.Weigel;Relativistic Mean Field Calculations of $Λ$ and $Σ$ Hypernuclei
hep-ph/9211297;hep-ph;0;120;;P.J.O'Donnell;K and B Physics: a way beyond the Standard Model
math/9211203;math.LO;0;0;;S.D.Friedman;The Genericity Conjecture
math/9211204;math.LO;0;0;;S.D.Friedman;A simpler proof of Jensen's coding theorem
math/9211205;math.LO;0;0;;S.D.Friedman;Minimal universes
hep-lat/9211057;hep-lat;0;6;;R.Gupta,D.Daniel,J.Grandy;Meson Form-factors and Wave-functions with Wilson fermions
hep-ph/9211298;hep-ph;0;0;;S.Weinberg;Conference Summary
hep-th/9211099;hep-th;0;36;;V.Ya.Fainberg,M.A.Soloviev;Non-Localizability and Asymptotic Commutativity
hep-th/9211100;hep-th;3;89;hep-th/9111014,hep-th/9202011,hep-th/9204020;D.Gepner;Foundations of Rational Quantum Field Theory, I
hep-th/9211101;hep-th,hep-ph;0;0;;P.F.Bedaque,A.Das;δ-expansion and self-consistent calculation
hep-th/9211102;hep-th;2;36;hep-th/9210129,hep-th/9211034;R.Kedem,T.R.Klassen,B.M.McCoy,E.Melzer;Fermionic Quasi-Particle Representations for Characters of ${(G^{(1)})_1 ×(G^{(1)})_1 ø(G^{(1)})_2}$
hep-th/9211103;hep-th;0;11;;T.Sano;The Ashtekar Formalism and WKB Wave Functions of N=1,2 Supergravities
hep-th/9211104;hep-th;0;13;;T.Sano,J.Shiraishi;The Non-perturbative Canonical Quantization of the N=1 Supergravity
hep-th/9211105;hep-th,math.QA,nlin.SI,solv-int;0;0;;V.Tarasov;Cyclic monodromy matrices for sl(n) trigonometric R-matrices
hep-th/9211106;hep-th;0;0;;J.L.Cortes,J.Gamboa,L.Velazquez;Electromagnetic Interaction of Anyons in Non-Relativistic Quantum Field Theory
cond-mat/9211017;cond-mat;0;28;;K.Yang,K.L.Warman,S.M.Girvin;Possible Quantum Spin Liquid States on the Triangular and Kagome Lattices
hep-th/9211107;hep-th;2;30;hep-th/9110073,hep-th/9112060;J.de Boer,J.Goeree;The Effective Action of $W_3$ Gravity to All Orders
hep-th/9211108;hep-th;2;29;hep-th/9110073,hep-th/9112060;J.de Boer,J.Goeree;KPZ Analysis for $W_3$ Gravity
hep-ph/9211299;hep-ph,hep-th;0;16;;V.Bhansali,S.D.H.Hsu;A New Anomaly Matching Condition?
nucl-th/9211013;nucl-th;0;44;;V.Stoks,J.J.de Swart;Comparison of potential models with the pp scattering data below 350 MeV
hep-th/9211109;hep-th;3;52;hep-th/9110073,hep-th/9112060,hep-th/9203077;J.de Boer,T.Tjin;Representation theory of finite W algebras
hep-th/9211110;hep-th,hep-ph;4;22;hep-th/9202046,hep-th/9202059,hep-th/9203071,hep-th/9205068;T.R.Taylor;Low-Energy Effective Action of Superstring Theory
hep-th/9211111;hep-th,nlin.SI,solv-int;0;0;;E.K.Sklyanin;Quantum Inverse Scattering Method. Selected Topics
hep-ph/9211300;hep-ph,nucl-th;0;0;;U.-G.Meißner;Chiral Symmetry and Parity--Violating Meson--Nucleon Vertices
hep-ph/9211301;hep-ph;0;7;;S.D.H.Hsu,P.Sikivie;Long Range Forces from Two Neutrino Exchange Revisited
hep-th/9211112;hep-th;0;15;;E.Aldrovandi,L.Bonora,V.Bonservizi,R.Paunov;Free field representation of Toda field theories
cond-mat/9211018;cond-mat;0;26;;M.Wallin,S.M.Girvin;I-V Characteristics of High Temperature Superconductors with Columnar Defects
hep-ph/9211302;hep-ph;2;32;hep-ph/9908362,hep-ph/9908363;M.Neubert;Two-loop corrections to the Isgur-Wise function in QCD sum rules
hep-th/9211113;hep-th;0;38;;C.M.Hull;W-Gravity
hep-th/9211114;hep-th;1;8;hep-th/9206047;H.J.de Vega,A.G.Ruiz;Boundary K-Matrices for the Six Vertex and the n(2n-1) A_{n-1} Vertex Models
funct-an/9211004;funct-an,math.OA;0;0;;R.Exel;Approximately Finite C*-Algebras and Partial Automorphisms
hep-th/9211115;hep-th;0;0;;P.Dorey,F.Ravanini;Generalising the staircase models
hep-th/9211116;hep-th,hep-ph;0;19;;A.Kostelecky,R.Potting;CPT, Strings, and the $K \bar K$ System
hep-th/9211117;hep-th;0;7;;B.Harms,Y.Leblanc;Black Extended Objects, Naked Singularities and P-Branes
hep-lat/9211058;hep-lat,hep-ph,nucl-th;0;0;;D.B.Leinweber,T.D.Cohen;Chiral Corrections to Lattice Calculations of Charge Radii
math/9211206;math.LO;0;15;;A.W.Miller;Measurable rectangles
math/9211207;math.FA;0;0;;N.J.Kalton,S.-C.Tam;Factorization theorems for quasi-normed spaces
math/9211208;math.FA;0;0;;N.J.Kalton,B.Randrianantoanina;Surjective isometries on rearrangement-invariant spaces
math/9211209;math.FA;0;0;;A.Koldobsky;Common subspaces of $L_p$-spaces
math/9211210;math.FA;0;0;;J.Farmer,W.B.Johnson;Polynomial Schur and Polynomial Dunford-Pettis Properties
math/9211211;math.FA;0;24;;H.König,N.Tomczak-Jaegermann;Norms of Minimal Projections
math/9211212;math.FA;0;44;;J.Szulga;Infinite order decoupling of random chaoses in Banach space
math/9211213;math.LO;0;0;;H.Judah,S.Shelah;Baire property and Axiom of Choice
math/9211214;math.LO;0;14;;R.Jin,S.Shelah;Planting Kurepa trees and killing Jech-Kunen trees in a model by using one inaccessible cardinal
math/9211215;math.DS;0;0;;M.Martens;Distortion results and invariant cantor sets of unimodal maps
math/9211216;math.MG,math.FA;0;4;;G.Kuperberg;A low-technology estimate in convex geometry
hep-th/9211118;hep-th;1;15;hep-th/9110065;A.G.Felce,T.M.Samols;Low-Energy Dynamics of String Solitons
hep-lat/9211059;hep-lat;0;8;;J.B.Kogut,J.-F.Lagae;Finite temperature QED3 with light fermions
funct-an/9211005;funct-an,math.OA;0;0;;L.B.Schweitzer;A Short Proof that $M_n(A)$ is local if $A$ is local and Fréchet
hep-th/9211119;hep-th;3;41;hep-th/9111014,hep-th/9111016,hep-th/9202011;E.Zaslow;Topological Orbifold Models and Quantum Cohomology Rings
hep-th/9211120;hep-th;0;0;;M.Terhoeven;Lift of dilogarithm to partition identities
cond-mat/9211019;cond-mat;0;34;;A.H.MacDonald,H.Akera,M.R.Norman;Quantum Mechanics and Superconductivity in a Magnetic Field
hep-ph/9211303;hep-ph;5;27;hep-ph/9203203,hep-ph/9204228,hep-ph/9208231,hep-ph/9209258,hep-ph/9211219;G.Gelmini,M.Gleiser;Kinetics of Sub-Critical Bubbles and the Electroweak Transition
hep-ph/9211304;hep-ph;0;0;;A.J.Buras,M.Jamin,M.E.Lautenbacher,P.H.Weisz;The Two-Loop Anomalous Dimension Matrix for $ΔS=1$ Weak Non-Leptonic Decays I: ${\cal O}(α_s^2)$
hep-ph/9211305;hep-ph;0;43;;F.M.Borzumati,B.A.Kniehl,G.Kramer;Higher-Order QCD Corrections to Inclusive Particle Production in p anti-p Collisions
hep-ph/9211306;hep-ph;0;22;;A.S.Kronfeld,B.Nizic;QCD results for nucleon Compton scattering
hep-ph/9211307;hep-ph;0;0;;K.Enqvist,H.Uibo;Cosmological Neutrino Mass Limit Revisited
hep-ph/9211308;hep-ph;0;11;;S.J.Brodsky,H.J.Lu;On the Self-Consistency of Scale-Setting Methods
hep-ph/9211309;hep-ph,hep-th;1;51;hep-th/9205068;I.Antoniadis,C.Muñoz,M.Quirós;Dynamical supersymmetry breaking with a large internal dimension
hep-ph/9211310;hep-ph;0;31;;N.G.Deshpande,E.Keith,T.G.Rizzo;SO(10) Grand Unification with a Low-Energy $M_R$
hep-ph/9211311;hep-ph;0;21;;M.Gronau,A.Nippe,J.L.Rosner;Method for Flavor Tagging in Neutral B Meson Decays
hep-ph/9211312;hep-ph;0;11;;J.L.Rosner;Electroweak Measurements and Top Quark Mass Limits
hep-ph/9211313;hep-ph;0;17;;A.K.Grant,J.L.Rosner;Quarkonium and Power Law Potentials
funct-an/9211006;funct-an,math.OA;0;0;;L.B.Schweitzer;A Non-Spectral Dense Banach Subalgebra of the Irrational Rotation Algebra
gr-qc/9211028;gr-qc,hep-th;0;17;;A.Anderson;Thawing the Frozen Formalism: The Difference Between Observables and What We Observe
hep-ph/9211314;hep-ph,astro-ph;0;0;;E.J.Weinberg;Vacuum Decay in Theories with Symmetry Breaking by Radiative Corrections
hep-th/9211121;hep-th;0;44;;D.Anselmi,P.Fre';Topological Twist in Four Dimensions, R-Duality and Hyperinstantons
hep-th/9211122;hep-th;0;25;;J.L.Petersen,A.Taormina;Coset Construction and Character Sumrules for the Doubly Extended $N=4$ Superconformal Algebras
hep-lat/9211060;hep-lat;1;9;hep-lat/9206008;W.Bock,J.Smit,J.C.Vink;Staggered fermion approach to chiral gauge theories on the lattice
funct-an/9211007;funct-an,math.OA;0;0;;N.C.Phillips,L.B.Schweitzer;Representable K-theory of Smooth Crossed Products by R and Z
hep-ph/9211315;hep-ph;0;5;;E.Ma;Hints within the standard model on m_t and m_H
hep-ph/9211316;hep-ph;0;12;;J.L.Rosner;Heavy Meson Masses and Decay Constants
hep-ph/9211317;hep-ph;0;0;;J.L.Rosner,M.P.Worah;Model of the Quark Mixing Matrix
hep-ph/9211318;hep-ph;0;8;;J.F.Amundson,J.L.Rosner,M.Worah,M.B.Wise;Test for Right-Handed $b$ Quark Decays
hep-ph/9211319;hep-ph,hep-th;0;39;;M.Bos;Explicit Calculation of the Renormalized Singlet Axial Anomaly
hep-th/9211123;hep-th;0;8;;A.K.Waldron,G.C.Joshi;Gauging octonion algebra
hep-ph/9211320;hep-ph;0;46;;E.Akhmedov,P.Lipari,M.Lusignoli;Matter Effects in Atmospheric Neutrino Oscillations
hep-th/9211124;hep-th;0;33;;D.Atkinson,V.P.Gusynin,P.Maris;Chiral Symmetry Breaking with the Curtis-Pennington Vertex
hep-ph/9211321;hep-ph;0;0;;A.J.Buras,M.Jamin,M.E.Lautenbacher;Two--Loop Anomalous Dimension Matrix for $ΔS=1$ Weak Non-Leptonic Decays II: ${\cal O}(α_e α_s)$
hep-ph/9211322;hep-ph;0;11;;M.Jezabek,J.H.Kuehn;Light Gluinos in $Z^0$ Decays?
hep-th/9211125;hep-th,math.QA;0;21;;T.S.Hakobyan,A.G.Sedrakyan;R-matrices for highest weight representations of sl_q(2,C) at roots of unity
hep-th/9211126;hep-th,nlin.SI,solv-int;1;24;hep-th/9211111;E.K.Sklyanin;Separation of Variables in the Classical Integrable SL(3) Magnetic Chain
hep-th/9211127;hep-th;0;0;;J.Miller,K.De'Bell;Randomly Branched Polymers and Conformal Invariance
hep-lat/9211061;hep-lat;1;7;hep-lat/9206008;W.Bock,C.Frick,J.Smit,J.C.Vink;No strong coupling regime in the fermion-Higgs sector of the standard model
hep-ph/9211323;hep-ph;0;1;;J.F.Gunion;Using Gluon Fusion to Probe CP Violation in the Higgs Sector
hep-ph/9211324;hep-ph;0;1;;J.F.Gunion;Searching for the Minimal Supersymmetric Model Higgs Bosons
funct-an/9211008;funct-an,math.OA;0;0;;V.G.Pestov;An analytic structure emerging in presence of infinitely many odd coordinates
funct-an/9211009;funct-an,math.OA;0;0;;L.B.Schweitzer;Spectral Invariance of Dense Subalgebras of Operator Algebras
hep-lat/9211062;hep-lat;0;0;;A.R.Conway,I.G.Enting,A.J.Guttmann;Algebraic Techniques for Enumerating Self-Avoiding Walks on the Square Lattice
hep-lat/9211063;hep-lat;0;14;;A.R.Conway,A.J.Guttmann;Enumeration of self avoiding trails on a square lattice using a transfer matrix technique
hep-lat/9211064;hep-lat;0;0;;S.Aoki,Y.Kikukawa;Fermion mass in the Wilson-Yukawa approach for chiral Yukawa theory
cond-mat/9211020;cond-mat;0;0;;H.Nakanishi,H.J.Herrmann;Diffusion and spectral dimension on Eden tree
hep-ph/9211325;hep-ph,astro-ph;0;62;;J.Ellis,D.V.Nanopoulos,K.Olive;Flipped Heavy Neutrinos from the Solar Neutrino Problem to Baryogenesis
hep-ph/9211326;hep-ph;0;3;;L.H.Orr,Yu.L.Dokshitzer,V.A.Khoze,W.J.Stirling;Top Width Effects in Soft Gluon Radiation
hep-th/9211128;hep-th;0;0;;R.Perret;A classical N=4 super W_3 algebra
hep-ph/9211327;hep-ph;0;14;;P.M.Stevenson;Response to Brodsky and Lu's Letter "On the Self-Consistency of Scale-Setting Methods
funct-an/9211010;funct-an,math.OA;0;0;;L.B.Schweitzer;Dense m-convex Frechet Subalgebras of Operator Algebra Crossed Products by Lie Groups
hep-lat/9211065;hep-lat;0;0;;J.L.Alonso,P.Boucaud,J.L.Cortes,F.Lesmes,E.Rivas;The S, U and Δρparameters in the Zaragoza proposal for lattice chiral gauge fermions
hep-th/9211129;hep-th,gr-qc;0;33;;J.H.Yoon;Algebraically Special Class of Space-Times and (1+1)-Dimensional Field Theories
hep-th/9211130;hep-th;0;0;;A.Honecker;Automorphisms of W-Algebras and Extended Rational Conformal Field Theories
hep-ph/9211328;hep-ph;0;19;;K.Iida,H.Minakata,O.Yasuda;A test of the equivalence principle by long-baseline neutrino-oscillation experiments
hep-ph/9211329;hep-ph;0;32;;A.Mishra,H.Mishra,S.P.Misra;Effective Potentials in QCD and Chiral Symmetry Breaking
funct-an/9211011;funct-an,math.OA;0;0;;K.Dykema;On certain free product factors via an extended matrix model
funct-an/9211012;funct-an,math.OA;0;0;;K.Dykema;Interpolated free group factors
funct-an/9211013;funct-an,math.OA;0;0;;K.Dykema;Free products of hyperfinite von Neumann algebras and free dimension
hep-th/9211131;hep-th;0;10;;N.L.Khviengia;Large\bf $ w_{1+∞} $--type constraints in two--matrix and Kontsevich model--different approach
hep-th/9211132;hep-th;0;0;;P.D.Vecchia,M.Moshe;On the Double Scaling Limit of O(N) Vector Models in d=2
hep-ph/9211330;hep-ph;0;1;;P.Jain,H.J.Munczek;q\bar q$ Bound States in the Bethe-Salpeter Formalism
hep-ph/9211331;hep-ph;1;28;hep-ph/9206254;D.A.Morris,R.D.Peccei,R.Rosenfeld;Multiple $W_L$ Production from Inelastic $W_L W_L$ Scattering at $\sqrt {\hat s} \gg M_H$
hep-th/9211133;hep-th;2;16;hep-th/9108007,hep-th/9111036;D.Bernard;An Introduction to Yangian Symmetries
hep-th/9211134;hep-th;2;28;hep-th/9202034,hep-th/9203003;A.Koubek;S-Matrices of $φ_{1,2}$ perturbed unitary minimal models: IRF-Formulation and Bootstrap-Program
hep-th/9211135;hep-th,gr-qc;9;38;hep-th/9201021,hep-th/9201061,hep-th/9201074,hep-th/9203042,hep-th/9203052,hep-th/9203054,hep-th/9205069,hep-th/9206087,hep-th/9207006;K.Hamada,A.Tsuchiya;Quantum Gravity and Black Hole Dynamics in 1+1 Dimensions
hep-th/9211136;hep-th;0;0;;F.Belgiorno,A.S.Cattaneo,F.Fucito,M.Martellini;Quantum Models of Black Hole Evaporation
hep-ph/9211332;hep-ph;0;14;;M.R.Ahmady,D.Liu;Exclusive Decays $B →K ψ, B →K^* ψ$ using Heavy Quark Symmetries
hep-th/9211137;hep-th,math.CA;0;0;;A.N.Kirillov;Dilogarithm identities and spectra in conformal field theory
astro-ph/9211014;astro-ph;0;0;;M.E.de Souza;On the General Properties of Matter
hep-th/9211138;hep-th;3;18;hep-th/9108005,hep-th/9111027,hep-th/9204020;P.D.Francesco,J.-B.Zuber;Fusion potentials I
cond-mat/9211021;cond-mat;0;0;;A.H.MacDonald,M.D.Johnson;Magnetic Oscillations of a Fractional Hall Dot
hep-ph/9211333;hep-ph;0;29;;W.Kilian,T.Mannel;QCD Corrected $1/m_b$ Contributions to $B\bbar $--Mixixng
hep-th/9211139;hep-th;0;0;;J.Schnittger,U.Ellwanger;Nonperturbative Conditions for Local Weyl Invariance on a Curved World Sheet
hep-ph/9211334;hep-ph,hep-th;0;23;;P.Arnold,P.Bedaque,A.Das,S.Vokos;On the Analytic Structure of the Self-Energy for Massive Gauge Bosons at Finite Temperature
funct-an/9211014;funct-an,math.OA;0;0;;W.Arveson;Non-commutative spheres and numerical quantum mechanics
funct-an/9211015;funct-an,math.OA;0;0;;W.Arveson;Discretized CCR algebras
hep-th/9211140;hep-th,hep-ph;0;0;;A.Polyakov;A View From the Island
hep-ph/9211335;hep-ph;0;35;;V.A.Kostelecký,M.M.Nieto,D.R.Truax;Supersqueezed States
hep-lat/9211066;hep-lat;0;0;;R.Narayanan;Running Coupling in pure gauge theories using the Schrödinger functional
hep-th/9211141;hep-th,cond-mat,math-ph,math.MP,nlin.SI,solv-int;0;31;;C.A.Tracy,H.Widom;Level-Spacing Distributions and the Airy Kernel
hep-ph/9211336;hep-ph;0;6;;P.Jain,J.P.Ralston;Interpretation of the Color Transparency Experiments
hep-ph/9211337;hep-ph;0;3;;P.Jain,D.W.McKay,H.J.Munczek;Infrared Corrections to the Top Quark Width
hep-ph/9211338;hep-ph;0;27;;K.Yamawaki;Tightly Bound Composite Higgs
hep-th/9212001;hep-th;0;9;;A.Sitarz;Noncommutative Geometry and The Ising Model
hep-th/9212002;hep-th;0;0;;H.Terao;Two Dimensional Black Hole Evapolation in the Light-Cone Gauge
alg-geom/9212001;alg-geom,math.AG;0;0;;J.-P.Demailly,L.Lempert,B.Shiffman;Algebraic approximations of holomorphic maps from Stein domains to projective manifolds
hep-th/9212003;hep-th;0;12;;R.Marnelius;Simple BRST quantization of general gauge models
hep-lat/9212001;hep-lat;1;3;hep-lat/9210022;W.Bock,A.K.De,E.Focht,J.Smit;Chiral fermions in two dimensions?
hep-th/9212004;hep-th;4;22;hep-th/9108004,hep-th/9109005,hep-th/9109024,hep-th/9206053;H.Dorn,H.-J.Otto;Remarks on the continuum formulation of noncritical strings
hep-th/9212005;hep-th;0;0;;D.B.Fairlie,J.Govaerts;Linearisation of Universal Field Equations
hep-ph/9212201;hep-ph;0;9;;S.Dawson;QCD Corrections to Higgs Boson Production
hep-ph/9212202;hep-ph;0;15;;H.Zhang;Global Constraints of Gauss' Law and the Solution to the Strong CP Problem
hep-th/9212006;hep-th;5;252;hep-th/9109048,hep-th/9111056,hep-th/9201056,hep-th/9201059,hep-th/9205068;L.Alvarez-Gaume,M.A.Vazquez-Mozo;Topics in String Theory and Quantum Gravity
hep-th/9212007;hep-th,nlin.SI,solv-int;0;25;;P.P.Kulish,R.Sasaki;Covariance Properties of Reflection Equation Algebras
cond-mat/9212001;cond-mat;0;8;;D.Senechal;The Mass Gap of the Nonlinear Sigma Model through the Finite Temperature Effective Action
hep-ph/9212203;hep-ph;0;37;;M.Ciuchini,E.Franco,G.Martinelli,L.Reina;$ε^′/ε$ at the next-to-leading order in QCD and QED
hep-ph/9212204;hep-ph,astro-ph;0;0;;J.N.Bahcall,H.A.Bethe;Do Solar Neutrino Experiments Imply New Physics?
hep-th/9212008;hep-th;0;10;;C.Pinheiro,G.O.Pires;Extending the Barnes-Rivers Operators to D=3 Topological Gravity
hep-th/9212009;hep-th;0;10;;Bender,Pinsky,van de Sande;Spontaneous Symmetry Breaking of phi4(1+1) in Light Front Field Theory
hep-ph/9212205;hep-ph;0;0;;C.L.Y.Lee;An Analysis of the Decay $B →D^* X ℓ\bar ν_ℓ$ with Predictions from Heavy Quark and Chiral Symmetry
hep-ph/9212206;hep-ph;0;36;;F.Cooper,J.M.Eisenberg,Y.Kluger,E.Mottola,B.Svetitsky;Particle production in the central rapidity region
math/9212201;math.LO;0;0;;S.D.Friedman;Jensen's Σ^* theory and the combinatorial content of V=L
math/9212202;math.LO;0;0;;S.D.Friedman;A large Pi-1-2 set absolute for set forcing
hep-th/9212010;hep-th;1;10;hep-th/9209046;Y.Matsuo;Some Additional Solutions of Conformal Turbulence
hep-th/9212011;hep-th,hep-lat;0;27;;M.I.Dobroliubov,I.I.Kogan,G.W.Semenoff,N.Weiss;Induced QCD Without Local Confinement
hep-ph/9212207;hep-ph;0;24;;V.P.Gudkov,X.-G.He,B.McKellar;On the CP-odd Nucleon Potential
hep-th/9212012;hep-th;0;12;;B.A.Harris,G.C.Joshi;A Self-Consistent Formulation of Quantum Field Theory on $S_4$
hep-ph/9212208;hep-ph;0;64;;K.-ichi.Kondo,M.Tanabashi,K.Yamawaki;Renormalization in the Gauged Nambu--Jona-Lasinio Model
hep-ph/9212209;hep-ph;0;19;;B.E.Hanlon,G.C.Joshi;A Non-Commutative Geometric Approach to Left-Right Symmetric Weak Interactions
hep-lat/9212002;hep-lat,cond-mat;0;0;;K.Yee;Dirac Strings and the Nonperturbative Photon Propagator in Compact QED
hep-lat/9212003;hep-lat;3;17;hep-th/9203019,hep-th/9207086,hep-th/9208002;M.Caselle,A.D'Adda,S.Panzeri;Kazakov-Migdal Induced Gauge Theory and the Coupling of 2D Quantum Gravity to D=1 Matter
hep-th/9212013;hep-th;2;22;hep-th/9108018,hep-th/9208037;L.Castellani;On the quantum Poincare' group
hep-th/9212014;hep-th,hep-lat;0;21;;T.Filk,M.Marcu,B.Scheffold;Monte Carlo Simulations of 2-Dimensional Quantum Gravity Coupled to $c = 1$ Matter
hep-ph/9212210;hep-ph,hep-lat;1;44;hep-ph/9711351;J.Letessier,A.Tounsi,U.Heinz,J.Sollfrank,J.Rafelski;Strangeness Conservation in Hot Nuclear Fireballs
hep-th/9212015;hep-th,cond-mat;0;14;;G.Falkovich,A.Hanany;Spectra of Conformal Turbulence
gr-qc/9212001;gr-qc;0;0;;S.A.Hayward;Cosmic Censorship in 2-Dimensional Dilaton Gravity
hep-th/9212016;hep-th;0;0;;P.West;On the spectrum, no ghost theorem and modular invariance of $W_3$ strings
nucl-th/9212001;nucl-th;0;23;;V.F.Dmitriev;The Nuclear Response in Delta-Isobar Region in the ($^3\!$He,t) Reaction
hep-th/9212017;hep-th;0;0;;H.Lu,B.E.W.Nilsson,C.N.Pope,K.S.Stelle,P.C.West;The Low-level Spectrum of the $W_3$ String
cond-mat/9212002;cond-mat;0;20;;H.U.Baranger,R.A.Jalabert,A.D.Stone;Weak-Localization and Integrability in Ballistic Cavities
hep-ph/9212211;hep-ph;0;74;;S.Ferrara,A.Masiero,M.Porrati;Non Linear Realizations of $SU(2)×U(1)$ in the MSSM: Model Independent Analysis and $g-2$ of $W$ Bosons
hep-ph/9212212;hep-ph;0;23;;J.C.Collins,L.Frankfurt,M.Strikman;Diffractive Hard Scattering with a Coherent Pomeron
hep-ph/9212213;hep-ph;0;15;;J.A.Bagger;Electroweak Symmetry Breaking at the SSC and LHC
hep-th/9212018;hep-th;3;13;hep-th/9108006,hep-th/9110057,hep-th/9112072;M.Carfora,M.Martellini,A.Marzuoli;12j-symbols and four-dimensional quantum gravity
hep-th/9212019;hep-th,chao-dyn,cond-mat,nlin.CD;0;8;;D.A.Lowe;Conformal Models of Two-Dimensional Turbulence
hep-th/9212020;hep-th,gr-qc;5;29;hep-th/9201007,hep-th/9204031,hep-th/9205027,hep-th/9206004,hep-th/9210123;M.Cvetič,S.Griffies,H.H.Soleng;Non-Extreme and Ultra-Extreme Domain Walls and Their Global Space-Times
hep-th/9212021;hep-th;0;0;;G.Ferretti,Z.Yang;Magnetic Fields and Passive Scalars in Polyakov's Conformal Turbulence
hep-ph/9212214;hep-ph;0;25;;O.Pantano,A.Riotto;Dynamics of the Cosmological Quark-Hadron Transition in a Matter Dominated Universe: Distribution and Evolution of Baryon Inhomogeneities
gr-qc/9212002;gr-qc;0;0;;R.D.Pietri,L.Lusanna,M.Pauri;Galilean Theories of Gravitation
hep-th/9212022;hep-th,math.DG;0;0;;C.Nash,D.O.Connor;Determinants of Laplacians, the Ray-Singer Torsion on Lens Spaces and the Riemann zeta function
cond-mat/9212003;cond-mat,hep-lat;0;37;;T.Poeschel;Recurrent Clogging and Density Waves in Granular Material Flowing through a Narrow Pipe
hep-ph/9212215;hep-ph;0;25;;P.G.Silvestrov;Constrained Instanton and Baryon Number Non--Conservation at High Energies
hep-th/9212023;hep-th;3;20;hep-th/9108004,hep-th/9111035,hep-th/9207064;E.Hsu,D.Kutasov;The Gravitational Sine-Gordon Model
hep-th/9212024;hep-th;0;32;;A.Kovner,B.Rosenstein;Quarks as topological defects or what is confined inside a hadron?
hep-th/9212025;hep-th;1;10;hep-th/9205085;H.Sonoda;Current-Current Singularities under External Gauge Fields
gr-qc/9212003;gr-qc;0;20;;C.H.Brans,D.Randall;Exotic Differentiable Structures and General Relativity
gr-qc/9212004;gr-qc;0;19;;A.L.Matacz,A.C.Ottewill,P.C.W.Davies;Quantum Vacuum Instability Near Rotating Stars
hep-th/9212026;hep-th;2;20;hep-th/9205051,hep-th/9205052;R.R.Khuri;Geodesic Scattering of Solitonic Strings
hep-ph/9212216;hep-ph;0;21;;P.Huet;Aspects of the Electroweak Phase Transition
hep-ph/9212217;hep-ph,hep-lat;3;55;hep-lat/9204007,hep-lat/9205020,hep-lat/9211051;S.Sharpe;Recent Progress in Lattice QCD
hep-ph/9212218;hep-ph,nucl-th;0;0;;M.J.Musolf,T.W.Donnelly;Non-Standard Physics and Nucleon Strangeness in Low-Energy PV Electron Scattering
hep-th/9212027;hep-th;4;27;hep-th/9110021,hep-th/9204028,hep-th/9207011,hep-th/9210120;A.Dhar,G.Mandal,S.R.Wadia;A Time-Dependent Classical Solution of C=1 String Field Theory and Non-Perturbative Effects
hep-th/9212028;hep-th;0;22;;S.N.Solodukhin;Supersymmetric Topological Quantum Field Theories Of Differential Forms I. Gauge p-forms
hep-th/9212029;hep-th;1;23;hep-th/9205052;R.R.Khuri;Classical Dynamics of Macroscopic Strings
hep-ph/9212219;hep-ph;4;24;hep-th/9202003,hep-ph/9203206,hep-th/9205011,hep-ph/9205230;K.S.Babu,S.M.Barr;Family Symmetry, Gravity, and the Strong CP Problem
hep-ph/9212220;hep-ph;1;20;hep-ph/9206241;J.G.Korner,D.Pirjol,K.Schilcher;Radiative Decays of the P-Wave Charmed Mesons
hep-ph/9212221;hep-ph;0;8;;B.Basista,P.Suranyi;Hamiltonian Effective Potential
hep-th/9212030;hep-th;1;32;hep-th/9110065;E.A.Bergshoeff,R.Kallosh,T.Ortin;Supersymmetric String Waves
cond-mat/9212004;cond-mat;0;28;;H.Nakanishi,M.Sahimi,M.C.Robertson,C.C.Sammis,M.D.Rintoul;Fractal Properties of the Distribution of Earthquake Hypocenters
hep-ph/9212222;hep-ph;0;14;;K.Charchula,J.Gajewski;Numerical study of radiative corrections in the low $Q^2$ region at HERA
hep-th/9212031;hep-th,math.AP;0;6;;K.Kowalski;Bäcklund transformations for nonlinear evolution equations: Hilbert space approach
hep-th/9212032;hep-th,hep-lat;0;28;;A.Sedrakyan;3D-Ising Model as a String Theory in Three Dimentional Euclidean Space
alg-geom/9212002;alg-geom,math.AG;0;0;;A.Neeman;On the stable rationality of $X/G$
hep-th/9212033;hep-th;1;52;hep-th/9201069;C.Bachas;On the Breakdown of Perturbation Theory
hep-ph/9212223;hep-ph;0;0;;J.Wu,S.Urano,R.Arnowitt;\cl {\bf $τ→μμ{\bar μ}$ and $τ→μe{\bar e}$ Decays in String Models with $\e 6$ Symmetry}
hep-th/9212034;hep-th;0;0;;R.Gass,L.Witten;Do Black Holes Form?
hep-th/9212035;hep-th,gr-qc;2;16;hep-th/9201029,hep-th/9202014;D.Kastor,J.Traschen;Cosmological Multi-Black Hole Solutions
math/9212203;math.FA;0;0;;A.Koldobsky;Operators preserving orthogonality are isometries
math/9212204;math.FA;0;0;;G.Pisier;Interpolation Between $H^p$ Spaces and Non-Commutative Generalizations II
math/9212205;math.FA;0;0;;G.Pisier;On the ``local theory'' of operator spaces
math/9212206;math.FA;0;0;;G.Pisier;Sur les opérateurs factorisables par $OH$
hep-th/9212036;hep-th;0;36;;V.A.Kazakov;D-dimensional Induced Gauge Theory as a Solvable Matrix Model
hep-ph/9212224;hep-ph;2;38;hep-ph/9203201,hep-ph/9203203;P.Huet,K.Kajantie,R.G.Leigh,B.-H.Liu,L.McLerran;Hydrodynamic Stability Analysis of Burning Bubbles in Electroweak Theory and in QCD
hep-th/9212037;hep-th;0;0;;E.Bergshoeff,R.Percacci,E.Sezgin,K.S.Stelle,P.K.Townsend;$U(1)$--Extended Gauge Algebras in $p$-Loop Space
hep-th/9212038;hep-th;1;18;hep-lat/9212005;E.Langmann,G.W.Semenoff;Gribov ambiguity and non-trivial vacuum structure of gauge theories on a cylinder
hep-th/9212039;hep-th;0;0;;K.Kimura;On Free Boson Representations of the Quantum Affine Algebra $U_q(\widehat {\sl }_2)$
hep-th/9212040;hep-th;0;0;;A.Matsuo;Free field realization of $q$-deformed primary fields for $U_q(\widehat {\sl }_2)$
hep-ph/9212225;hep-ph,hep-lat;2;23;hep-lat/9205020,hep-ph/9208253;T.D.Cohen,D.B.Leinweber;The Pion Cloud in Quenched QCD
hep-ph/9212226;hep-ph;3;22;hep-ph/9208256,hep-ph/9209204,hep-ph/9211247;E.Jenkins,M.Luke,A.V.Manohar,M.J.Savage;Chiral Perturbation Theory Analysis of the Baryon Magnetic Moments
hep-th/9212041;hep-th,gr-qc,hep-ph;1;21;hep-ph/9207202;H.La;Time-Dependent Dilatonic Domain Walls
hep-ph/9212227;hep-ph;0;8;;I.I.Bigi,B.Blok,M.Shifman,N.G.Uraltsev,A.Vainshtein;A QCD ``Manifesto'' on Inclusive Decays of Beauty and Charm
hep-lat/9212004;hep-lat;1;9;hep-lat/9206026;P.E.L.Rakow;Magnetic Monopoles in non-compact QED - is there a Phase Transition?
hep-ph/9212228;hep-ph,astro-ph;3;48;hep-ph/9206233,astro-ph/9207001,hep-ph/9207255;L.Perivolaropoulos;On the Statistics of CMB Fluctuations Induced by Topological Defects
cond-mat/9212005;cond-mat;0;23;;D.Cai,A.R.Bishop,A.Sanchez;Length-scale competition in the damped sine-Gordon chain
hep-ph/9212229;hep-ph;0;44;;P.Hernandez,F.J.Vegas;One Loop Effects of Non-Standard Triple Gauge Boson Vertices
astro-ph/9212001;astro-ph;0;30;;H.Falcke,P.L.Biermann,W.J.Duschl,P.G.Mezger;A rotating black hole in the Galactic Center
hep-th/9212042;hep-th;0;17;;J.Pawelczyk;Quark Spin and the Theta-Term for the QCD String
hep-lat/9212005;hep-lat,hep-th;4;19;hep-th/9204083,hep-th/9210011,hep-th/9212038,hep-lat/9305020;J.E.Hetrick;Gauge fixing and Gribov copies in pure Yang-Mills on a circle
cond-mat/9212006;cond-mat,hep-lat;0;14;;U.-J.Wiese,H.-P.Ying;A determination of the low energy parameters of the 2-d Heisenberg antiferromagnet
hep-th/9212043;hep-th;0;0;;E.Getzler;Batalin-Vilkovisky algebras and two-dimensional topological field theories
hep-th/9212044;hep-th;5;41;hep-th/9108009,hep-th/9110017,hep-th/9111056,hep-th/9203054,hep-th/9205069;M.McGuigan;Third Quantization and Black Holes
hep-ph/9212230;hep-ph;1;30;hep-ph/9206230;J.L.Goity;Electromagnetic Mass Splittings in Heavy Mesons
hep-ph/9212231;hep-ph;1;10;hep-ph/9207228;A.C.Mattingly,P.M.Stevenson;Applying Optimized Perturbation Theory to QCD at Low Energies
hep-ph/9212232;hep-ph;0;49;;S.A.Bludman;The First Gauge Theory of Weak Interactions and the Prediction of Weak Neutral Currents
hep-ph/9212233;hep-ph;0;6;;N.G.Uraltsev;FSI phases and CP asymmetries in beauty: QCD point of view
nucl-th/9212002;nucl-th;0;18;;J.R.Shepard,C.E.Price,T.C.Ferrée;Exact 1-Fermion Loop Contributions in 1+1 Dimensional Solitons
hep-th/9212045;hep-th,hep-ph;3;26;hep-th/9202046,hep-th/9204030,hep-th/9205068;I.Antoniadis,E.Gava,K.S.Narain,T.R.Taylor;Superstring Threshold Corrections to Yukawa Couplings
cond-mat/9212007;cond-mat;0;0;;Y.Meir,N.S.Wingreen,P.A.Lee;Low Temperature Transport through a Quantum Dot: The Anderson Model out of Equilibrium
cond-mat/9212008;cond-mat;0;0;;E.Dagotto,J.Riera;Indications of d_{x^2 - y^2} Superconductivity in the Two Dimensional t-J Model
cond-mat/9212009;cond-mat;0;0;;J.Riera,E.Dagotto;Basis Set Reduction Applied to the Two Dimensional t-Jz Model
cond-mat/9212010;cond-mat;0;0;;D.Poilblanc,T.Ziman,H.J.Schulz,E.Dagotto;Dynamical Properties of a Single Hole in an Antiferromagnet
hep-th/9212046;hep-th;0;27;;J.Bieńkowska;Light-Cone Quantization of the Liouville Model
hep-ph/9212234;hep-ph;0;13;;M.J.Booth,G.Jungman;P and T Violation From Certain Dimension Eight Weinberg Operators
hep-ph/9212235;hep-ph;0;40;;P.Arnold,O.Espinosa;The Effective Potential and First-Order Phase Transitions: Beyond Leading Order
hep-ph/9212236;hep-ph;0;11;;A.V.Manohar,M.B.Wise;Exotic QQ\qbar \qbar States in QCD
hep-lat/9212006;hep-lat,hep-th;0;19;;M.Baig,D.Espriu;The Crumpling Transition Revisited
hep-th/9212047;hep-th;0;25;;S.Watamura;Quantum Deformation of BRST Algebra
hep-lat/9212007;hep-lat;0;16;;M.Plagge;INvestigation Of The Biconjugate Gradient Algorithm For The Inversion Of Fermion Matrices
hep-lat/9212008;hep-lat;0;10;;A.A.Khan;Renormalization Group Flow in non-compact QED with two charged staggered Fermions
hep-th/9212048;hep-th;0;0;;P.Ruelle,E.Thiran,J.Weyers;Implications of an arithmetical symmetry of the commutant for modular invariants
hep-th/9212049;hep-th,astro-ph,gr-qc;1;22;hep-th/9109048;R.Brustein,P.Steinhardt;Challenges for Superstring Cosmology
cond-mat/9212011;cond-mat;0;21;;M.C.Marchetti,D.R.Nelson;Translational Correlations in the Vortex Array at the Surface of a Type-II Superconductor
alg-geom/9212003;alg-geom,math.AG;0;0;;S.J.Colley,G.Kennedy;The enumeration of simultaneous higher-order contacts between plane curves
hep-ph/9212237;hep-ph;0;0;;Z.Bern,L.Dixon,D.A.Kosower;The Five Gluon Amplitude and One-Loop Integrals
hep-ph/9212238;hep-ph;0;0;;R.Alkofer,H.Reinhardt;The chiral anomaly and electromagnetic pion decay in effective quark models
hep-ph/9212239;hep-ph,hep-th;0;0;;E.Farhi,V.V.Khoze,R.S.Jr;Minkowski Space Non-Abelian Classical Solutions with Non-Integer Winding Number Change
hep-ph/9212240;hep-ph;0;16;;S.A.Bludman;Cosmological and Astrophysical Bounds on Neutrino Masses and Lifetimes
hep-ph/9212241;hep-ph;0;0;;S.A.Bludman,N.Hata,D.C.Kennedy,P.G.Langacker;Theoretical Implications of the Combined Solar Neutrino Observations
hep-ph/9212242;hep-ph;0;13;;N.A.Tornqvist;Polarization and Handedness in Tau -> 3 Pi + Neutrino Decay Produced in e+e- Annihilations
cond-mat/9212012;cond-mat,hep-lat,hep-th,math-ph,math.MP;0;32;;L.Frachebourg,M.Henkel;Exact Correlation Function at the Lifshitz Points of the Spherical Model
cond-mat/9212013;cond-mat;0;0;;S.Rao,D.Sen;Bosonic Mean Field Theory of the Spiral Phases of Heisenberg Antiferromagnets on a Chain
cond-mat/9212014;cond-mat,hep-lat;0;0;;O.Golinelli,Th.Jolicoeur,R.Lacaze;Dynamical Properties of a Haldane Gap Antiferromagnet
gr-qc/9212005;gr-qc;0;28;;H.H.Soleng;Dark Matter and Non-Newtonian Gravity From General Relativity on a Stringy Background
math/9212207;math.FA;0;0;;G.Pisier;Multipliers and lacunary sets in non-amenable groups
math/9212208;math.FA;0;0;;G.Pisier;Espace de Hilbert d'opérateurs et Interpolation complexe
math/9212209;math.QA;0;0;;A.Cap,P.W.Michor,H.Schichl;A quantum-group-like structure on noncommutative 2-tori
math/9212210;math.DS;0;0;;M.Lyubich;Combinatorics, geometry and attractors of quasi-quadratic maps
cond-mat/9212015;cond-mat;0;33;;N.E.Bonesteel;Theory of Anisotropic Superexchange in Insulating Cuprates
nucl-th/9212003;nucl-th;0;19;;J.A.McNeil,C.E.Price,J.R.Shepard;Relativistic Nuclear Matter with Self-Consistent Correlation Energy
cond-mat/9212016;cond-mat;0;11;;L.Zheng,A.H.MacDonald;Tunneling Conductance Between Parallel Two Dimensional Electron Systems
cond-mat/9212017;cond-mat;0;41;;K.H.Lee,D.Stroud,S.M.Girvin;Flux Pinning and Phase Transitions in Model High-Temperature Superconductors with Columnar Defects
hep-ph/9212243;hep-ph;0;0;;P.Jain,J.P.Ralston,B.Pire;High Energy Hadronic Helicity Violation: What Helicity Flip Form Factors Measure
hep-ph/9212244;hep-ph;0;3;;P.Jain;Consistent Quantum Expansion Around Soliton Solutions
hep-ph/9212245;hep-ph;0;0;;Z.G.Berezhiani,R.Rattazzi;Inverse Hierarchy Approach to Fermion Masses
hep-th/9212050;hep-th;0;0;;V.V.Bazhanov,R.J.Baxter;Star-Triangle Relation for a Three Dimensional Model
hep-th/9212051;hep-th;0;0;;S.Okubo;Triple Products and Yang-Baxter Equation (I): Octonionic and Quaternionic Triple Systems
hep-th/9212052;hep-th;0;0;;S.Okubo;Triple Products and Yang-Baxter Equation (II): Orthogonal and Symplectic Ternary Systems
hep-th/9212053;hep-th,hep-lat;1;13;hep-th/9112048;B.S.Balakrishna;Double Scaling Limit of Scalar Theories on the Lattice
hep-th/9212054;hep-th;0;14;;R.Schimmrigk;Marginal Flows between Mirror Pairs of Landau-Ginzburg String Vacua: Thickening Moduli Space via c=0 Theories
hep-th/9212055;hep-th;1;17;hep-th/9207029;T.A.Larsson;$Z^N$-graded Lie algebras: Fock representations and reducibility conditions
hep-th/9212056;hep-th;0;18;;S.A.Frolov,A.A.Slavnov,C.Sochichiu;On the SO(N) symmetry of the chiral SU(N) Yang--Mills model
hep-th/9212057;hep-th,hep-ph;4;59;hep-th/9203012,hep-th/9206077,hep-ph/9207268,hep-th/9207103;J.Ellis,N.E.Mavromatos,D.V.Nanopoulos;CPT Violation in String-Modified Quantum Mechanics and the Neutral Kaon System
hep-th/9212058;hep-th;0;0;;A.Toon;Particle Content in Topological Field Theories
hep-th/9212059;hep-th;0;19;;F.J.Alexander,S.Habib;Statistical Mechanics of Kinks in (1+1)-Dimensions
hep-th/9212060;hep-th;0;0;;T.Gannon;The Classification of Affine SU(3) Modular Invariant Partition Functions
hep-th/9212061;hep-th;3;19;hep-th/9111021,hep-th/9201005,hep-th/9201017;M.Li;Some remarks on tachyon action in 2d string theory
hep-th/9212062;hep-th;0;41;;J.Distler;Notes on N=2 $σ$-models$
hep-lat/9212009;hep-lat;0;6;;K.Akemi,Ph.deForcrand,M.Fujisaki,T.Hashimoto,H.C.Hege,S.Hioki,O.Miyamura,A.Nakamura,M.O.I.O.Stamatescu,Y.Tago,T.Takaishi;Autocorrelation in Updating Pure SU(3) Lattice Gauge Theory by the use of Overrelaxed Algorithms
gr-qc/9212006;gr-qc;0;0;;S.A.Hayward;On Cosmological Isotropy, Quantum Cosmology and the Weyl Curvature Hypothesis
hep-th/9212063;hep-th;0;0;;B.Broda;A path-integral approach to polynomial invariants of links
hep-th/9212064;hep-th,math.QA;0;0;;N.A.Liskova,A.N.Kirillov;Clebch-Gordan and Racah-Wigner coefficients for $U_q(SU(1,1))$
cond-mat/9212018;cond-mat;1;7;cond-mat/9208012;A.Auerbach;Spin Tunneling, Berry phases and Doped Antiferromagnets
hep-ph/9212246;hep-ph;0;0;;A.Ballestrero,E.Maina,S.Moretti;Heavy Quarks and Leptons at $e^+e^-$ Colliders
hep-lat/9212010;hep-lat,hep-ph;0;0;;Y.Shamir;The Euclidean Spectrum of Kaplan's Lattice Chiral Fermions
hep-ph/9212247;hep-ph;0;0;;S.M.Bilenky;Neutrino Mixing
hep-lat/9212011;hep-lat;0;19;;V.Azcoiti,X.Q.Luo;Phase Structure of Compact $QED_3$ with Massless Fermions
hep-th/9212065;hep-th;1;11;hep-th/9108018;A.Nowicki,E.Sorace,M.Tarlini;The Quantum Deformed Dirac Equation from the k-Poincare` Algebra
hep-ph/9212248;hep-ph,hep-th;8;54;hep-ph/9203201,hep-ph/9203203,hep-ph/9204228,hep-ph/9205232,hep-ph/9206227,hep-ph/9210278,hep-ph/9211211,hep-ph/9212235;J.R.Espinosa,M.Quiros,F.Zwirner;On the nature of the electroweak phase transition
hep-ph/9212249;hep-ph;0;25;;R.N.Mohapatra,T.G.Rizzo;Radiative $W$ and $Z$ Decays and Spontaneous R-Parity Violation
gr-qc/9212007;gr-qc;0;21;;D.J.M.Manus,M.A.Vandyck;Weak-Field Gravity of Revolving Circular Cosmic Strings
hep-lat/9212012;hep-lat;0;14;;S.Caracciolo,R.G.Edwards,A.Pelissetto,A.D.Sokal;Possible Failure of Asymptotic Freedom in Two-Dimensional $RP^2$ and $RP^3$ $σ$-Models
gr-qc/9212008;gr-qc,astro-ph;4;32;astro-ph/9206005,gr-qc/9301010,astro-ph/9303001,gr-qc/9304001;A.L.Matacz;The Coherent State Representation of Quantum Fluctuations in the Early Universe
hep-th/9212066;hep-th;0;0;;C.-P.Sun;Exotic Quantum Double,Its Universal R-matrix And Their Representations
hep-th/9212067;hep-th;3;20;hep-th/9108017,hep-th/9201031,hep-th/9203035;D.Arnaudon;Composition of Kinetic Momenta: The U_q(sl(2)) case
hep-th/9212068;hep-th,hep-ph;0;0;;R.Efraty,V.P.Nair;Chern-Simons Theory and the Quark-Gluon Plasma
hep-th/9212069;hep-th;2;67;hep-th/9109018,hep-th/9205056;J.Feinberg;Stabilised Matrix Models for Non-Perturbative Two Dimensional Quantum Gravity
hep-th/9212070;hep-th;4;28;hep-th/9109054,hep-th/9112053,hep-th/9201001,hep-th/9204019;L.Bonora,C.S.Xiong;Multi-matrix models without continuum limit
hep-ph/9212250;hep-ph;0;39;;F.Schlumpf;Relativistic Constituent Quark Model of Electroweak Properties of Baryons
hep-ph/9212251;hep-ph;0;22;;J.C.Collins;Spin in Perturbative QCD; Coherent Hard Diffraction
nucl-th/9212004;nucl-th,hep-ph;0;0;;W.R.Greenberg,E.L.Lomon;The Lamda-N - Sigma-N Interaction with Isobar Coupling and Six-Quark Resonances
astro-ph/9212002;astro-ph,hep-ph;0;18;;H.A.Feldman,A.E.Evrard;Structure in a Loitering Universe
hep-ph/9212252;hep-ph;0;8;;L.S.Brown,C.Zhai;2 →n threshold production at tree level
hep-th/9212071;hep-th;0;0;;S.Wu;An Integration Formula for the Moment Maps of Circle Actions
hep-th/9212072;hep-th;0;10;;M.Penkava,A.Schwarz;On Some Algebraic Structures Arising in String Theory
funct-an/9212001;funct-an,math.OA;0;0;;A.G.Leiderman,S.A.Morris,V.G.Pestov;The free abelian topological group and the free locally convex space on the unit interval
hep-ph/9212253;hep-ph;0;31;;F.Buccella,M.Lusignoli,G.Mangano,G.Miele,A.Pugliese,P.Santorelli;CP violating asymmetries in charged D meson decays
hep-th/9212073;hep-th;0;26;;J.Ambjorn,A.Sedrakyan,G.Thorleifsson;The 3d Ising Model represented as Random Surfaces
hep-th/9212074;hep-th,hep-lat;2;22;hep-th/9207086,hep-th/9208002;M.Caselle,A.D'Adda,S.Panzeri;The Kazakov-Migdal Model as a High Temperature Lattice Gauge Theory
hep-th/9212075;hep-th;0;0;;C.Schmidhuber;Exactly Marginal Operators and Running Coupling Constants in 2D Gravity
hep-lat/9212013;hep-lat,cond-mat,hep-th;0;21;;M.Caselle,F.Gliozzi,S.Vinti;Finite-Size Effects in the Interface of 3D Ising Model
hep-lat/9212014;hep-lat;0;10;;P.B.Mackenzie;A New Action for Heavy Lattice Fermions
hep-th/9212076;hep-th,nlin.SI,solv-int;3;17;hep-th/9210089,hep-th/9211111,hep-th/9211126;E.K.Sklyanin;Separation of variables in the quantum integrable models related to the Yangian Y[sl(3)]
hep-th/9212077;hep-th;0;2;;K.A.Milton;Maxwell-Chern-Simons Casimir Effect
hep-th/9212078;hep-th;0;17;;P.Menotti,D.Seminara;Closed time like curve and the energy condition in 2+1 dimensional gravity
hep-lat/9212015;hep-lat;0;9;;L.Lin,G.Münster,M.Plagge,I.Montvay,H.Wittig,C.Frick,T.Trappenberg;Mass Spectrum and Bounds on the Couplings in Yukawa Models With Mirror-Fermions
hep-ph/9212254;hep-ph;0;16;;D.Kreimer;2-loop Integrals in the Standard Model
hep-th/9212079;hep-th;0;6;;A.Gamba,I.Kolokolov,M.Martellini;Mean Field Approach to the Giant Wormhole Problem
hep-th/9212080;hep-th;0;0;;M.Martellini,M.Spreafico,K.Yoshida;A Continuum Approach to 2D-Quantum Gravity for C>1
hep-th/9212081;hep-th;4;17;hep-th/9109004,hep-th/9201024,hep-th/9203024,hep-th/9204016;S.Bellucci,E.Ivanov,S.Krivonos;Multi-Field Coset Space Realizations of $w_{1+∞}$
hep-th/9212082;hep-th;0;52;;F.W.Nijhoff,H.W.Capel;Integrable Quantum Mappings and Quantization Aspects of Integrable Discrete-time Systems
hep-ph/9212255;hep-ph;0;0;;H.J.Lipkin;Bose-Einstein Correlations for Mixed Neutral Mesons
hep-th/9212083;hep-th;0;57;;D.Boyanovsky,D.-S.Lee,A.Singh;Phase Transitions out of Equilibrium: domain formation and growth
hep-lat/9212016;hep-lat,hep-ph;0;0;;D.B.Leinweber,T.Draper,R.M.Woloshyn;Baryon Octet to Decuplet Electromagnetic Transitions
nucl-th/9212005;nucl-th;0;0;;M.Matsuo,T.Døssing,E.Vigezzi,R.A.Broglia;Microscopic Origin of Quantum Chaos in Rotational Damping
nucl-th/9212006;nucl-th;0;0;;M.Matsuo,T.Døssing,B.Herskind,S.Frauendorf;Poisson and Porter-Thomas Fluctuations in off-Yrast Rotational Transitions
cond-mat/9212019;cond-mat;0;37;;M.Raykin,A.Auerbach;The $1/N$ Expansion and Spin Correlations in Constrained Wavefunctions
nucl-th/9212007;nucl-th;0;8;;J.G.Congleton;Hyperfine Populations Prior to Muon Capture
hep-th/9212084;hep-th,math.QA;0;0;;A.N.Kirillov;Fusion algebra and Verlinde's formula
hep-ph/9212256;hep-ph;0;20;;K.Sridhar;Shedding light on quarkonium formation by producing a photon in association
hep-th/9212085;hep-th;1;26;hep-th/9109007;M.B.Green;The Influence of World-Sheet Boundaries on Critical Closed String Theory
hep-th/9212086;hep-th;2;17;hep-th/9207061,hep-th/9208057;H.Aratyn,C.P.Constantinidis,L.A.Ferreira,J.F.Gomes,A.H.Zimerman;Hirota's Solitons in the Affine and the Conformal Affine Toda Models
gr-qc/9212009;gr-qc,hep-th;2;16;hep-th/9111045,hep-th/9112008;P.C.Aichelburg,P.Bizon;Magnetically Charged Black Holes and their Stability
hep-ph/9212257;hep-ph,nucl-th;0;0;;V.Bernard,N.Kaiser,U.-G.Meißner;Small Momentum Evolution of the Extended Drell--Hearn--Gerasimov Sum Rule
funct-an/9212002;funct-an,math.OA;0;0;;E.Christensen,A.M.Sinclair;On von Neumann algebras which are complemented subspaces of B(H)
hep-th/9212087;hep-th,math.QA;0;0;;M.J.Bergvelt,A.P.E.ten Kroode;Partitions, Vertex Operator Constructions and Multi-component KP equations
hep-th/9212088;hep-th,hep-lat;0;24;;E.V.Shuryak,J.J.M.Verbaarschot;Random matrix theory and spectral sum rules for the Dirac operator in QCD
hep-ph/9212258;hep-ph;0;0;;P.K.Mohapatra;How unique are the MSW parameters ?
hep-ph/9212259;hep-ph;0;0;;P.K.Mohapatra;Differentiating various extra $Z^′$'s at Future Colliders
hep-ph/9212260;hep-ph;0;15;;J.L.Hewett;Constraints on the Charged Higgs Sector from B Physics
hep-ph/9212261;hep-ph;0;9;;M.A.Doncheski,J.L.Hewett;Signals for Virtual Leptoquark Exchange at Colliders
hep-ph/9212262;hep-ph,astro-ph;0;0;;J.Bahcall;Summary Talk: International Symposium on Neutrino Astrophysics, Takayama/Kamioka (10/'92)
hep-lat/9212017;hep-lat;5;68;hep-lat/9202004,hep-lat/9204005,hep-lat/9204016,hep-lat/9205001,hep-lat/9205018;A.D.Kennedy;Progress in Lattice Field Theory Algorithms
hep-lat/9212018;hep-lat;1;48;hep-lat/9205010;P.B.Mackenzie;Heavy Quark Physics
cond-mat/9212020;cond-mat;0;29;;Z.Weihong,C.J.Hamer;Spin-Wave Theory and Finite-Size Scaling for the Heisenberg Antiferromagnet
cond-mat/9212021;cond-mat,hep-th;0;26;;R.A.Römer,B.Sutherland;Test of Conformal Invariance in One-Dimensional Quantum Liquid with Long-Range Interaction
hep-ph/9212263;hep-ph;0;20;;E.R.Nakamura,K.Kudo,T.Hashimoto,I.Yoneda;Intermittency and Phase Transition
hep-th/9212089;hep-th;0;0;;L.Ibanez,D.Luest;A Comment on Duality Transformations and (Discrete) Gauge Symmetries in Four-Dimensional Strings
hep-th/9212090;hep-th,hep-lat;0;9;;B.Rusakov;Large-N quantum gauge theories in two dimensions
gr-qc/9212010;gr-qc,hep-th;0;0;;A.Casher,F.Englert;Black Hole Tunneling Entropy and the Spectrum of Gravity
hep-th/9212091;hep-th;0;0;;C.R.Hagen;Comment on "Attractive Forces between Electrons in 2 + 1 Dimensional QED"
hep-ph/9212264;hep-ph;0;19;;T.Altherr,E.Petitgirard,T.del Rio Gaztelurrutia;Photon Propagation in Dense Media
cond-mat/9212022;cond-mat;0;17;;F.Guinea,J.Gonzalez,M.A.H.Vozmediano;Electronic interactions in fullerene spheres
hep-th/9212092;hep-th;0;0;;E.Sezgin;Self duality and supersymmetry
hep-ph/9212265;hep-ph;0;22;;U.Ellwanger,L.Vergara;Flow Equations for the Higgs Top System
hep-lat/9212019;hep-lat,hep-ph,hep-th;0;0;;R.Narayanan,H.Neuberger;Infinitely many regulator fields for chiral fermions
nucl-th/9212008;nucl-th,hep-ph;1;81;hep-ph/9207251;T.Barnes,E.S.Swanson;Kaon-Nucleon Scattering Amplitudes and Z$^*$-Enhancements from Quark Born Diagrams
hep-th/9212093;hep-th;1;24;hep-th/9206029;B.Zumino;Differential Calculus on Quantum Spaces and Quantum Groups
hep-ph/9212266;hep-ph;1;24;hep-ph/9908363;M.Neubert,Z.Ligeti,Y.Nir;The Subleading Isgur-Wise Form Factor $χ_3(v\cdot v')$ to Order $α_s$ in QCD Sum Rules
hep-ph/9212267;hep-ph;1;13;hep-ph/9203220;G.K.Leontaris,N.D.Tracas;Predictive Ansatz for Fermion Masses in SUSY GUTS
hep-th/9212094;hep-th,math.QA;0;17;;E.Frenkel,A.Szenes;Dilogarithm identities, q-difference equations and the Virasoro algebra
hep-th/9212095;hep-th,gr-qc;7;33;hep-th/9110065,hep-th/9110067,hep-th/9111044,hep-th/9203039,hep-th/9205046,hep-th/9206077,hep-th/9206078;N.Mohammedi;Arbitrary Spacetimes from the SL(2,R)/U(1) Coset Model
hep-th/9212096;hep-th;0;7;;E.Elizalde,S.Leseduarte,A.Romeo;Spectral Zeta Functions for Spherical Aharonov-Bohm Quantum Bags
hep-th/9212097;hep-th;2;40;hep-th/9109007,hep-th/9201054;A.A.Bytsenko,E.Elizalde,S.D.Odintsov,S.Zerbini;A Finite-Temperature Periodic Structure in (SUPER)STRING Theory
hep-th/9212098;hep-th;0;23;;J.-P.Ader,H.Kachkachi;The Polyakov action on the supertorus
hep-th/9212099;hep-th;3;24;hep-th/9109048,hep-th/9205046,hep-th/9206078;K.Behrndt;The Tachyon in a Linear Expanding Universe
nucl-th/9212009;nucl-th;0;0;;A.Rapisarda;Cross Section Fluctuations and Chaoticity in Heavy-Ion Dynamics
astro-ph/9212003;astro-ph;1;22;astro-ph/9207001;G.F.Smoot,P.J.Steinhardt;Gravity's rainbow
astro-ph/9212004;astro-ph;0;32;;P.J.Steinhardt;Recent advances in extended inflationary cosmology
hep-ph/9212268;hep-ph,hep-th;0;38;;C.Grosse-Knetter,R.Koegerler;Unitary Gauge, Stueckelberg Formalism and Gauge Invariant Models for Effective Lagrangians
hep-ph/9212269;hep-ph;1;4;hep-ph/9206242;V.Pleitez;Comment on ``Chiral Dilepton Model and the Flavor Question''
hep-th/9212100;hep-th;0;0;;T.J.Hollowood,J.L.Miramontes;New Topological Theories and Conjugacy Classes of the Weyl Group
hep-th/9212101;hep-th;0;6;;S.Sachse;A Deformed Poincaré Algebra On A Cubic Lattice
hep-th/9212102;hep-th,cond-mat;0;20;;F.David,B.Duplantier,E.Guitter;Renormalization of Crumpled Manifolds
cond-mat/9212023;cond-mat;0;0;;T.Ala-Nissila,T.Hjelt,J.M.Kosterlitz,O.Venäläinen;Scaling Exponents for Kinetic Roughening in Higher Dimensions
cond-mat/9212024;cond-mat;0;10;;P.Ossadnik;Multiscaling analysis and width of the active zone of large off-lattice DLA
hep-ph/9212270;hep-ph;0;13;;V.D.Duca;Jet inclusive cross sections
hep-ph/9212271;hep-ph;1;19;hep-ph/9206242;J.C.Montero,F.Pisano,V.Pleitez;Neutral Currents and GIM Mechanism in SU(3)_L X U(1)_N Models for Electroweak Interactions
hep-ph/9212272;hep-ph;0;8;;R.Garisto,J.N.Ng;What can the L3 $γγll$ events be?
hep-ph/9212273;hep-ph;0;22;;H.A.Riggs,H.J.Schnitzer;CP-Violating Yukawa Couplings in the Skyrme Model and the Neutron Electric Dipole Moment
gr-qc/9212011;gr-qc;0;15;;M.Rosenbaum,M.P.Ryan,S.Sinha;A Nonlinear Model of a Quantum Minisuperspace System with Back Reaction
hep-ph/9212274;hep-ph;0;28;;P.Cho;Chiral Estimates of Strong CP Violation Revisited
hep-ph/9212275;hep-ph;0;29;;S.Yu.Khlebnikov,R.D.Peccei;Light fermions in composite models
hep-th/9212103;hep-th;2;31;hep-th/9112042,hep-th/9201027;K.Takasaki;Dressing operator approach to Moyal algebraic deformation of selfdual gravity
hep-ph/9212276;hep-ph,hep-th;0;8;;A.Barducci,R.Casalbuoni,G.Pettini,R.Gatto;Discontinuity Theorem for First Order Phase Transitions. Implications for QCD
cond-mat/9212025;cond-mat;0;11;;D.Yoshioka;Fractional Quantum Hall States in Narrow Channels
hep-th/9212104;hep-th;2;16;hep-th/9111062,hep-th/9206031;K.Hornfeck;W-algebras with set of primary fields of dimensions (3, 4, 5) and (3,4,5,6)
hep-lat/9212020;hep-lat;0;0;;V.Azcoiti,G.D.Carlo,A.F.Grillo;Large N Lattice QED
hep-th/9212105;hep-th,alg-geom,math.AG;1;33;hep-th/9112067;G.Falqui,C.-M.Viallet;Singularity, complexity, and quasi--integrability of rational mappings
hep-th/9212106;hep-th;0;29;;F.David;Non-Perturbative Effects in Matrix Models and Vacua of Two Dimensional Gravity
cond-mat/9212026;cond-mat;0;10;;J.Hemmingsson,H.J.Herrmann;On Oscillations in Cellular Automata
hep-lat/9212021;hep-lat;0;0;;T.Kalkreuter;Multigrid Methods for the Computation of Propagators in Gauge Fields
hep-th/9212107;hep-th;1;30;hep-th/9110058;A.Fring;Couplings in Affine Toda Field Theories
nucl-th/9212010;nucl-th;0;44;;L.R.Dodd,D.E.Driscoll;Chiral colour-dielectric model with perturbative quantum pions and gluons
nucl-th/9212011;nucl-th;0;24;;A.Bianconi,S.Boffi,D.E.Kharzeev;Colour Transparency in Hadronic Basis
hep-th/9212108;hep-th;0;6;;P.D.Francesco,C.Itzykson;A Generating Function for Fatgraphs
hep-ph/9212277;hep-ph;2;15;hep-ph/9209268,hep-ph/9211226;B.Holdom,M.Sutherland;Hyperfine Effects and Large $1/m_Q^2$ Corrections
hep-ph/9212278;hep-ph;0;0;;M.Leurer,Y.Nir,N.Seiberg;Mass Matrix Models
nucl-th/9212012;nucl-th;0;41;;C.M.Chen,D.J.Ernst,M.B.Johnson;High-energy pion-nucleus elastic scattering
hep-th/9212109;hep-th;0;37;;J.-L.Gervais;Recent Progress of the Liouville Approach to 2D Gravity and its Toda (W) Generalizations
nucl-th/9212013;nucl-th;0;35;;C.M.Chen,D.J.Ernst,M.B.Johnson;Microscopic approach to pion-nucleus dynamics
hep-ph/9212279;hep-ph,cond-mat;0;0;;S.Rudaz,A.M.Srivastava;On the Production of Flux Vortices and Magnetic Monopoles in Phase Transitions
hep-ph/9212280;hep-ph,hep-th;0;17;;E.N.Argyres,C.G.Papadopoulos,R.Kleiss;On amplitude zeros at threshold
hep-th/9212110;hep-th;1;14;hep-th/9111063;P.R.Devi,T.R.Govindarajan,R.K.Kaul;Three Dimensional Chern-Simons Theory as a Theory of Knots and Links III : Compact Semi-simple Group
hep-th/9212111;hep-th;0;0;;M.Cederwall;$E_7$ as $D=10$ space-time symmetry --- Origin of the twistor transform
hep-ph/9212281;hep-ph;0;42;;J.W.F.Valle;Beyond the Standard Model in Tau Decays
hep-ph/9212282;hep-ph;0;11;;C.O.Escobar,O.L.G.Peres,V.Pleitez,R.Z.Funchal;Constraints on singlet right-handed neutrinos coming from the $Z^0$-width
hep-lat/9212022;hep-lat,cond-mat;0;77;;P.Hasenfratz,F.Niedermayer;Finite size and temperature effects in the AF Heisenberg model
hep-th/9212112;hep-th;0;18;;A.Brandhuber,M.Langer,M.Schweda,O.Piguet,S.P.Sorella;A short comment on the supersymmetric structure of Chern-Simons theory in the axial gauge
gr-qc/9212012;gr-qc;0;18;;C.Klimčík,P.Kolník;Collisions of Einstein-Conformal Scalar Waves
hep-th/9212113;hep-th;8;58;hep-th/9112016,hep-th/9112069,hep-th/9201013,hep-th/9204063,hep-th/9204085,hep-th/9206049,hep-th/9207004,hep-th/9207032;B.Gato-Rivera,A.M.Semikhatov;Singular Vectors and Topological Theories from Virasoro Constraints via the Kontsevich-Miwa Transform
hep-lat/9212023;hep-lat;0;13;;A.K.Bukenov,A.V.Pochinsky,M.I.Polikarpov,L.Polley,U.-J.Wiese;Cosmic Strings on the Lattice
hep-th/9212114;hep-th,hep-lat;7;44;hep-th/9108016,hep-th/9109018,hep-th/9112017,hep-th/9205006,hep-th/9205073,hep-th/9207028,hep-th/9212069;M.Karliner,A.Migdal,B.Rusakov;Ground State of 2D Quantum Gravity and Spectral Density of Random Matrices
hep-th/9212115;hep-th,math.QA;0;17;;D.S.Freed;Higher Algebraic Structures and Quantization
hep-lat/9212024;hep-lat;0;15;;A.K.De,E.Focht,W.Franzki,J.Jersak;How much are 2d Yukawa models similar to the Gross-Neveu models?
nucl-th/9212014;nucl-th;0;14;;B.Shao,N.R.Walet,R.D.Amado;Dynamics of antibaryon-baryon annihilation in the Skyrme model
funct-an/9212003;funct-an,math.OA;0;0;;A.Hopenwasser,C.Laurie;Compression Limit Algebras
hep-th/9212116;hep-th;0;35;;M.M.Nieto;Coherent States and Squeezed States, Supercoherent States and Supersqueezed States
hep-ph/9212283;hep-ph;0;27;;M.M.Nieto;Past, Present, and Possible Future Limits on the Photon Rest Mass
hep-ph/9212284;hep-ph;1;20;hep-ph/9206242;D.Ng;The electroweak theory of SU(3) $×$ U(1)
hep-lat/9212025;hep-lat,hep-ph;0;13;;C.H.L.Smith,N.J.Watson;The Shifted Coupled Cluster Method: A New Approach to Hamiltonian Lattice Gauge Theories
cond-mat/9212027;cond-mat;1;22;cond-mat/9204001;J.Ye,S.Sachdev,N.Read;A Solvable Spin-Glass of Quantum Rotors
cond-mat/9212028;cond-mat;1;16;hep-th/9202057;B.Sutherland,B.S.Shastry;Solution of Some Integrable One-Dimensional Quantum Systems
hep-th/9212117;hep-th;0;0;;H.Lu,C.N.Pope,S.Schrans,X.J.Wang;The Interacting $W_3$ String
hep-ph/9212285;hep-ph;1;70;hep-ph/9205238;S.Fanchiotti,B.Kniehl,A.Sirlin;Incorporation of QCD Effects in Basic Corrections of the Electroweak Theory
hep-lat/9212026;hep-lat,hep-ph;8;60;hep-lat/9107001,hep-lat/9201004,hep-lat/9203001,hep-lat/9205004,hep-lat/9206008,hep-lat/9207034,hep-lat/9209012,hep-lat/9210022;W.Bock,C.Frick,J.Smit,J.C.Vink;Can the Couplings in the Fermion-Higgs Sector of the Standard Model be Strong?
cond-mat/9212029;cond-mat;0;22;;B.S.Shastry,B.Sutherland;Super Lax Pairs and Infinite Symmetries in The $1/r^2$ System
funct-an/9212004;funct-an,math.OA;0;0;;R.Exel;The Soft Torus II: A Variational Analysis of Commutator Norms
hep-th/9212118;hep-th;0;46;;H.Konno;$SU(2)_k×SU(2)_l/SU(2)_{k+l}$ Coset Conformal Field Theory and Topological Minimal Model on Higher Genus Riemann Surface
hep-th/9212119;hep-th;0;42;;G.Mussardo;Correlation Functions in 2-Dimensional Integrable Quantum Field Theories
hep-ph/9212286;hep-ph;2;22;hep-ph/9206216,hep-ph/9211215;H.La;Electroweak Z-string in Two-Higgs-Doublet Standard Model
hep-ph/9212287;hep-ph,nucl-th;0;41;;A.Mishra,H.Mishra,S.P.Misra,S.N.Nayak;QCD at Finite Temperature: A Variational Approach:
hep-lat/9212027;hep-lat,hep-th;1;17;hep-lat/9207035;S.Aoki,A.Gocksch;The Spectrum of the Kazakov Migdal-Model
hep-th/9212120;hep-th;0;2;;J.G.Russo;Classical Solutions in Two-Dimensional String Theory and Gravitational Collapse
hep-ph/9212288;hep-ph;2;0;hep-ph/9203201,hep-ph/9203203;J.Bagnasco,M.Dine;Some Two-Loop Corrections to the Finite Temperature Effective Potential in the Electroweak Theory
hep-lat/9212028;hep-lat;0;16;;S.Ohta;Large scale numerical simulation of the three-state Potts model
hep-ph/9212289;hep-ph;0;20;;Z.Guralnik,A.V.Manohar;QCD Mass Inequalities in the Heavy Quark Limit
hep-ph/9212290;hep-ph;0;23;;M.R.Ahmady,V.Elias,N.C.A.Hill;On-Mass-Shell Renormalization of the $\langle \bar tt \rangle $ Contribution to the $ΔI = 1/2$ $s \leftrightarrow d$ Self-Energy Transition
hep-th/9212121;hep-th;0;15;;V.I.M.G.Marmo,S.Solimeno,F.Zaccaria;Physical nonlinear aspects of classical and quantum q-oscillators
gr-qc/9212013;gr-qc;1;194;0807.0869;M.A.H.MacCallum;Inhomogeneous and anisotropic cosmologies
gr-qc/9212014;gr-qc;0;122;;M.A.H.MacCallum;Anisotropic and inhomogeneous cosmologies
hep-th/9212122;hep-th;0;19;;V.I.Man'ko;Geometrical phase,generalized quasienergy and Floquet operator as invariants
hep-th/9212123;hep-th;0;0;;D.I.Olive,M.V.Saveliev,J.W.R.Underwood;On a Solitonic Specialisation for the General Solutions of Some Two-Dimensional Completely Integrable Systems
hep-lat/9212029;hep-lat;1;19;hep-lat/9107001;K.Jansen,J.Kuti,C.Liu;Strongly Interacting Higgs Sector in the Minimal Standard Model?
hep-lat/9212030;hep-lat;2;10;hep-lat/9206013,hep-lat/9206014;K.Jansen;Chiral Fermions, Anomalies and Chern-Simons Currents on the Lattice
hep-th/9212124;hep-th,cond-mat;0;0;;L.Mezincescu,R.I.Nepomechie;Introduction to the Thermodynamics of Spin Chains
hep-th/9212125;hep-th,cond-mat;0;0;;L.Mezincescu,R.I.Nepomechie,P.K.Townsend,A.M.Tsvelik;Low-Temperature Thermodynamics of $A^{(2)}_2$ and su(3)-invariant Spin Chains
hep-ph/9212291;hep-ph;0;20;;R.Boenisch,C.Grosse-Knetter,R.Koegerler;Bounds on Bess Model Parameters from Vector-Boson Production in e+e- Collisions
hep-ph/9212292;hep-ph;0;0;;R.Oehme;On the Analytic Structure of Hadronic Amplitudes in QCD
hep-ph/9212293;hep-ph;3;45;nucl-th/9211009,hep-ph/9211329,hep-ph/9212287;S.P.Misra;Phase Transitions in Quantum Field Theory
hep-ph/9212294;hep-ph,hep-th;0;0;;J.Wu,R.Arnowitt;Very Large Intermediate Breaking Scale In The Gepner Three Generation Model
hep-ph/9212295;hep-ph;5;28;hep-ph/9206230,hep-ph/9208244,hep-ph/9209239,hep-ph/9209241,hep-ph/9212230;E.Jenkins;Heavy Meson Masses in Chiral Perturbation Theory with Heavy Quark Symmetry
hep-ph/9212296;hep-ph,hep-th;0;0;;C.S.Lam;Multiloop String-Like Formulas for QED
hep-ph/9212297;hep-ph;0;15;;L.Durand,K.Honjo,R.Gandhi,I.Sarcevic,H.Pi;Jets and Jet Multiplicities in High Energy Photon-Nucleon Inetraction:
hep-th/9212126;hep-th;0;10;;H.Dykstra,J.Lykken,E.Raiten;Exact Path Integrals by Equivariant Cohomology
hep-ph/9212298;hep-ph;0;49;;K.Honjo,L.Durand,R.Gandhi,I.Sarcevic,H.Pi;High Energy Photon-Nucleon and Photon-Nucleus Cross Sections
cond-mat/9212030;cond-mat;1;25;cond-mat/9204001;S.Sachdev,J.Ye;Gapless Spin-Fluid Ground State in a Random Quantum Heisenberg Magnet
alg-geom/9212004;alg-geom,math.AG;0;0;;A.Grassi,D.R.Morrison;Automorphisms and the Kähler cone of certain Calabi-Yau manifolds
hep-th/9212127;hep-th;1;34;hep-th/9109046;R.C.Brower,N.Deo,S.Jain,C.-I.Tan;Symmetry Breaking in the Double-Well Hermitian Matrix Models
hep-th/9212128;hep-th;0;18;;K.Ikegami,T.Kimura,R.Mochizuki;Treatment of Constraints in Stochastic Quantization Method and Covariantized Langevin Equation
hep-th/9212129;hep-th;0;0;;R.K.Kaul;Complete Solution of SU(2) Chern-Simons Theory
hep-th/9212130;hep-th;0;14;;R.Mochizuki,K.Yoshida;(D+1)-Dimensional Formulation for D-Dimensional Constrained Systems
hep-th/9212131;hep-th;0;8;;R.Mochizuki,K.Yoshida;Large N Limit on Langevin Equation: Two-Dimensional Nonlinear Sigma Model
hep-th/9212132;hep-th;0;11;;K.Ikegami,R.Mochizuki,K.Yoshida;Dynamical Symmetry Breaking on Langevin Equation : Nambu $\cdot $ Jona-Lasinio Model
hep-th/9212133;hep-th;0;0;;C.Klimcik;Grassmann Integral Topological Invariants
hep-ph/9212299;hep-ph;0;28;;S.A.Abel,W.N.Cottingham,I.B.Whittingham;Spontaneous Baryogenesis in Supersymmetric Models
hep-th/9212134;hep-th;0;18;;O.F.Dayi;A General Solution of the Master Equation for a Class of First Order Systems
hep-th/9212135;hep-th;0;16;;A.R.Its,A.G.Izergin,V.E.Korepin,N.A.Slavnov;Temperature Correlations of Quantum Spins
hep-lat/9212031;hep-lat,hep-ph;0;9;;F.Butler,H.Chen,J.Sexton,A.Vaccarino,D.Weingarten;Hadron Mass Predictions of the Valence Approximation to Lattice QCD
hep-ph/9212300;hep-ph,cond-mat;0;16;;J.F.Nieves,P.B.Pal;The Third Electromagnetic Constant of an Isotropic Medium:
hep-ph/9212301;hep-ph;0;0;;M.James,L.Perivolaropoulos,T.Vachaspati;Detailed Stability Analysis of Electroweak Strings
hep-ph/9212302;hep-ph;0;11;;C.A.Dominguez,J.G.Korner,K.Schilcher;Spectral Functions for Heavy-Light Currents and Form Factor Relations in Hqet
hep-th/9212136;hep-th;16;33;hep-th/9110037,hep-th/9201061,hep-th/9201074,hep-th/9202004,hep-th/9202075,hep-th/9203042,hep-th/9203052,hep-th/9203054,hep-th/9205069,hep-th/9205089,hep-th/9206020,hep-th/9207034,hep-th/9207105,hep-th/9209008,hep-th/9209055,hep-th/9211030;T.Banks,M.O'Loughlin;Nonsingular Lagrangians for Two Dimensional Black Holes
hep-th/9212137;hep-th;1;23;hep-th/9202018;D.A.Ugon,R.Gambini,P.Mora;Knot Invariants for Intersecting Loops
hep-ph/9212303;hep-ph;0;16;;P.Arnold;A Review of the Instability of Hot Electroweak Theory and its Bounds on $m_h$ and $m_t$
hep-ph/9212304;hep-ph;0;0;;P.D.Mannheim;Linear Potentials and Galactic Rotation Curves
hep-ph/9212305;hep-ph;1;32;hep-ph/9203210;J.R.Espinosa,M.Quirós;Upper Bounds on the Lightest Higgs Boson Mass in General Supersymmetric Standard Models
astro-ph/9212005;astro-ph,gr-qc;0;9;;R.H.Price,J.Pullin,P.Kundu;The Escape of Gravitational Radiation from the Field of Massive Bodies
hep-th/9212138;hep-th;1;23;hep-th/9112009;F.Yu;D>2 Topological String
hep-th/9212139;hep-th;7;25;hep-th/9111056,hep-th/9201061,hep-th/9201074,hep-th/9203052,hep-th/9204026,hep-th/9204072,gr-qc/9208002;E.Elizalde,S.Naftulin,S.D.Odintsov;One Loop Counterterms in 2D Dilaton-Maxwell Quantum Gravity
hep-th/9212140;hep-th,gr-qc;0;20;;I.Antoniadis,S.D.Odintsov;Conformal dynamics of quantum gravity with torsion
hep-th/9212141;hep-th;0;0;;L.Castellani;U_q(N) Gauge Theories
hep-th/9212142;hep-th;1;24;hep-th/9204070;A.Smailagic,E.Spallucci;General treatment of anomalies in (1,0) and (1,1) two-dimensional super-gravity
hep-th/9212143;hep-th;0;0;;P.Dorey;Hidden geometrical structures in integrable models
hep-th/9212144;hep-th;0;0;;R.Brooks;Diff(SIGMA) and Metrics from Hamiltonian-TQFT's in 2+1 Dimensions
cond-mat/9212031;cond-mat;0;40;;M.Troyer,H.Tsunetsugu,T.M.Rice,J.Riera,E.Dagotto;Spin Gap and Superconductivity in the One-Dimensional t-J Model with Coulomb Repulsion
hep-th/9212145;hep-th,cond-mat;0;0;;A.M.Polyakov;The Theory of Turbulence in Two Dimensions
hep-ph/9212306;hep-ph;0;27;;D.-di.Wu,C.Kao;A Z' Model Which May Be Relevant to the New LEP Events
hep-ph/9212307;hep-ph;0;15;;J.F.Donoghue,J.Tandean;The Equivalence Theorem and Global Anomalies
hep-th/9212146;hep-th;0;0;;S.Mignemi,N.R.Stewart;Charged black holes in effective string theory
hep-th/9212147;hep-th;0;0;;A.Khare,U.P.Sukhatme;New Shape Invariant Potentials in Supersymmetric Quantum Mechanics
hep-th/9212148;hep-th,hep-lat,hep-ph;1;38;hep-th/9109007;D.J.Gross;Some New/Old Approaches to QCD
hep-th/9212149;hep-th,hep-ph;1;24;hep-th/9109007;D.J.Gross;Two Dimensional QCD as a String Theory
hep-lat/9212032;hep-lat;0;0;;A.J.Guttmann,I.G.Enting;Series studies of the Potts model. I: The simple cubic Ising model
hep-th/9212150;hep-th,math.CA,math.CO;0;0;;A.N.Kirillov;Dilogarithm identities, partitions and spectra in conformal field theory, I
hep-th/9212151;hep-th;1;61;hep-th/9208010;S.Majid;Beyond Supersymmetry and Quantum Symmetry (an introduction to braided groups and braided matrices)
hep-lat/9212033;hep-lat,cond-mat,hep-th;0;14;;A.Krasnitz,R.Potting;A realistic heat bath: theory and application to kink-antikink dynamics
hep-lat/9212034;hep-lat;0;0;;K.Bitar,R.G.Edwards,U.M.Heller,A.D.Kennedy;On the Dynamics of Light Quarks in QCD
hep-lat/9212035;hep-lat,hep-ph;0;16;;C.Bernard,Y.Shen,A.Soni;Calculating the Isgur-Wise Function on the Lattice
hep-ph/9212308;hep-ph,hep-th;0;0;;Z.Bern,L.Dixon,D.A.Kosower;Dimensionally Regulated One-Loop Integrals
hep-ph/9212309;hep-ph;0;27;;V.A.Rubakov,D.T.Son,P.G.Tinyakov;An Example of Semiclassical Instanton-Like Scattering: (1+1) Dimensional Sigma Model
nucl-th/9212015;nucl-th;0;0;;M.Matsuo,T.Døssing,B.Herskind,S.Frauendorf,E.Vigezzi,R.A.Broglia;Chaotic Behavior in Warm Deformed Nuclei Induced by Residual Two-Body Interactions
cond-mat/9212032;cond-mat;0;22;;D.I.Golosov,M.I.Kaganov;Spatial Correlation of Conduction Electrons in Metal with Complicated Geometry Of The Fermi Surface
hep-ph/9212310;hep-ph;0;52;;A.Mishra,S.P.Misra;Gluon Condensates, Chiral Symmetry Breaking and Pion Wave Function
hep-ph/9212311;hep-ph;0;0;;H.B.Kim,J.E.Kim;An Orbifold Compactification with Three Families from Twisted Sectors
hep-th/9212152;hep-th,math.CO;0;12;;A.N.Kirillov;Unimodality of generalized Gaussian coefficients
hep-th/9212153;hep-th;0;17;;E.E.Donets,D.V.Gal'Tsov;Stringy Sphalerons and Non-Abelian Black Holes
cond-mat/9212033;cond-mat,hep-th;0;30;;D.Li;Hierarchical Wave Functions and Fractional Statistics in Fractional Quantum Hall Effect on the Torus
cond-mat/9212034;cond-mat,hep-th;1;24;hep-th/9110061;D.Li;Hierarchical Wave Functions of Fractional Quantum Hall Effect on the Torus
hep-ph/9212312;hep-ph;0;20;;Y.Yasui,I.Watanabe,J.Kodaira,I.Endo;Measuring the Beam Polarizations and the Luminosity at Photon-Photon Colliders
nucl-th/9212016;nucl-th;0;29;;C.J.Benesh,J.L.Friar;Electromagnetic Dissociation of Nuclei in Heavy-Ion Collisions
hep-th/9212154;hep-th;2;31;hep-th/9108006,hep-th/9110057;M.Fukuma,S.Hosono,H.Kawai;Lattice Topological Field Theory in Two Dimensions
hep-ph/9212313;hep-ph;0;25;;S.Hashimoto,T.Inagaki,T.Muta;Dynamical CP Violation in Composite Higgs Models
hep-th/9212155;hep-th;0;24;;A.Galperin,E.Ivanov,O.Ogievetsky;Harmonic space and quaternionic manifolds
hep-th/9212156;hep-th;1;17;hep-th/9109032;I.Ya.Aref'eva,P.B.Medvedev,A.P.Zubarev;Interaction of d=2 c=1 Discrete States from String Field Theory
gr-qc/9212015;gr-qc;1;34;hep-th/9110028;J.H.Yoon;(1+1)-Dimensional Methods for General Relativity
cond-mat/9212035;cond-mat;0;0;;I.S.Sandalov,M.Richter;On flux phase and Néel antiferromagnetism in the {\em t}-{\em J}-model}}
hep-ph/9212314;hep-ph;0;5;;M.Bander,H.R.Rubinstein;On the 545 keV Line in the Spectrum of the Crab Nebula
gr-qc/9212016;gr-qc,hep-th;0;0;;C.O.Lousto,N.Sánchez;String Instabilities in Black Hole Spacetimes
hep-ph/9212315;hep-ph;0;0;;L.Randall,M.B.Wise;Chiral Perturbation Theory for $B →D^*$ and $B →D$ Semileptonic Transition Matrix Elements at Zero Recoil
cond-mat/9212036;cond-mat;1;11;cond-mat/9205014;K.Harigaya,M.Fujita;Dimerization structures on the metallic and semiconducting fullerene tubules
hep-th/9212157;hep-th;1;28;hep-th/9204089;A.T.Filippov,A.P.Isaev,A.B.Kurdikov;Paragrassmann Extensions of the Virasoro Algebra
hep-ph/9212316;hep-ph;0;0;;H.J.Lipkin;Paradoxes in Strange Quark Contributions to Hyperon Spins
hep-ph/9212317;hep-ph;0;6;;M.Bando,N.Maekawa;A Signal for Technicolor?
hep-ph/9212318;hep-ph;1;81;hep-ph/9205230;Z.G.Berezhiani,R.N.Mohapatra,G.Senjanovic;Planck-Scale Physics and Solutions to the Strong CP Problem without Axion
funct-an/9212005;funct-an,math.OA;0;0;;R.Exel;A Fredholm Operator Approach To Morita Equivalence
hep-th/9212158;hep-th,hep-lat;4;9;hep-th/9206095,hep-th/9207086,hep-lat/9207035,hep-th/9208002;B.S.Balakrishna;Difficulties in Inducing a Gauge Theory at Large N
astro-ph/9212006;astro-ph;0;0;;J.I.Katz;Two Populations and Models of Gamma Ray Bursts
# 3261 entries
# 25808 / 54913 = 0.4700 total success rate
# | Category | Papers | ArXiv refs | Total refs | Avg. arXiv | Avg. total |  Ratio |
# |:--------:| ------:| ----------:| ----------:| ----------:| ----------:| ------:|
# |   hep-ph |    755 |       8890 |      16018 |      11.77 |      21.22 | 55.50% |
# |  nucl-th |     49 |        529 |       1031 |      10.79 |      21.04 | 51.31% |
# |  hep-lat |    322 |       2631 |       5143 |       8.17 |      15.97 | 51.16% |
# |   hep-th |   1384 |      12129 |      24909 |       8.76 |      18.00 | 48.69% |
# |    gr-qc |    101 |        722 |       1998 |       7.14 |      19.78 | 36.14% |
# | astro-ph |     59 |        281 |        929 |       4.76 |      15.75 | 30.25% |
# | cond-mat |    219 |        581 |       3378 |       2.65 |      15.42 | 17.20% |
# | alg-geom |     70 |         32 |        529 |       0.45 |       7.56 |  6.05% |
# |     math |    277 |         13 |        978 |       0.04 |       3.53 |  1.33% |
# | funct-an |     25 |          0 |          1 |       0.00 |       0.04 |  0.00% |