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Fast Methods for Cosmological Simulations
FastSim serves as a tool for quick N-body simulations in modified gravity.
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Classes | |
| class | Power_Spectra |
Variables | |
| cosmo = csmm.FlatLambdaCDM(70.,0.3,Tcmb0=2.725) | |
| cosmo_h = cosmo.clone(H0=100) | |
| c = c.to(u.km/u.second) | |
| cosmo_fid | |
| dictionary | pk_params = {'non_linear':1,'kmax':30,'kmin':1.e-4,'nk':5000} |
| PS = Power_Spectra() | |
| l | |
| cl2 | |
| n_zl | |
| log_zl | |
| True | |
| zl_min | |
| zl_max | |
| pk_func | |
| fontsize | |
| fmt | |
| cl_cmbl_bm.c = c.to(u.km/u.second) |
Definition at line 12 of file cl_cmbl_bm.py.
Referenced by nlohmann::detail::serializer< BasicJsonType >.dump_float(), nlohmann::detail::lexer< BasicJsonType >.get_token_string(), tkEH_0(), u_nfw_c(), and window_function().
| cl_cmbl_bm.cl2 |
Definition at line 103 of file cl_cmbl_bm.py.
| cl_cmbl_bm.cosmo = csmm.FlatLambdaCDM(70.,0.3,Tcmb0=2.725) |
Definition at line 10 of file cl_cmbl_bm.py.
Referenced by a_of_chi(), ccl_angular_cl_native(), ccl_cosmology_create(), ccl_cosmology_create_flat_lcdm(), ccl_sigmaR(), ccl_sigmaV(), chi_integrand(), compare_bbks(), compare_bcm(), compare_cls(), compare_corr(), compare_correlation_3d(), compare_distances(), compare_distances_hiz(), compare_distances_hiz_mnu(), compare_distances_mnu(), compare_eh(), compare_emu(), compare_emu_nu(), compare_growth(), compare_growth_hiz(), compare_halomod(), compare_massfunc(), compare_sigmam(), compute_chi(), dfzero(), fzero(), growth_change(), growth_ode_system(), growth_rate(), main(), one_halo_integral(), two_halo_integral(), window_lensing(), window_magnification(), and write_Pk_CLASS().
| cl_cmbl_bm.cosmo_fid |
Definition at line 14 of file cl_cmbl_bm.py.
| cl_cmbl_bm.cosmo_h = cosmo.clone(H0=100) |
Definition at line 11 of file cl_cmbl_bm.py.
| cl_cmbl_bm.fmt |
Definition at line 112 of file cl_cmbl_bm.py.
Referenced by Catch::StringMaker< T[SZ]>.convert().
| cl_cmbl_bm.fontsize |
Definition at line 108 of file cl_cmbl_bm.py.
| cl_cmbl_bm.l |
Definition at line 103 of file cl_cmbl_bm.py.
Referenced by __ctest_spherical_bessel_tests_compare_gsl_run(), ccl_tracer_corr_legendre(), compare_cls(), compute_spectra(), compute_w_theta(), anonymous_namespace{chameleon.cpp}::ChiSolver< T >.correct_sol(), emuInit(), anonymous_namespace{main.cpp}.init_and_run_app(), MultiGridSolver< NDIM, T >.l_operator(), main(), spectra(), test_angpow_precision(), tkEH_0(), transfer_rsd(), MultiGridSolver< NDIM, T >.upd_operator(), anonymous_namespace{chameleon.cpp}::ChiSolver< T >.upd_operator(), and write_cl_single().
| cl_cmbl_bm.log_zl |
Definition at line 103 of file cl_cmbl_bm.py.
| cl_cmbl_bm.n_zl |
Definition at line 103 of file cl_cmbl_bm.py.
| cl_cmbl_bm.pk_func |
Definition at line 103 of file cl_cmbl_bm.py.
Referenced by cl_cmbl_bm.Power_Spectra.cl_z().
| dictionary cl_cmbl_bm.pk_params = {'non_linear':1,'kmax':30,'kmin':1.e-4,'nk':5000} |
Definition at line 16 of file cl_cmbl_bm.py.
| cl_cmbl_bm.PS = Power_Spectra() |
Definition at line 102 of file cl_cmbl_bm.py.
| cl_cmbl_bm.True |
Definition at line 103 of file cl_cmbl_bm.py.
| cl_cmbl_bm.zl_max |
Definition at line 103 of file cl_cmbl_bm.py.
| cl_cmbl_bm.zl_min |
Definition at line 103 of file cl_cmbl_bm.py.