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from classy import Class |
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from math import pi |
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get_ipython().run_line_magic('matplotlib', 'inline') |
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import matplotlib |
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import matplotlib.pyplot as plt |
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common_settings = { |
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'h':0.67810, |
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'omega_b':0.02238280, |
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'omega_cdm': 0.1201075, |
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'A_s':2.100549e-09, |
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'tau_reio': 0.05430842} |
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l_max_scalars = 3000 |
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l_max_tensors = 600 |
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M = Class() |
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M.set(common_settings) |
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M.set({'output':'tCl,pCl','modes':'s','lensing':'no','n_s':0.9660499, |
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'l_max_scalars':l_max_scalars}) |
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M.compute() |
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cls = M.raw_cl(l_max_scalars) |
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M.empty() |
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M.set(common_settings) |
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M.set({'output':'tCl,pCl','modes':'t','lensing':'no','r':0.1,'n_t':0, |
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'l_max_tensors':l_max_tensors}) |
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M.compute() |
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clt = M.raw_cl(l_max_tensors) |
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M.empty() |
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M.set(common_settings) |
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M.set({'output':'tCl,pCl,lCl','modes':'s,t','lensing':'yes','n_s':0.9660499,'r':0.1,'n_t':0, |
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'l_max_scalars':l_max_scalars,'l_max_tensors':l_max_tensors}) |
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M.compute() |
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cl_tot = M.raw_cl(l_max_scalars) |
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cl_lensed = M.lensed_cl(l_max_scalars) |
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plt.xlim([2,l_max_scalars]) |
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plt.ylim([1.e-8,10]) |
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plt.xlabel(r"$\ell$") |
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plt.ylabel(r"$\ell (\ell+1) C_l^{XY} / 2 \pi \,\,\, [\times 10^{10}]$") |
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plt.title(r"$r=0.1$") |
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plt.grid() |
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ell = cl_tot['ell'] |
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ellt = clt['ell'] |
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factor = 1.e10*ell*(ell+1.)/2./pi |
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factort = 1.e10*ellt*(ellt+1.)/2./pi |
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plt.loglog(ell,factor*cls['tt'],'r-',label=r'$\mathrm{TT(s)}$') |
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plt.loglog(ellt,factort*clt['tt'],'r:',label=r'$\mathrm{TT(t)}$') |
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plt.loglog(ell,factor*cls['ee'],'b-',label=r'$\mathrm{EE(s)}$') |
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plt.loglog(ellt,factort*clt['ee'],'b:',label=r'$\mathrm{EE(t)}$') |
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plt.loglog(ellt,factort*clt['bb'],'g:',label=r'$\mathrm{BB(t)}$') |
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plt.loglog(ell,factor*(cl_lensed['bb']-cl_tot['bb']),'g-',label=r'$\mathrm{BB(lensing)}$') |
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plt.legend(loc='right',bbox_to_anchor=(1.4, 0.5)) |
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plt.savefig('cl_ST.pdf',bbox_inches='tight') |
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