add more motions

process_ste.py

@@ -0,0 +1,49 @@
+from python.ste import *
+
+fig_tau_cc, ax_tau_cc = plt.subplots()
+ax_tau_cc.set_title('tau_cc')
+
+fig_beta_cc, ax_beta_cc = plt.subplots()
+ax_beta_cc.set_title('beta_cc')
+
+fig_finfty_cc, ax_finfty_cc = plt.subplots()
+ax_finfty_cc.set_title('f_infty_cc')
+
+fig_tau_ss, ax_tau_ss = plt.subplots()
+ax_tau_ss.set_title('tau_ss')
+
+fig_beta_ss, ax_beta_ss = plt.subplots()
+ax_beta_ss.set_title('beta_ss')
+
+fig_finfty_ss, ax_finfty_ss = plt.subplots()
+ax_finfty_ss.set_title('f_infty_ss')
+
+for conf_file in pathlib.Path('.').glob(f'IsotropicAngle/angle=*/Delta/tau=*/*_parameter.txt'):
+    print(conf_file)
+    vary_string, tau_cc, beta_cc, finfty_cc = fit_ste(conf_file, f'coscos', plot_decays=False, verbose=False)
+    _, tau_ss, beta_ss, finfty_ss = fit_ste(conf_file, f'sinsin', plot_decays=False, verbose=False)
+    _, tau_2, beta_2, finfty_2 = fit_ste(conf_file, f'f2', plot_decays=True, verbose=True)
+
+    ax_tau_cc.semilogy(tau_cc[:, 0], tau_cc[:, 1], label=vary_string)
+    ax_tau_cc.axhline(tau_2[:, 1], color='k', linestyle='--')
+    ax_beta_cc.plot(*beta_cc.T, label=vary_string)
+    ax_finfty_cc.plot(*finfty_cc.T, label=vary_string)
+    ax_tau_ss.semilogy(tau_ss[:, 0], tau_ss[:, 1], label=vary_string)
+    ax_tau_ss.axhline(tau_2[:, 1], color='k', linestyle='--')
+    ax_beta_ss.plot(*beta_ss.T, label=vary_string)
+    ax_finfty_ss.plot(*finfty_ss.T, label=vary_string)
+
+    np.savetxt(
+        conf_file.with_name(f'ste_fit_{vary_string}.dat'),
+        np.c_[
+            tau_cc, beta_cc[:, 1], finfty_cc[:, 1],
+            tau_ss[:, 1], beta_ss[:, 1], finfty_ss[:, 1],
+        ],
+        header=f'Fit STE {vary_string}\n'
+               f'F2: tau={tau_2[0, 1]} beta={beta_2[0, 1]} finfty={finfty_2[0, 1]}\n'
+               f'tevo\ttaucc\tbetacc\tfinftycc\ttauss\tbetass\tfinftyss',
+    )
+
+for ax in [ax_tau_cc, ax_beta_cc, ax_finfty_cc, ax_tau_ss, ax_beta_ss, ax_finfty_ss]:
+    ax.legend()
+plt.show()