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import numpy as np
import os
from datetime import datetime
from scipy.interpolate import InterpolatedUnivariateSpline, UnivariateSpline, interp1d
from scipy import interpolate
from astropy.table import Table
import galsim
vc_A = 2.99792458e+18 # speed of light: A/s
vc_m = 2.99792458e+8 # speed of light: m/s
h_Plank = 6.626196e-27 # Plank constant: erg s
def magToFlux(mag):
"""
flux of a given AB magnitude
Parameters:
mag: magnitude in unit of AB
Return:
flux: flux in unit of erg/s/cm^2/Hz
"""
flux = 10**(-0.4*(mag+48.6))
return flux
def extAv(nav, seed=1212123):
"""
Generate random intrinsic extinction Av
following the distribution from Holwerda et al, 2015
"""
np.random.seed(seed)
tau = 0.4
peak, a = 0.1, 0.5
b = a*(tau-peak)
pav = lambda av: (a*av+b)*np.exp(-av/tau)
avmin, avmax = 0., 3.
avs = np.linspace(avmin, avmax, int((avmax-avmin)/0.001)+1)
norm = np.trapz(pav(avs), avs)
pav_base = pav(avs)/np.sum(pav(avs))
rav = np.random.choice(avs, nav, p=pav_base)
return rav
###########################################
def seds(sedlistn, seddir="./", unit="A"):
"""
read SEDs and save into Python dictionary
Parameters:
sedlistn: filename of the sed template list and corresponding intrinsic
extinction model, see tmag_dz.py for detailes
listdir: directory of the list
unit: wavelength unit of the input templates
Return:
SED dictionary, the output wavelength unit is 'A'
"""
seds = {}
reds = {}
sedlist = seddir + sedlistn
sedn = open(sedlist).read().splitlines()
sedtype = range(1,len(sedn)+1)
for i in range(len(sedn)):
xxx = sedn[i].split()
isedn = seddir+xxx[0]
itype = sedtype[i]
ised = np.loadtxt(isedn)
if unit=="nm": ised[:,0] *= 10.0
seds[itype] = ised
reds[itype] = int(xxx[1])
return seds, reds
def sed_assign(phz, btt, rng):
"""
assign SED template to a galaxy.
"""
sedid = list(range(1, 34))
lzid = sedid[0:13] + sedid[23:28]
hzid = sedid[13:23]
if btt == 1.0:
sedtype = rng.sample(sedid[0:5] + sedid[28:33], 1)[0]
if phz > 2.0 and sedtype in sedid[0:5]:
sedtype = rng.sample(sedid[28:33], 1)[0]
elif btt > 0.3 and btt < 1.0:
sedtype = rng.sample(sedid, 1)[0]
if phz > 2.0 and sedtype in lzid:
sedtype = rng.sample(hzid, 1)[0]
elif btt >= 0.1 and btt < 0.3:
sedtype = rng.sample(sedid[5:28], 1)[0]
if phz > 1.5 and sedtype in lzid:
sedtype = rng.sample(hzid, 1)[0]
elif btt >= 0.0 and btt < 0.1:
sedtype = rng.sample(sedid[5:23], 1)[0]
if phz > 1.5 and sedtype in lzid:
sedtype = rng.sample(hzid, 1)[0]
else:
sedtype = 0
return sedtype
###########################################
def tflux(filt, sed, redshift=0.0, av=0.0, redden=0):
"""
calculate the theoretical SED for given filter set and template
Only AB magnitude is support!!!
Parameters:
filt: 2d array
fliter transmissions: lambda(A), T
sed: 2d array
sed templateL lambda (A), flux (erg s-1 cm-2 A-1)
redshift: float
redshift of the corresponding source, default is zero
av: float
extinction value for intrincal extinction
redden: int
reddening model, see Function 'reddening' for details
return:
tflux: float
theoretical flux
sedObs: array
SED in observed frame
"""
z = redshift + 1.0
sw, sf = sed[:,0], sed[:,1]
# reddening
sf = reddening(sw, sf, av=av, model=redden)
sw, sf = sw*z, sf*(z**3)
# lyman forest correction
sf = lyman_forest(sw, sf, redshift)
sedxx = (sw.copy(), sf.copy())
sw = vc_A/sw
sf = sf*(vc_A/sw**2) # convert flux unit to erg/s/cm^s/Hz
sw, sf = sw[::-1], sf[::-1]
sfun = interp1d(sw, sf, kind='linear')
fwave, fresp = filt[:,0], filt[:,1]
fwave = vc_A/fwave
fwave, fresp = fwave[::-1], fresp[::-1]
tflux = sfun(fwave)
zpflux = 3.631*1.0e-20
tflux = np.trapz(tflux*fresp/fwave,fwave)/np.trapz(zpflux*fresp/fwave,fwave)
#tflux = np.trapz(tflux*fresp,fwave)/np.trapz(zpflux*fresp,fwave)
return tflux, sedxx
###########################################
def lyman_forest(wavelen, flux, z):
"""
Compute the Lyman forest mean absorption of an input spectrum,
according to D_A and D_B evolution from Madau (1995).
The waveeln and flux are in observed frame
"""
if z<=0:
flux0 = flux
else:
nw = 200
istep = np.linspace(0,nw-1,nw)
w1a, w2a = 1050.0*(1.0+z), 1170.0*(1.0+z)
w1b, w2b = 920.0*(1.0+z), 1015.0*(1.0+z)
wstepa = (w2a-w1a)/float(nw)
wstepb = (w2b-w1b)/float(nw)
wtempa = w1a + istep*wstepa
ptaua = np.exp(-3.6e-03*(wtempa/1216.0)**3.46)
wtempb = w1b + istep*wstepb
ptaub = np.exp(-1.7e-3*(wtempb/1026.0)**3.46\
-1.2e-3*(wtempb/972.50)**3.46\
-9.3e-4*(wtempb/950.00)**3.46)
da = (1.0/(120.0*(1.0+z)))*np.trapz(ptaua, wtempa)
db = (1.0/(95.0*(1.0+z)))*np.trapz(ptaub, wtempb)
if da>1.0: da=1.0
if db>1.0: db=1.0
if da<0.0: da=0.0
if db<0.0: db=0.0
flux0 = flux.copy()
id0 = wavelen<=1026.0*(1.0+z)
id1 = np.logical_and(wavelen<1216.0*(1.0+z),wavelen>=1026.0*(1.0+z))
flux0[id0] = db*flux[id0]
flux0[id1] = da*flux[id1]
return flux0
###########################################
def reddening(sw, sf, av=0.0, model=0):
"""
calculate the intrinsic extinction of a given template
Parameters:
sw: array
wavelength
sf: array
flux
av: float or array
model: int
Five models will be used:
1: Allen (1976) for the Milky Way
2: Seaton (1979) fit by Fitzpatrick (1986) for the Milky Way
3: Fitzpatrick (1986) for the Large Magellanic Cloud (LMC)
4: Prevot et al (1984) and Bouchet (1985) for the Small Magellanic Cloud (SMC)
5: Calzetti et al (2000) for starburst galaxies
6: Reddy et al (2015) for star forming galaxies
Return:
reddening-corrected flux or observed flux
"""
if model==0 or av==0.0:
flux=sf
elif model==1: # Allen (1976) for the Milky Way
lambda0 = np.array([1000, 1110, 1250, 1430, 1670, \
2000, 2220, 2500, 2850, 3330, \
3650, 4000, 4400, 5000, 5530, \
6700, 9000, 10000, 20000, 100000], dtype=float)
kR = np.array([4.20, 3.70, 3.30, 3.00, 2.70, \
2.80, 2.90, 2.30, 1.97, 1.69, \
1.58, 1.45, 1.32, 1.13, 1.00, \
0.74, 0.46, 0.38, 0.11, 0.00],dtype=float)
ext0 = InterpolatedUnivariateSpline(lambda0, kR, k=1)
A_lambda = av*ext0(sw)
A_lambda[A_lambda<0.0] = 0.0
flux = sf*10**(-0.4*A_lambda)
elif model==2: # Seaton (1979) fit by Fitzpatrick (1986) for the Milky Way
Rv=3.1
al0, ga, c1, c2, c3, c4 = 4.595, 1.051, -0.38, 0.74, 3.96, 0.26
ff11 = __red(1100.0,al0,ga,c1,c2,c3,c4)
ff12 = __red(1200.0,al0,ga,c1,c2,c3,c4)
slope=(ff12-ff11)/100.0
lambda0 = np.array([3650, 4000, 4400, 5000, 5530, \
6700, 9000, 10000, 20000, 100000], dtype=float)
kR = np.array([1.58, 1.45, 1.32, 1.13, 1.00, \
0.74, 0.46, 0.38, 0.11, 0.00],dtype=float)
fun = interp1d(lambda0, kR, kind='linear')
sw0 = sw[sw<1200.0]
A_lambda0 = (ff11+(sw0-1100.0)*slope)/Rv+1.0
sw1 = sw[np.logical_and(sw>=1200.0, sw<=3650.0)]
ff = __red(sw1,al0,ga,c1,c2,c3,c4)
A_lambda1 = ff/Rv+1.0
sw2 = sw[np.logical_and(sw>3650.0, sw<=100000.0)]
A_lambda2 = fun(sw2)
A_lambda3 = sw[sw>100000.0]*0.0
A_lambda = av*np.hstack([A_lambda0,A_lambda1,A_lambda2,A_lambda3])
A_lambda[A_lambda<0.0] = 0.0
flux = sf*10**(-0.4*A_lambda)
elif model==3: # Fitzpatrick (1986) for the Large Magellanic Cloud (LMC)
Rv=3.1
al0, ga, c1, c2, c3, c4 = 4.608, 0.994, -0.69, 0.89, 2.55, 0.50
ff11 = __red(1100.0,al0,ga,c1,c2,c3,c4)
ff12 = __red(1200.0,al0,ga,c1,c2,c3,c4)
slope=(ff12-ff11)/100.0
lambda0 = np.array([3330, 3650, 4000, 4400, 5000, 5530, \
6700, 9000, 10000, 20000, 100000], dtype=float)
kR = np.array([1.682, 1.58, 1.45, 1.32, 1.13, 1.00, \
0.74, 0.46, 0.38, 0.11, 0.00],dtype=float)
fun = interp1d(lambda0, kR, kind='linear')
sw0 = sw[sw<1200.0]
A_lambda0 = (ff11+(sw0-1100.0)*slope)/Rv+1.0
sw1 = sw[np.logical_and(sw>=1200.0, sw<=3330.0)]
ff = __red(sw1,al0,ga,c1,c2,c3,c4)
A_lambda1 = ff/Rv+1.0
sw2 = sw[np.logical_and(sw>3330.0, sw<=100000.0)]
A_lambda2 = fun(sw2)
A_lambda3 = sw[sw>100000.0]*0.0
A_lambda = av*np.hstack([A_lambda0,A_lambda1,A_lambda2,A_lambda3])
A_lambda[A_lambda<0.0] = 0.0
flux = sf*10**(-0.4*A_lambda)
elif model==4: # Prevot et al (1984) and Bouchet (1985) for the Small Magellanic Cloud (SMC)
Rv = 2.72
lambda0 = np.array([1275, 1330, 1385, 1435, 1490, 1545, \
1595, 1647, 1700, 1755, 1810, 1860, \
1910, 2000, 2115, 2220, 2335, 2445, \
2550, 2665, 2778, 2890, 2995, 3105, \
3704, 4255, 5291, 12500, 16500, 22000], dtype=float)
kR = np.array([13.54, 12.52, 11.51, 10.80, 9.84, 9.28, \
9.06, 8.49, 8.01, 7.71, 7.17, 6.90, 6.76, \
6.38, 5.85, 5.30, 4.53, 4.24, 3.91, 3.49, \
3.15, 3.00, 2.65, 2.29, 1.81, 1.00, 0.00, \
-2.02, -2.36, -2.47],dtype=float)
kR = kR/Rv+1.0
ext0 = InterpolatedUnivariateSpline(lambda0, kR, k=1)
A_lambda = av*ext0(sw)
A_lambda[A_lambda<0.0] = 0.0
flux = sf*10**(-0.4*A_lambda)
elif model==5: # Calzetti et al (2000) for starburst galaxies
Rv = 4.05
sw = sw*1.0e-04 #wavelength in microns
fun1 = lambda x: 2.659*(-2.156+1.509/x-0.198/x**2+0.011/x**3)+Rv
fun2 = lambda x: 2.659*(-1.857+1.040/x)+Rv
ff11, ff12 = fun1(0.11), fun1(0.12)
slope1=(ff12-ff11)/0.01
ff99, ff100 = fun2(2.19), fun2(2.2)
slope2=(ff100-ff99)/0.01
sw0 = sw[sw<0.12]
sw1 = sw[np.logical_and(sw>=0.12, sw<=0.63)]
sw2 = sw[np.logical_and(sw>0.63, sw<=2.2)]
sw3 = sw[sw>2.2]
k_lambda0 = ff11+(sw0-0.11)*slope1
k_lambda1, k_lambda2 = fun1(sw1), fun2(sw2)
k_lambda3 = ff99+(sw3-2.19)*slope2
A_lambda = av*np.hstack([k_lambda0,k_lambda1,k_lambda2,k_lambda3])/Rv
A_lambda[A_lambda<0.0] = 0.0
flux = sf*10**(-0.4*A_lambda)
elif model==6: # Reddy et al (2015) for satr forming galaxies
Rv = 2.505
sw = sw*1.0e-04
fun1 = lambda x: -5.726+4.004/x-0.525/x**2+0.029/x**3+Rv
fun2 = lambda x: -2.672-0.010/x+1.532/x**2-0.412/x**3+Rv
ff11, ff12 = fun1(0.14), fun1(0.15)
slope1=(ff12-ff11)/0.01
ff99, ff100 = fun2(2.84), fun2(2.85)
slope2=(ff100-ff99)/0.01
sw0 = sw[sw<0.15]
sw1 = sw[np.logical_and(sw>=0.15, sw<0.60)]
sw2 = sw[np.logical_and(sw>=0.60, sw<2.85)]
sw3 = sw[sw>=2.85]
k_lambda0 = ff11+(sw0-0.14)*slope1
k_lambda1, k_lambda2 = fun1(sw1), fun2(sw2)
k_lambda3 = ff99+(sw3-2.84)*slope2
A_lambda = av*np.hstack([k_lambda0,k_lambda1,k_lambda2,k_lambda3])/Rv
A_lambda[A_lambda<0.0] = 0.0
flux = sf*10**(-0.4*A_lambda)
else:
print("!!! Please select a proper reddening model")
sys.exit(0)
return flux
###########################################
def __red(alan,al0,ga,c1,c2,c3,c4):
fun1 = lambda x: c3/(((x-(al0**2/x))**2)+ga*ga)
fun2 = lambda x,cc: cc*(0.539*((x-5.9)**2)+0.0564*((x-5.9)**3))
fun = lambda x,cc: c1+c2*x+fun1(x)+fun2(x,cc)
ala = alan*1.0e-04 #wavelength in microns
p = 1.0/ala
if np.size(p)>1:
p1, p2 = p[p>=5.9], p[p<5.9]
ff = np.append(fun(p1,c4), fun(p2,0.0))
elif np.size(p)==1:
if p<5.9: c4 = 0.0
ff = fun(p, c4)
else:
return
return ff
###########################################
def sed2mag(mag_i, sedCat, filter_list, redshift=0.0, av=0.0, redden=0):
# load the filters
nfilt = len(filter_list)
aflux = np.zeros(nfilt)
nid = -1
for k in range(nfilt):
if filter_list[k].filter_type == 'i':
nid = k
bandpass = filter_list[k].bandpass_full
ktrans = np.transpose(np.array([bandpass.wave_list*10.0, bandpass.func(bandpass.wave_list)]))
aflux[k], isedObs = tflux(ktrans, sedCat, redshift=redshift, av=av, redden=redden)
# normalize to i-band
aflux = aflux / aflux[nid]
# magnitudes in all filters
amag = -2.5*np.log10(aflux) + mag_i
spec = galsim.LookupTable(x=np.array(isedObs[0]), f=np.array(isedObs[1]), interpolant='nearest')
isedObs = galsim.SED(spec, wave_type='A', flux_type='1', fast=False)
return amag, isedObs
def eObs(e1,e2,g1,g2):
"""
Calculate the sheared (observed) ellipticity using the
intrinsic ellipticity and cosmic shear components.
Parameters:
e1, e2: scalar or numpy array
g1, g2: scalar or numpy array
Return:
Sheared (observed) ellipticity components, absolute value, and orientation
in format of scalar or numpy array
** NOTE: e1, e2, g1, and g2 should have the same dimensions.
"""
if np.isscalar(e1):
e1 = np.array([e1])
e2 = np.array([e2])
g1 = np.array([g1])
g2 = np.array([g2])
else:
e1 = e1.flatten()
e2 = e2.flatten()
g1 = g1.flatten()
g2 = g2.flatten()
# calculate the sheared (observed) ellipticity using complex rule
nobj = len(e1)
e1obs, e2obs = [], []
eeobs, theta = [], []
for i in range(nobj):
e = complex(e1[i], e2[i])
g = complex(g1[i], g2[i])
e, gg = abs(e), abs(g)
if gg<=1.0:
tt = e + g
bb = 1.0 + e*g.conjugate()
eobs = tt/bb
else:
tt = 1.0 + g*e.conjugate()
bb = e.conjugate() + g.conjugate()
eobs = tt/bb
# derive the orientation
dd = 0.5*np.arctan(abs(eobs.imag/eobs.real))*180.0/np.pi
if eobs.imag>0 and eobs.real>0: dd = dd
if eobs.imag>0 and eobs.real<0: dd = 90.0 - dd
if eobs.imag<0 and eobs.real>0: dd = 0.0 - dd
if eobs.imag<0 and eobs.real<0: dd = dd - 90.0
e1obs += [eobs.real]
e2obs += [eobs.imag]
eeobs += [abs(eobs)]
theta += [dd]
e1obs,e2obs,eeobs,theta = np.array(e1obs),np.array(e2obs),np.array(eeobs),np.array(theta)
if nobj == 1: e1obs,e2obs,eeobs,theta = e1obs[0],e2obs[0],eeobs[0],theta[0]
return e1obs, e2obs, eeobs, theta
def getObservedSED(sedCat, redshift=0.0, av=0.0, redden=0):
z = redshift + 1.0
sw, sf = sedCat[:,0], sedCat[:,1]
# reddening
sf = reddening(sw, sf, av=av, model=redden)
sw, sf = sw*z, sf*(z**3)
# lyman forest correction
sf = lyman_forest(sw, sf, redshift)
isedObs = (sw.copy(), sf.copy())
return isedObs
def integrate_sed_bandpass(sed, bandpass):
wave = np.linspace(bandpass.blue_limit, bandpass.red_limit, 1000) # in nm
flux_normalized = sed(wave)*bandpass(wave)
# print('in integrate_sed_bandpass', bandpass.blue_limit, bandpass.red_limit)
int_flux = np.trapz(y=flux_normalized, x=wave) * 10. # convert to photons s-1 m-2 A-1
return int_flux
def getABMAG(interFlux, bandpass):
throughtput = Table(np.array(np.array([bandpass.wave_list*10.0, bandpass.func(bandpass.wave_list)])).T, names=(['WAVELENGTH', 'SENSITIVITY']))
sWave = bandpass.blue_limit*10.0
eWave = bandpass.red_limit*10.0
# print('in getABMAG', sWave, eWave)
ABMAG_zero = getABMagAverageVal(
ABmag=0,
norm_thr=throughtput,
sWave=sWave,
eWave=eWave)
flux_ave = interFlux / (eWave-sWave)
ABMAG_spec = -2.5 * np.log10(flux_ave/ABMAG_zero)
return ABMAG_spec
def getABMagAverageVal(ABmag=20.,norm_thr=None, sWave=6840, eWave=8250):
"""
norm_thr: astropy.table, 2 colum, 'WAVELENGTH', 'SENSITIVITY'
Return:
the integerate flux of AB magnitude in the norm_thr(the throughtput of band), photos s-1 m-2 A-1
"""
inverseLambda = norm_thr['SENSITIVITY']/norm_thr['WAVELENGTH']
norm_thr_i = interpolate.interp1d(norm_thr['WAVELENGTH'], inverseLambda)
x = np.linspace(sWave,eWave, int(eWave)-int(sWave)+1)
y = norm_thr_i(x)
AverageLamdaInverse = np.trapz(y,x)/(eWave-sWave)
norm = 54798696332.52474 * pow(10.0, -0.4 * ABmag) * AverageLamdaInverse
# print('AverageLamdaInverse = ', AverageLamdaInverse)
# print('norm = ', norm)
return norm
def getNormFactorForSpecWithABMAG(ABMag=20., spectrum=None, norm_thr=None, sWave=6840, eWave=8250):
"""
Use AB magnitude system (zero point, fv = 3631 janskys) in the normal band(norm_thr) normalize the spectrum by inpute ABMag
Parameters
----------
spectrum: astropy.table, 2 colum, 'WAVELENGTH', 'FLUX'
norm_thr: astropy.table, 2 colum, 'WAVELENGTH', 'SENSITIVITY'
sWave: the start of norm_thr
eWave: the end of norm_thr
Return:
the normalization factor flux of AB system(fix a band and magnitude ) /the flux of inpute spectrum(fix a band)
"""
spectrumi = interpolate.interp1d(spectrum['WAVELENGTH'], spectrum['FLUX'])
norm_thri = interpolate.interp1d(norm_thr['WAVELENGTH'], norm_thr['SENSITIVITY'])
x = np.linspace(sWave,eWave, int(eWave)-int(sWave)+1)
y_spec = spectrumi(x)
y_thr = norm_thri(x)
y = y_spec*y_thr
specAve = np.trapz(y,x)/(eWave-sWave)
norm = getABMagAverageVal(ABmag=ABMag, norm_thr=norm_thr, sWave=sWave, eWave=eWave)
if specAve == 0:
return 0
# print('specAve = ', specAve)
return norm / specAve
def tag_sed(h5file, model_tag, teff=5000, logg=2, feh=0):
model_tag_str = model_tag.decode("utf-8").strip()
teff_grid = np.unique(h5file["teff"][model_tag_str])
logg_grid = np.unique(h5file["logg"][model_tag_str])
feh_grid = np.unique(h5file["feh"][model_tag_str])
close_teff = teff_grid[np.argmin(np.abs(teff_grid - teff))]
close_logg = logg_grid[np.argmin(np.abs(logg_grid - logg))]
if model_tag_str == "koester" or model_tag_str == "MC":
close_feh = 99
else:
close_feh = feh_grid[np.argmin(np.abs(feh_grid - feh))]
path = model_tag_str + f"_teff_{close_teff:.1f}_logg_{close_logg:.2f}_feh_{close_feh:.1f}"
wave = np.array(h5file["wave"][model_tag_str][()]).ravel()
flux = np.array(h5file["sed"][path][()]).ravel()
return path, wave, flux
from astropy.modeling.models import Gaussian2D
from scipy import signal
def convolveGaussXorders(img=None, sigma = 1):
offset = int(np.ceil(sigma*10))
g_size = 2*offset+1
m_cen = int(g_size/2)
g_PSF_ = Gaussian2D(1, m_cen, m_cen, sigma, sigma)
yp, xp = np.mgrid[0:g_size, 0:g_size]
g_PSF = g_PSF_(xp, yp)
psf = g_PSF/g_PSF.sum()
convImg = signal.fftconvolve(img, psf, mode='full', axes=None)
return convImg, offset