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January 25, 2019 16:24
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import numpy as np | |
import sys | |
sys.path.append("../Lensing-PowerSpectra/Simulations/") | |
from units import * | |
import theano.tensor as tt | |
def deflection_sis(x, y, x0=0, y0=0, b=1.5): | |
""" Deflection for singular isothermal ellipsoid, from astro-ph/0102341 | |
""" | |
# Go into shifted coordinats of the potential | |
xsie = x - x0 | |
ysie = y - y0 | |
# Compute potential gradient | |
psi = np.sqrt(xsie**2 + ysie**2) | |
xg = b * xsie / psi # (psi + tt.switch((tt.eq(psi,0), 1, 0) )) | |
yg = b * ysie / psi # (psi + tt.switch((tt.eq(psi,0), 1, 0) )) | |
# Return value | |
return xg, yg | |
def deflection_nfw(x, y, x0=0, y0=0, M=1e14*M_s, c=20, D_s=1*Mpc, D_l=0.5*Mpc): | |
""" Deflection for an NFW halo, from astro-ph/0102341 | |
TODO: deal with origin singularity as in SIE case | |
""" | |
D_ls = D_s - D_l | |
# Coordinates in natural (not angular) units | |
xnfw = (x - x0)*D_l*asctorad | |
ynfw = (y - y0)*D_l*asctorad | |
r = np.sqrt(xnfw**2 + ynfw**2) | |
delta_c = (200/3.)*c**3/(np.log(1+c) - c/(1+c)) | |
rho_s = rho_c*delta_c | |
r_s = (M/((4/3.)*np.pi*c**3*200*rho_c))**(1/3.) # NFW scale radius | |
x = r/r_s | |
Sigma_crit = Sigma_cr(D_l, D_s) # Critical lensing density | |
kappa_s = rho_s*r_s/Sigma_crit | |
# Get spherically symmetric deflection | |
Fvec = tt.switch(tt.eq(x,1), 1, tt.switch(x > 1, F1(x), F2(x))) | |
phitg = 4*kappa_s*r_s*(np.log(x/2.) + Fvec)/x | |
# Get x and y coordinates of deflection | |
xtg = phitg*xnfw/r | |
ytg = phitg*ynfw/r | |
# Convert back to rad, then arcsecs | |
return xtg/D_l*radtoasc, ytg/D_l*radtoasc | |
def Sigma_cr(D_l, D_s): | |
return 1./(4*np.pi*GN)*D_s/((D_s - D_l)*D_l) | |
def F1(x): | |
""" Helper function for NFW deflection, from astro-ph/0102341 | |
""" | |
return np.arctan(np.sqrt(x**2-1))/(np.sqrt(x**2 - 1)) | |
def F2(x): | |
""" Helper function for NFW deflection, from astro-ph/0102341 | |
""" | |
return np.arctanh(np.sqrt(1-x**2))/(np.sqrt(1-x**2)) | |
def f_gal_sersic(x, y, n=4, I_gal=1e-16*erg/Centimeter**2/Sec/Angstrom, theta_e_gal=1): | |
""" Sersic profile surface brightness, following Daylan et al | |
""" | |
theta = np.sqrt(x**2 + y**2) | |
b_n = 2*n - 1/3. + 4/(405*n) + 46/(25515*n**2) | |
f_e_gal = I_gal/(7.2*np.pi*theta_e_gal**2) | |
return f_e_gal*np.exp(-b_n*((theta/theta_e_gal)**(1/n) - 1)) |
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