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compute_log_derivative.py
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compute_log_derivative.py
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from classy import Class
import numpy as np
import matplotlib.pyplot as plt
from matplotlib import cm
from classy import CosmoComputationError
from time import time
from matplotlib.backends.backend_pdf import PdfPages
from sys import exit
import matplotlib
from matplotlib import rc
from scipy.interpolate import interp1d
import math
rc('font',**{'family':'serif','serif':['Times']})
rc('text', usetex=True)
# matplotlib.rc('font', **font)
matplotlib.mathtext.rcParams['legend.fontsize']='medium'
plt.rcParams["figure.figsize"] = [8.0,6.0]
start = time()
'''
This is likely the only section you will need to modify
All parameters defined here
'''
# Functionality for reading in .ini file isn't built in yet.
# Will build that if needed.
# Parameters we won't be changing
params = {'scf_potential' : 'axion',
'output':'tCl,lCl',
'compute damping scale':'yes',
'scf_parameters' : '3,0',
'log10_fraction_axion_ac' : -1,
'log10_axion_ac' : -3.5,
'scf_tuning_index':0,
'lensing':'yes',
'scf_evolve_like_axionCAMB':'no',
'do_shooting':'yes',
'do_shooting_scf':'yes',
'use_big_theta_scf':'yes',
'scf_has_perturbations':'yes',
'attractor_ic_scf':'no',
'adptative_stepsize':100,
'scf_evolve_as_fluid':'no'}
# 'input_verbose':1,
# 'background_verbose':1,
# 'thermodynamics_verbose':1,
# 'perturbations_verbose':1,
# 'transfer_verbose':1,
# 'primordial_verbose':1,
# 'spectra_verbose':1,
# 'nonlinear_verbose':1,
# 'lensing_verbose':1,
# 'output_verbose':1}
n = 3
wn = (n-1.)/(n+1.)
params['n_axion'] = n
# params['cs2_is_w'] = 'yes'
params['omega_b'] = 0.022383
params['omega_cdm'] = 0.12011
params['tau_reio'] = 0.0543
params['ln10^{10}A_s'] = 3.0448
params['n_s'] = 0.96605
H0_or_theta_s = 'theta_s'
v1_or_v2 = 'v2'
if H0_or_theta_s == 'theta_s':
theta_s = 0.01040909
params['100*theta_s'] = 100*theta_s
# param_list=['HP','rs_rec','rs_rec_over_rd_rec','da_rec','H0']
param_list=['HP','rs_rec','rs_rec_over_rd_rec','da_rec','H0']
# param_legend = ['Peak Height',r'$r_s$',r'$r_s/r_d$',r'$d_a$',r'$H_0$']
param_legend = ['Peak Height',r'$r_s$',r'$r_s/r_d$',r'$d_a$',r'$H_0$']
filename = "log_derivative_n1_vThetas_fiducial5percent.txt"
filename2 = "log_derivative_n1_vThetas_fiducial5percent_alaTristan.txt"
elif H0_or_theta_s == 'H0':
params['H0'] = 67
param_list=['HP','rs_rec','rs_rec_over_rd_rec','da_rec','theta_s']
param_legend = ['Peak Height',r'$r_s$',r'$r_s/r_d$',r'$d_a$',r'$100~\theta_s$']
filename = "log_derivative_n1_vH0_fiducial5percent.txt"
filename2 = "log_derivative_n1_vH0_fiducial5percent_alaTristan.txt"
# params['h'] = 0.67
# params['back_integration_stepsize'] = 5e-4
# params['reio_parametrization'] = 'reio_none'
N = 10 # Number of ac values
color_list = ['blue','red','green','purple','orange']
# params = ['omega_cdm','Om_ac','N_ur']
ac_values = np.logspace(-5, -3.1, N, endpoint = True)
der_param = np.zeros((N,len(param_list)))
Omega_ac_fid = np.zeros((N))
percentage_difference = 0.05
fraction_fiducial = 0.05
write_file = False
load_from_file = False
###############################################################################################################################################
# DEFINE FUNCTION TO CALCULATE THINGS
###############################################################################################################################################
def calculate_derivative_param(params,param_to_test,param_fiducial,percentage_difference,param_list,der_param,write_file,i):
cosmo = Class() # Create an instance of the CLASS wrapper
param = np.zeros((N,3,len(param_list)))
for j in range(3):
# going over a_c and Om_fld values
# if j==0:
# params['Omega_fld_ac'] = Omega_ac_fid[i]
# if j==1:
# params['Omega_fld_ac'] = Omega_ac_fid[i]+percentage_difference*Omega_ac_fid[i]
# if j==2:
# params['Omega_fld_ac'] = Omega_ac_fid[i]-percentage_difference*Omega_ac_fid[i]
if param_to_test == 'scf_parameters':
if j==0:
params['scf_parameters'] = '%.5f,0.0'%(param_fiducial)
if j==1:
params['scf_parameters'] = '%.5f,0.0'%(param_fiducial+percentage_difference*param_fiducial)
if j==2:
params['scf_parameters'] = '%.5f,0.0'%(param_fiducial-percentage_difference*param_fiducial)
else:
if j==0:
params[param_to_test] = param_fiducial
if j==1:
params[param_to_test] = param_fiducial+percentage_difference*param_fiducial
if j==2:
params[param_to_test] = param_fiducial-percentage_difference*param_fiducial
# if j==0:
# params['Omega_many_fld'] = Omega0_fld
# if j==1:
# params['Omega_many_fld'] = Omega0_fld+percentage_difference*Omega0_fld
# if j==2:
# params['Omega_many_fld'] = Omega0_fld-percentage_difference*Omega0_fld
print params[param_to_test], param_fiducial
# try to solve with a certain cosmology, no worries if it cannot
# l_theta_s = np.pi/(theta_s)
# print "here:",l_theta_s
# try:
cosmo.set(params) # Set the parameters to the cosmological code
cosmo.compute() # solve physics
cl = cosmo.lensed_cl(2500)
ell = cl['ell'][2:]
tt = cl['tt'][2:]
fTT = interp1d(ell,tt*ell*(ell+1))
for k in range(len(param_list)):
print 'k', k, len(param_list)
#calculate height peak difference
if(param_list[k] == 'HP'):
# param[i][j][k] = max(tt)-fTT(10)
param[i][j][k] = max(tt*ell*(ell+1))
elif(param_list[k] == 'rs_rec'):
param[i][j][k] = cosmo.rs_rec()
elif(param_list[k] == 'rd_rec'):
param[i][j][k] = cosmo.rd_rec()
elif(param_list[k] == 'rs_rec_over_rd_rec'):
# print cosmo.rs_rec()/cosmo.rd_rec()
param[i][j][k] = cosmo.rs_rec()/cosmo.rd_rec()
elif(param_list[k] == 'da_rec'):
param[i][j][k] = cosmo.da_rec()
elif(param_list[k] == 'theta_s'):
param[i][j][k] = cosmo.theta_s()
elif(param_list[k] == 'H0'):
param[i][j][k] = cosmo.Hubble(0)
print max(tt*ell*(ell+1)), cosmo.theta_s(), cosmo.da_rec(), cosmo.rs_rec(), cosmo.z_rec()
# for l in range(len(tt)):
# # print l, tt[l], max(tt*ell*(ell+1))
# if tt[l]*ell[l]*(ell[l]+1) == max(tt*ell*(ell+1)):
# print "l:", l,max(tt*ell*(ell+1))
# except CosmoComputationError: # this happens when CLASS fails
# print CosmoComputationError
# pass # eh, don't do anything
#calculate derivative
# der_HP[i]= (HP[i][1]-HP[i][2])/(Omega_ac_fid[i]+percentage_difference*Omega_ac_fid[i]-(Omega_ac_fid[i]-percentage_difference*Omega_ac_fid[i]))*Omega_ac_fid[0]/HP[i][0]
cosmo.empty()
cosmo.struct_cleanup()
if write_file == True:
f.write(str(ac_values[i])+'\t\t')
print "calculating derivative"
for k in range(len(param_list)):
# der_HP[i]= (HP[i][1]-HP[i][2])/(fraction_fiducial+percentage_difference*fraction_fiducial-(fraction_fiducial-percentage_difference*fraction_fiducial))*fraction_fiducial/HP[i][0]
der_param[i][k] = (param[i][1][k]-param[i][2][k])/(param_fiducial+percentage_difference*param_fiducial-(param_fiducial-percentage_difference*param_fiducial))*param_fiducial/param[i][0][k]
if write_file == True:
f.write(str(der_param[i][k])+'\t\t') # info on format
print param_list[k],der_param[i][k]
if write_file == True:
f.write('\n')
return
# der_rs_drag[i] =
# der_HP[i]= (HP[i][1]-HP[i][2])/(Omega0_fld+percentage_difference*Omega0_fld-(Omega0_fld-percentage_difference*Omega0_fld))*Omega0_fld/HP[i][0]
########### v1: CALCULATE LOG DERIVATIVE WRT f(a_c) AS A FUNCTION OF a_c ###########
if v1_or_v2=='v1':
param_to_test = 'log10_fraction_axion_ac'
param_fiducial = math.log10(fraction_fiducial)
# param_to_test = 'scf_parameters'
# param_fiducial = 2.5
if load_from_file == False:
if write_file == True:
f = open(filename, 'w') # creates a new file to write in / overwrites
f.write('# a_c, HP,rs_rec,rs_rec_over_rd_rec,da_rec,theta_s\n') # info on format
for i in range(N):
params['log10_axion_ac'] = math.log10(ac_values[i])
print "a_c = ",ac_values[i]
calculate_derivative_param(params,param_to_test,param_fiducial,percentage_difference,param_list,der_param,write_file,i)
if write_file == True:
f.close()
elif load_from_file == True:
file = np.loadtxt(filename, comments='#')
if write_file == True:
f2 = open(filename2, 'w') # creates a new file to write in / overwrites
###############################################################################################################################################
# PLOT THINGS
###############################################################################################################################################
end = time()
print('\n\nTime taken for everything but plot = %.2f seconds' %(end - start))
fig, ax = plt.subplots() # new plot
ax.tick_params(axis='x',labelsize=23)
ax.tick_params(axis='y',labelsize=23)
if write_file == True:
f2.write('# a_c, HP,rs_rec,rs_rec_over_rd_rec,da_rec,theta_s\n') # info on format
for i in range(len(file[:,0])):
f2.write(str(file[i,0])+'\t\t')
for k in range(len(param_list)):
f2.write(str(file[i,k+1]/fraction_fiducial)+'\t\t')
f2.write('\n')
for k in range(len(param_list)):
if load_from_file == True:
ax.plot(file[:,0],file[:,k+1],label=param_legend[k],color=color_list[k])
ax.set_xlim((file[:,0].min(), file[:,0].max()))
# ax.set_
# ax.set_ylim((file[:,k+1].min(),der_param.max()))
else:
ax.plot(ac_values,der_param[:,k],label=param_legend[k],color=color_list[k])
ax.set_xlim((ac_values.min(), ac_values.max()))
# ax.set_ylim((der_param.min(),der_param.max()))
ax.set_ylim((-0.1,0.05))
if H0_or_theta_s == 'H0':
ax.set_title(r'$n = $ %d, $H_0 = 67$' %params['n_axion'], fontsize = 22)
elif H0_or_theta_s == 'theta_s':
ax.set_title(r'$n = $ %d, $100~\theta_s = 1.040909$' %params['n_axion'], fontsize = 22)
if load_from_file == True and write_file == True:
f2.close()
ax.set_xlabel(r'$a_c$', fontsize = 23)
ax.set_ylabel(r'dln Param/dln$f_{\rm EDE}(a_c)$', fontsize = 23)
# ax.set_ylabel(r'dlog(X)/dlog(Y)', fontsize = 23)
#
# # ax.set_xscale("log")
# # ax.set_yscale("log")
plt.xscale('log')
# plt.yscale('log')
ax.legend(frameon=False,prop={'size':15},loc='best',borderaxespad=0.)
# for k in range(len(param_list)):
# ax.plot((10**-4)*(1+np.zeros((N,len(param_list)))),der_param[:,k],color=color_list[k],label=param_legend[k])
# plt.savefig(output_file + '.png',bbox_inches='tight')
plt.show()
########## v2: CALCULATE LOG DERIVATIVE WRT DIFFERENT COSMOLOGICAL PARAMETERS ##########
elif v1_or_v2 == 'v2':
params_new = {'output':'tCl,pCl,lCl,mPk',
'lensing':'yes',
'compute damping scale':'yes'}
params_new['omega_b'] = 0.022383
params_new['omega_cdm'] = 0.12011
params_new['tau_reio'] = 0.0543
params_new['ln10^{10}A_s'] = 3.0448
params_new['n_s'] = 0.96605
if H0_or_theta_s == 'H0':
params_new['H0'] = 67
# param_to_test = ['N_ur','omega_cdm','H0','fraction_axion_ac']
param_to_test = ['N_ur','omega_cdm','H0','scf_parameters']
param_fiducial = [3.046,0.12,67,2.5]
param_list=['HP','rs_rec','rs_rec_over_rd_rec','da_rec','theta_s']
labels = ['blank','Peak Height',r'$r_s$',r'$r_d/r_d$',r'$d_a$',r'$100~\theta_s$']
# param_legend = [r'$N_{\rm eff}$',r'$\omega_{\rm cdm}$',r'$H_0$',r'$f_{\rm EDE}(a_c)$']
param_legend = [r'$N_{\rm eff}$',r'$\omega_{\rm cdm}$',r'$H_0$',r'$\theta_i$']
if H0_or_theta_s == 'theta_s':
params_new['100*theta_s'] = 1.040909
# param_to_test = ['N_ur','omega_cdm','100*theta_s','fraction_axion_ac']
# param_to_test = ['N_ur','omega_cdm','100*theta_s','scf_parameters']
param_to_test = ['omega_cdm','scf_parameters']
# param_fiducial = [3.046,0.12,1.040909,2.5]
param_fiducial = [0.12,2.5]
param_list=['HP','rs_rec','rs_rec_over_rd_rec','da_rec','H0']
labels = ['blank','Peak Height',r'$r_s$',r'$r_s/r_d$',r'$d_a$',r'$H_0$']
# param_legend = [r'$N_{\rm eff}$',r'$\omega_{\rm cdm}$',r'$100~\theta_s$',r'$f_{\rm EDE}(a_c)$']
param_legend = [r'$\omega_{\rm cdm}$',r'$\theta_i$']
fig, ax = plt.subplots() # new plot
ax.tick_params(axis='x',labelsize=23)
ax.tick_params(axis='y',labelsize=23)
list = [0,1,2,3,4]
for i in range(len(param_to_test)):
print "i", i,len(param_to_test)
print "param = ",param_to_test[i]
if param_to_test[i] == 'scf_parameters':
params_new = {'scf_potential' : 'axion',
'output':'tCl,lCl',
'compute damping scale':'yes',
'n_axion':n,
# 'scf_parameters' : '0.1,0',
'log10_fraction_axion_ac' : -1,
'log10_axion_ac' : -3.5,
'scf_tuning_index':0,
'lensing':'yes',
'scf_evolve_like_axionCAMB':'no',
'do_shooting':'yes',
'do_shooting_scf':'yes',
'use_big_theta_scf':'yes',
'scf_has_perturbations':'yes',
'attractor_ic_scf':'no',
'adptative_stepsize':100,
'scf_evolve_as_fluid':'no'}
params_new['omega_b'] = 0.022383
params_new['omega_cdm'] = 0.12011
params_new['tau_reio'] = 0.0543
params_new['ln10^{10}A_s'] = 3.0448
params_new['n_s'] = 0.96605
calculate_derivative_param(params_new,param_to_test[i],param_fiducial[i],percentage_difference,param_list,der_param,False,i)
ax.plot(list,der_param[i,:],color=color_list[i],label=param_legend[i])
end = time()
print('\n\nTime taken for everything = %.2f seconds' %(end - start))
ax.set_xlabel(r'cosmological parameter', fontsize = 23)
ax.set_xticklabels(labels)
# ax.set_ylabel(r'dln Param/dln$f_{\rm EDE}(a_c)$', fontsize = 23)
# ax.set_ylabel(r'dlog(X)/dlog$(f_{\rm EDE}(a_c))$', fontsize = 23)
ax.set_ylabel(r'dlog(X)/dlog(Y)', fontsize = 23)
# # ax.set_xscale("log")
# # ax.set_yscale("log")
# plt.xscale('log')
# plt.yscale('log')
ax.legend(frameon=False,prop={'size':20},loc='best',borderaxespad=0.)
# for k in range(len(param_list)):
# ax.plot((10**-4)*(1+np.zeros((N,len(param_list)))),der_param[:,k],color=color_list[k],label=param_legend[k])
# plt.savefig(output_file + '.png',bbox_inches='tight')
plt.show()