def random_gal(galreal,Nrand,Nmin=10):
""" Prefered random galaxy generator. For a given galaxy with a
given magnitude (and other properties), it calculates the redshift
sensitivity function from galaxies in a magnitude band around the
selected one (i.e., including slightly brighter and fainter
galaxies), and places Nrand new galaxies at a random redshift given
by a smoothed version of the observed sensitivity function. For
extremely bright or faint galaxies (rare) the sensitivity function
is calculated from at least Nmin (=50) galaxies (i.e. the magnitude
band is increased)."""
from astro.sampledist import RanDist
from astro.fit import InterpCubicSpline
from scipy.ndimage import gaussian_filter as gf
Ckms = 299792.458
Nmin = int(Nmin) #minimum number of galaxys for the fit
zmin = np.min(galreal.ZGAL)
zmax = np.max(galreal.ZGAL) + 0.1
DZ = 0.01 #delta z for the histogram for getting the spline in z
smooth_scale = 10. #smoothing scale for the histogram (in number
#of bins, so depends on DZ)
galreal.sort(order='MAG') #np.recarray.sort()
galrand = galreal.repeat(Nrand)
delta_mag = 0.5 # half of the magnitude bandwidth to generate the z histogram
bins = np.append(np.linspace(0,zmin,20),np.arange(zmin+DZ, zmax, DZ))
for i in xrange(len(galreal)):
if i < Nmin:
vals,bins = np.histogram(galreal.ZGAL[:Nmin], bins)
vals = gf(vals.astype(float),smooth_scale) # smooth the histogram
spl = InterpCubicSpline(0.5*(bins[:-1] + bins[1:]), vals.astype(float))
else:
delta_mag2=delta_mag
while True:
cond = (galreal.MAG > 0) & (galreal.MAG < 90)
cond = cond & (galreal.MAG<=galreal.MAG[i]+delta_mag2)&(galreal.MAG>galreal.MAG[i]-delta_mag2)
if np.sum(cond)>=Nmin:
break
else:
delta_mag2+=0.1
vals,bins = np.histogram(galreal.ZGAL[cond], bins)
vals = gf(vals.astype(float),smooth_scale) # smooth the histogram
spl = InterpCubicSpline(0.5*(bins[:-1] + bins[1:]), vals.astype(float))
rvals = np.linspace(0, zmax, 1e4)
rand_z = RanDist(rvals, spl(rvals))
zrand = rand_z.random(Nrand)
integer_random2 = np.random.randint(0,len(galreal),Nrand) #for RA,DEC
RArand = galreal.RA[integer_random2]
DECrand = galreal.DEC[integer_random2]
galrand.ZGAL[i*Nrand:(i+1)*Nrand] = zrand
galrand.RA[i*Nrand:(i+1)*Nrand] = RArand
galrand.DEC[i*Nrand:(i+1)*Nrand] = DECrand
return galrand
def random_gal(galreal,Nrand,Nmin=20):
""" Prefered random galaxy generator. For a given galaxy with a
given magnitude (and other properties), it calculates the redshift
sensitivity function from galaxies in a magnitude band around the
selected one (i.e., including slightly brighter and fainter
galaxies), and places Nrand new galaxies at a random redshift given
by a smoothed version of the observed sensitivity function. For
extremely bright or faint galaxies (rare) the sensitivity function
is calculated from at least Nmin (=50) galaxies (i.e. the magnitude
band is increased)."""
from astro.sampledist import RanDist
from astro.fit import InterpCubicSpline
from scipy.ndimage import gaussian_filter as gf
Ckms = 299792.458
Nmin = int(Nmin) #minimum number of galaxys for the fit
zmin = np.min(galreal.ZGAL)
zmax = np.max(galreal.ZGAL) + 0.1
DZ = 0.01 #delta z for the histogram for getting the spline in z
smooth_scale = 10. #smoothing scale for the histogram (in number
#of bins, so depends on DZ)
galreal.sort(order='MAG') #np.recarray.sort()
galrand = galreal.repeat(Nrand)
delta_mag = 0.5 # half of the magnitude bandwidth to generate the z histogram
bins = np.append(np.linspace(0,zmin,20),np.arange(zmin+DZ, zmax, DZ))
for i in xrange(len(galreal)):
if i < Nmin:
vals,bins = np.histogram(galreal.ZGAL[:Nmin], bins)
vals = gf(vals.astype(float),smooth_scale) # smooth the histogram
spl = InterpCubicSpline(0.5*(bins[:-1] + bins[1:]), vals.astype(float))
else:
delta_mag2=delta_mag
while True:
cond = (galreal.MAG > 0) & (galreal.MAG < 90)
cond = cond & (galreal.MAG<=galreal.MAG[i]+delta_mag2)&(galreal.MAG>galreal.MAG[i]-delta_mag2)
if np.sum(cond)>=Nmin:
break
else:
delta_mag2+=0.1
vals,bins = np.histogram(galreal.ZGAL[cond], bins)
vals = gf(vals.astype(float),smooth_scale) # smooth the histogram
spl = InterpCubicSpline(0.5*(bins[:-1] + bins[1:]), vals.astype(float))
rvals = np.linspace(0, zmax, 1e4)
rand_z = RanDist(rvals, spl(rvals))
zrand = rand_z.random(Nrand)
galrand.ZGAL[i*Nrand:(i+1)*Nrand] = zrand
return galrand
def random_abs(absreal, Nrand, wa, er, sl=3, R=20000, ion='HI'):
"""From a real absorber catalog it creates a random catalog. For
a given real absorber with (z_obs,logN_obs,b_obs) it places it at
a new z_rand, defined by where the line could have been
observed.
Input parameters:
---
absreal: numpy rec array with the absorber catalog.
Nrand: number of random lines per real one generated (integer).
wa: numpy array of wavelenght covered by the spectrum.
er: numpy array of error in the normalized flux of the spectrum for
a given wavelenght.
sl: significance level for the detection of the absorption line.
From the error we calculate the Wmin = sl * wa * er / (1+z) / R,
where z = wa/w0 - 1 (w0 is the rest frame wavelenght of the
transition) and R is the resolution of the spectrograp. We then
smooth Wmin with a boxcar (sharp edges).
For the given absorber we transform (logN_obs,b_obs) to a W_obs assuming
linear part of the curve-of-growth.
We then compute the redshifts where W_obs could have been observed
according to the given Wmin, and place Nrand new absorbers with
the same properties as the given one accordingly.
"""
from astro.sampledist import RanDist
from scipy.ndimage import gaussian_filter as gf
absreal.sort(order='LOGN') #np.recarray.sort() sorted by column density
Nrand = int(Nrand)
absrand = absreal.repeat(Nrand)
Ckms = 299792.458
if ion == 'HI':
w0 = 1215.67 # HI w0 in angstroms
z = wa / w0 - 1. # spectrum in z coordinates
er = np.where(er == 0, 1e10, er)
er = np.where(np.isnan(er), 1e10, er)
Wmin = 3 * sl * w0 * er / R #3*sl*wa*er / (1. + z) / R
Wmin = gf(Wmin.astype(float), 10) # smoothed version
for i in xrange(len(absreal)):
Wr = logN_b_to_Wr(absreal.LOGN[i], absreal.B[i], ion='HI')
zgood = (Wr > Wmin) & (z > 0)
rand_z = RanDist(z, zgood * 1.)
zrand = rand_z.random(Nrand)
absrand.ZABS[i * Nrand:(i + 1) * Nrand] = zrand
return absrand
def random_abs(absreal,Nrand,wa,er,sl=3,R=20000,ion='HI'):
"""From a real absorber catalog it creates a random catalog. For
a given real absorber with (z_obs,logN_obs,b_obs) it places it at
a new z_rand, defined by where the line could have been
observed.
Input parameters:
---
absreal: numpy rec array with the absorber catalog.
Nrand: number of random lines per real one generated (integer).
wa: numpy array of wavelenght covered by the spectrum.
er: numpy array of error in the normalized flux of the spectrum for
a given wavelenght.
sl: significance level for the detection of the absorption line.
From the error we calculate the Wmin = sl * wa * er / (1+z) / R,
where z = wa/w0 - 1 (w0 is the rest frame wavelenght of the
transition) and R is the resolution of the spectrograp. We then
smooth Wmin with a boxcar (sharp edges).
For the given absorber we transform (logN_obs,b_obs) to a W_obs assuming
linear part of the curve-of-growth.
We then compute the redshifts where W_obs could have been observed
according to the given Wmin, and place Nrand new absorbers with
the same properties as the given one accordingly.
"""
from astro.sampledist import RanDist
from scipy.ndimage import gaussian_filter as gf
absreal.sort(order='LOGN') #np.recarray.sort() sorted by column density
Nrand = int(Nrand)
absrand = absreal.repeat(Nrand)
Ckms = 299792.458
if ion=='HI':
w0 = 1215.67 # HI w0 in angstroms
z = wa/w0 - 1. # spectrum in z coordinates
er = np.where(er==0,1e10,er)
er = np.where(np.isnan(er),1e10,er)
Wmin = 3*sl*w0*er/R #3*sl*wa*er / (1. + z) / R
Wmin = gf(Wmin.astype(float),10) # smoothed version
for i in xrange(len(absreal)):
Wr = logN_b_to_Wr(absreal.LOGN[i],absreal.B[i],ion='HI')
zgood = (Wr > Wmin) & (z>0)
rand_z = RanDist(z, zgood*1.)
zrand = rand_z.random(Nrand)
absrand.ZABS[i*Nrand:(i+1)*Nrand] = zrand
return absrand
def random_abs(absreal,Nrand,wa,fl,er,sl=3.,R=20000,FWHM=10.,ion='HI'):
"""From a real absorber catalog it creates a random catalog. For
a given real absorber with (z_obs,logN_obs,b_obs) it places it at
a new z_rand, defined by where the line could have been
observed.
Input parameters:
---
absreal: numpy rec array with the absorber catalog.
Nrand: number of random lines per real one generated (integer).
wa: numpy array of wavelenght covered by the spectrum.
fl: numpy array of normalized flux.
er: numpy array of error in the normalized flux of the spectrum for
a given wavelenght.
sl: significance level for the detection of the absorption line.
R: resolution of the spectrograph, assumed constant
FWHM: Full-width at half maximum in pixels (assumed constant). This
parameter defines the smoothing scale for Wmin.
ion: Name of the ion. Function only valid for HI so far.
From the error we calculate the Wmin = sl * wa * er / (1+z) / R,
where z = wa/w0 - 1 (w0 is the rest frame wavelenght of the
transition) and R is the resolution of the spectrograp. We then
smooth Wmin with a boxcar along FWHM pixels.
For the given absorber we transform (logN_obs,b_obs) to a W_obs assuming
linear part of the curve-of-growth.
We then compute the redshifts where W_obs could have been observed
according to the given Wmin, and place Nrand new absorbers with
the same properties as the given one accordingly.
"""
from astro.sampledist import RanDist
absreal.sort(order='LOGN') #np.recarray.sort() sorted by column density
Nrand = int(Nrand)
absrand = absreal.repeat(Nrand)
Ckms = 299792.458
if ion=='HI':
z_Lya, Wmin_Lya = compute_Wmin(wa,fl,er,sl=sl,R=R,FWHM=FWHM,ion='HI')
z_Lyb, Wmin_Lyb = compute_Wmin(wa,fl,er,sl=sl,R=R,FWHM=FWHM,ion='HILyb')
for i in xrange(len(absreal)):
if absreal.ZABS[i]>np.max(z_Lya): # lines that were observed through Lyb
Wr = logN_b_to_Wr(absreal.LOGN[i],absreal.B[i],ion='HILyb')
z = z_Lyb
z = np.where(z<=z_Lya,-1.,z) #mask out region with Lya coverage
Wmin = Wmin_Lyb
else: #lines that were observed through Lya only
Wr = logN_b_to_Wr(absreal.LOGN[i],absreal.B[i],ion='HI')
z = z_Lya
Wmin = Wmin_Lya
zgood = (Wr > Wmin) & (z>0)
assert np.sum(zgood)>0, \
'There are not regions in the spectrum with Wmin<%s A. Addjust significance.' %(Wr)
rand_z = RanDist(z, zgood*1.)
zrand = rand_z.random(Nrand)
absrand.ZABS[i*Nrand:(i+1)*Nrand] = zrand
return absrand
def random_abs(zobs,
Wobs,
Nrand,
wa,
fl,
er,
sl=3.,
R=20000,
FWHM=10.,
wa0=1215.67,
zmax=None,
zmin=None):
"""From a list of observed redshifts (zobs) and observed rest-frame
equivalent widths (Wobs), it creates a random catalog. For a given
real absorber with Wobs it creates Nrand random ones at the new
zrand, defined by where the line could have been observed. It
returns those zrand.
Inputs
------
zobs: observed redshifts.
Wobs: observed rest-frame equivalent widths (in A).
Nrand: number of randWr = logN_b_to_Wr()om lines per real one generated (integer).
wa: numpy array of wavelenght covered by the spectrum.
fl: numpy array of normalized flux.
er: numpy array of error in the normalized flux of the spectrum for
a given wavelenght.
sl: significance level for the detection of the absorption line.
R: resolution of the spectrograph, assumed constant
FWHM: Full-width at half maximum in pixels (assumed constant). This
parameter defines the smoothing scale for Wmin.
wa0: rest-frame wavelenght (in A).
zmax: if given, is the maximum redshift allowed for the randoms
zmin: if given, is the minimum redshift allowed for the randoms
We first compute Wmin (see abslines.Wmin). We compute the redshifts
where Wobs could have been observed according to the given Wmin,
and place Nrand new absorbers with the same properties as the given
one accordingly.
"""
zobs = np.array(zobs)
Wobs = np.array(Wobs)
wa = np.array(wa)
fl = np.array(fl)
er = np.array(er)
assert len(zobs)==len(Wobs), \
'zobs and Wobs do not have same dimensions!'
assert (len(wa)==len(fl)) and (len(wa)==len(er)),\
'wa,fl and er do not have same dimensions!'
Nrand = int(Nrand)
zrand = zobs.repeat(Nrand)
z, Wmin = compute_Wmin(wa, fl, er, sl=sl, R=R, FWHM=FWHM, wa0=wa0)
if zmax is None:
zmax = 1000. ## Here, sort out zlims
if zmin is None:
zmin = 0.
for i in xrange(len(Wobs)):
zgood = (Wobs[i] > Wmin) & (z >= zmin) & (z < zmax)
if np.sum(zgood) == 0: #This is not good so plot situation.
pl.plot(z, Wmin, drawstyle='steps-mid')
pl.axis([z[0], z[-1], 0, 0.1])
pl.show()
print Wmin
assert np.sum(zgood)>0, \
'There are not regions in the spectrum with Wmin<{} A. The minimum is {} A. Adjust significance.'.format(Wobs,np.min(Wmin))
rand_z = RanDist(z, zgood * 1.)
aux = rand_z.random(Nrand)
zrand[i * Nrand:(i + 1) * Nrand] = aux
return zrand
def random_abs(zobs,Wobs,Nrand,wa,fl,er,sl=3.,R=20000,FWHM=10.,wa0=1215.67,zmax=None,zmin=None):
"""From a list of observed redshifts (zobs) and observed rest-frame
equivalent widths (Wobs), it creates a random catalog. For a given
real absorber with Wobs it creates Nrand random ones at the new
zrand, defined by where the line could have been observed. It
returns those zrand.
Inputs
------
zobs: observed redshifts.
Wobs: observed rest-frame equivalent widths (in A).
Nrand: number of randWr = logN_b_to_Wr()om lines per real one generated (integer).
wa: numpy array of wavelenght covered by the spectrum.
fl: numpy array of normalized flux.
er: numpy array of error in the normalized flux of the spectrum for
a given wavelenght.
sl: significance level for the detection of the absorption line.
R: resolution of the spectrograph, assumed constant
FWHM: Full-width at half maximum in pixels (assumed constant). This
parameter defines the smoothing scale for Wmin.
wa0: rest-frame wavelenght (in A).
zmax: if given, is the maximum redshift allowed for the randoms
zmin: if given, is the minimum redshift allowed for the randoms
We first compute Wmin (see abslines.Wmin). We compute the redshifts
where Wobs could have been observed according to the given Wmin,
and place Nrand new absorbers with the same properties as the given
one accordingly.
"""
zobs = np.array(zobs)
Wobs = np.array(Wobs)
wa = np.array(wa)
fl = np.array(fl)
er = np.array(er)
assert len(zobs)==len(Wobs), \
'zobs and Wobs do not have same dimensions!'
assert (len(wa)==len(fl)) and (len(wa)==len(er)),\
'wa,fl and er do not have same dimensions!'
Nrand = int(Nrand)
zrand = zobs.repeat(Nrand)
z, Wmin = compute_Wmin(wa,fl,er,sl=sl,R=R,FWHM=FWHM,wa0=wa0)
if zmax is None:
zmax = 1000. ## Here, sort out zlims
if zmin is None:
zmin = 0.
for i in xrange(len(Wobs)):
zgood = (Wobs[i] > Wmin) & (z >= zmin) & ( z < zmax)
if np.sum(zgood)==0: #This is not good so plot situation.
pl.plot(z,Wmin,drawstyle='steps-mid')
pl.axis([z[0],z[-1],0,0.1])
pl.show()
print Wmin
assert np.sum(zgood)>0, \
'There are not regions in the spectrum with Wmin<{} A. The minimum is {} A. Adjust significance.'.format(Wobs,np.min(Wmin))
rand_z = RanDist(z, zgood*1.)
aux = rand_z.random(Nrand)
zrand[i*Nrand:(i+1)*Nrand] = aux
return zrand