Add script to fit NET vs. PWV

bolo-calc/pbdr_v2/fit_NET_v_pwv.py

@@ -0,0 +1,41 @@
+import os
+import sys
+
+import matplotlib.pyplot as plt
+import numpy as np
+import toml
+
+
+table = toml.load("outputs_july27/NET_v_pwv.toml")
+
+pwv_ref = 1.0
+
+nrow, ncol = 2, 2
+fig = plt.figure(figsize=[12 * ncol, 6 * nrow])
+iplot = 0
+
+for key in table.keys():
+    if key.endswith(".yaml"):
+        subtable = table[key]
+        iplot += 1
+        ax = fig.add_subplot(nrow, ncol, iplot)
+        ax.set_title(key)
+        for band in subtable:
+            pwv = np.array(subtable[band]["pwv"]) * 1e-3
+            net = np.array(subtable[band]["NET"])
+            pivot_pwv = subtable[band]["xdefault"] * 1e-3
+            p = np.polyfit(pwv, net, 2)
+            pivot_net = np.polyval(p, pivot_pwv)
+            plt.plot(pwv, net / pivot_net, label=f"{band} : {pivot_net:.1f}", lw=3)
+            #plt.plot(np.log(pwv), np.log((net / pivot_net) ** 2), label=f"{band} : {pivot_net:.1f}", lw=3)
+            p /= pivot_net
+            x = np.linspace(0, 6, 100)
+            plt.plot(x, np.polyval(p, x), "k--", label=f"{band} : fit = {p[2]:.6f}, {p[1]:.6f}, {p[0]:.6f}")
+            #plt.plot(np.log(x), np.log(np.polyval(p, x) ** 2), "k--", label=f"{band} : fit = {p[2]:.6f}, {p[1]:.6f}, {p[0]:.6f}")
+            print(f"{key} {band} {p[2]:.6f}, {p[1]:.6f}, {p[0]:.6f}")
+        ax.set_ylim([0, 3])
+        ax.set_xlabel("PWV [mm]")
+        ax.set_ylabel("NET factor")
+        plt.legend(loc="best")
+fig.savefig("NET_v_pwv_fit.png")
+plt.show()

jbolo/AoA/2022/ApertureFuncs

@@ -0,0 +1 @@
+../ApertureFuncs

jbolo/AoA/2022/BK_bands/BK15_150_bandpass_20180920.txt

@@ -0,0 +1,339 @@
+# BICEP2/Keck Array October 2018 Data Products
+# BICEP2/Keck Array X: Constraints on Primordial Gravitational Waves using Planck, WMAP, and New BICEP2/Keck Observations through the 2015 Season
+# http://bicepkeck.org/
+#
+# File: BK15_150_bandpass_20180920.txt
+# Date: 2018-09-20
+#
+# BK15 150 GHz band frequency spectrum
+#   Column 1 = frequency in GHz
+#   Column 2 = response to a source with uniform spectra radiance
+#   Column 3 = response to a source with Rayleigh-Jeans spectrum
+#
+# Spectra are given for a beam filling source and have been peak-normalized.
+# Negative values are at the noise level of the Fourier-transform spectroscopy
+# measurement.
+#
+# Response to a source with uniform spectral radiance (column 2) matches the
+# convention used in the Planck Reduced Instrument Model (http://pla.esac.esa.int/pla,
+# see Planck 2013 results IX). Response to a source with Rayleigh-Jeans 
+# spectrum (column 3) matches the convention used in the WMAP bandpass files 
+# available on LAMBDA (http://lambda.gsfc.nasa.gov).
+#
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