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403 lines
11 KiB
C
403 lines
11 KiB
C
#include <stdlib.h>
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#include <stdio.h>
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#include <math.h>
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#include "header.h"
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/* It is not elegant to do things in this manner, but the code was
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* written with auto-correlation functions in mind first, and so copy+edit for
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* a second HOD was the most efficient method of modifying the code for the
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* cross-correlation function.
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*
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* NB-- No blue/red galaxies for the second HOD.
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*/
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/* This file holds several useful functions for the HOD, such as the number of
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* central and satellite halos, their second moment.
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*
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* This also intializes the HOD parameters.
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*/
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/* internal routines.
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*/
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double fixfunc1_2(double m);
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double fixfunc2_2(double m);
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double func_mlow2(double m);
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double func_mhi2(double m);
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/*****************
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* DIFFERENT HOD PARAMETERIZATIONS: (1) Central galaxies
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*
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* This integer HOD.pdfc controls the parameterization of the central occupation.
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* (I realize 'pdf' is not the right acronym, but it's a holdover from old code.)
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*
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* For soft central cutoffs, the PDF is the nearest integer distribution, AKA
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* Bernoulli distribution.
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*
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* 0 = No galaxies, just halos. (always returns 1)
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* 1 = Hard cutoff at M_min. Unity above M_min. (DEFAULT)
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* 2 = Soft cutoff of the form 0.5*(1+erf((log10(m) - log10(HOD.M_min))/HOD.sigma_logM)
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* 3 = Soft cutoff of the form N_cen = exp(-HOD.M_min/m)
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* 4 = Hard cutoff, but N_cen -> 0 for M>M_min (i.e., blue galaxies)
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* MaxCen*exp(-(lgM-lgM_min)**2/2/(sigma_logM)**2)
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* NB! -> The value of N_cen(M_min) can be < 1. (It will== MaxCen)
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* 5 = Hard Cutoff, Step function, but N_cen != 1, but some number < 1.
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* 6 = Same as 4, but symmetric Gaussian around M_min (This is for mag bins.)
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* 7 = A sqaure function. N_cen=1 for M_min <= m <= M_cen_max (for mag bin data)
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* 8 = A sqaure function (like case 7) but with Gaussian cutoffs on either edge
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* instead of sharp cutoffs.
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*
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* 9 = Magnitude bin model, but the upper mass cutoff is defined by the lower
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* mass cutoff of the next-highest bin. (see function in ml_minimization.c)
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*
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* M_low is a parameter created to keep the integrals from having to go to M=0 for
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* soft central cutoffs. N_cen(mlow) = 1.0E-3;
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* If the value of sigma_logM gets above 1 or so, then M_low can be rediculously
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* small, so I have placed a lower limit on M_low of 1.0E+7 Msol/h
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*/
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double N_cen2(double m)
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{
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double x,f=1;
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switch(HOD2.pdfc) {
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case 0:
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return 1;
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case 1:
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if(m<HOD2.M_min)return(0);
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return(f*1.0);
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break;
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case 2:
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return(f*0.5*(1+erf((log10(m) - log10(HOD2.M_min))/HOD2.sigma_logM)));
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break;
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case 3:
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return(f*exp(-HOD2.M_min/m));
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break;
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case 4:
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if(m<HOD2.M_min)return(0);
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x = (log10(m) - log10(HOD2.M_min))/HOD2.sigma_logM;
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return(f*HOD2.MaxCen*exp(-x*x/2));
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case 5:
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if(m<HOD2.M_min)return(0);
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return(f*HOD2.MaxCen);
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case 6:
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x = (log10(m) - log10(HOD2.M_min))/HOD2.sigma_logM;
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return(f*HOD2.MaxCen*exp(-x*x/2));
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case 7:
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if(m>=HOD2.M_min && m<=HOD2.M_cen_max)return(f);
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return(0);
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case 8:
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if(m>=HOD2.M_min && m<=HOD2.M_cen_max)return(f);
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if(m<HOD2.M_low)return(0);
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if(m<HOD2.M_min)
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x = (log10(m) - log10(HOD2.M_min))/HOD2.sigma_logM;
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else
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x = (log10(m) - log10(HOD2.M_cen_max))/HOD2.sigma_logM;
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return(f*exp(-x*x/2));
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case 9:
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return(f*N_cen_i(m,HOD2.i_wp));
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default:
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endrun("Illegal value of HOD2.pdfc.");
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}
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return 0;
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}
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/*****************
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* DIFFERENT HOD PARAMETERIZATIONS: (1) Satellite galaxies
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*
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* This integer HOD2.pdfs controls the parameterization of the satellite occupation.
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*
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* 0 = halos only, no galaxies (always returns zero)
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* 1 = power law: N_sat = pow(m/HOD2.M1,HOD2.alpha) [cut off at M_low]
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* 2 = power law with soft cutoff: N_sat = pow((m-HOD2.M_cut)/HOD2.M1,alpha)
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* 3 = power law with exp cutoff: N_sat = pow(m/HOD2.M1,alpha)*exp(-M_cut/(m-M_min))
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* 4 = broken power law with exp cutoff (alpha changes at some high mass value)
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* 5 = broken power law (m-mcut)/m1 parameterization
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*
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* The PDF is always assumed to be Poisson for satellite galaxies.
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*/
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double N_sat2(double m)
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{
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double m1,f=1;
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switch(HOD2.pdfs) {
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case 0:
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return 0;
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case 1:
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if(m<HOD2.M_min)return(0);
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return(f*pow(m/HOD2.M1,HOD2.alpha));
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break;
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case 2:
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if(m<HOD2.M_low || m<HOD2.M_cut)return(0);
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return(f*pow((m-HOD2.M_cut)/HOD2.M1,HOD2.alpha));
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break;
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case 3:
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if(m<HOD2.M_min)return(0);
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return(f*exp(-HOD2.M_cut/(m-HOD2.M_min))*pow(m/HOD2.M1,HOD2.alpha));
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break;
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case 4:
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if(m<HOD2.M_min)return(0);
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if(m<HOD2.M_sat_break)
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return(f*exp(-HOD2.M_cut/(m-HOD2.M_min))*pow(m/HOD2.M1,HOD2.alpha));
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else
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{
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m1 = exp(log(HOD2.M_sat_break) - HOD2.alpha/HOD2.alpha1*log(HOD2.M_sat_break/HOD2.M1));
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/*
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m1 = exp(log(HOD2.M_sat_break) - 1/HOD2.alpha1*
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(HOD2.alpha*log(HOD2.M_sat_break/HOD2.M1) - HOD2.M_cut/(HOD2.M_sat_break-HOD2.M_min)));
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*/
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return(f*exp(-HOD2.M_cut/(m-HOD2.M_min))*pow(m/m1,HOD2.alpha1));
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}
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break;
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case 5:
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if(m<HOD2.M_low || m<HOD2.M_cut)return(0);
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if(m<HOD2.M_sat_break)
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return(f*pow((m-HOD2.M_cut)/HOD2.M1,HOD2.alpha));
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else
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{
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m1 = HOD2.M_sat_break*pow((HOD2.M_sat_break-HOD2.M_cut)/HOD2.M1,-HOD2.alpha/HOD2.alpha1);
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return(f*pow(m/m1,HOD2.alpha1));
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}
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break;
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default:
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endrun("Illegal value of HOD2.pdfs.");
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}
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return 0;
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}
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/* If what is needed is the total number of galaxies in a halo.
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*/
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double N_avg2(double m)
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{
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return(N_cen2(m)+N_sat2(m));
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}
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/* This is the <(N_sat-1)(N_sat)> moment, which is
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* for the number of pairs of satellite galaxies.
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* For a Poisson distribution, <N(N-1)> = N^2
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*/
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double moment_ss2(double m)
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{
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double n;
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n=N_sat2(m);
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return(n*n);
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}
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/* This is a function to set the HOD parameters until
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* I get some input code or batch file set up.
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*
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*/
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void set_HOD2_params()
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{
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int i,j=1;
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double m,error=1.0,tol=1.0E-4,prev,s1,mlo;
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if(HOD2.pdfc == 2 || HOD2.pdfc == 3 || HOD2.pdfc == 6 || HOD2.pdfc == 8 || HOD2.pdfc == 9)
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SOFT_CENTRAL_CUTOFF=1;
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/* Error trap both the galaxy density and M_min both left unspecified.
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*/
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if(HOD2.M_min<=0 && GALAXY_DENSITY2<=0 && HOD2.free[0]==0)
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endrun("ERROR: Must specify either M_min or GALAXY_DENSITY2");
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/* If the user has specified M_min and M1, calculate the galaxy density.
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*/
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if(HOD2.M_min>0 && HOD2.M1>0)
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{
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HOD2.M_low = -1;
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if(SOFT_CENTRAL_CUTOFF)
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HOD2.M_low = exp(zbrent(func_mlow2,log(HOD2.M_min*1.0E-6),log(HOD2.M_min*1.1),1.0E-5));
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else
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HOD2.M_low = HOD2.M_min;
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GALAXY_DENSITY2=qromo(func_galaxy_density2,log(HOD2.M_low),log(HOD2.M_max),midpnt);
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if(OUTPUT) {
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fprintf(stdout,"M_low= %e\n",HOD2.M_low);
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fprintf(stdout,"ng= %e\n",GALAXY_DENSITY2); }
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}
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/* If M_min<=0 then use the specified galaxy density to calculate M_min
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*/
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if(HOD2.M_min<=0)
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{
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if(HOD2.pdfc==7 && HOD2.pdfc==8)
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HOD2.M_min=pow(10.0,zbrent(fixfunc1_2,8.0,log10(HOD2.M_cen_max*0.99),1.0E-5));
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else
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HOD2.M_min=pow(10.0,zbrent(fixfunc1_2,8.0,14.8,1.0E-5));
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HOD2.M_low = -1;
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if(SOFT_CENTRAL_CUTOFF)
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HOD2.M_low = exp(zbrent(func_mlow2,log(HOD2.M_min)-5*HOD2.sigma_logM*2.3,
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log(HOD2.M_min),1.0E-5));
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else
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HOD2.M_low = HOD2.M_min;
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if(HOD2.M_low<1.0E7)HOD2.M_low=1.0E+7;
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if(OUTPUT) {
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fprintf(stdout,"M_min %e [ng= %e]\n",HOD2.M_min,GALAXY_DENSITY2);
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fprintf(stdout,"M_low= %e\n",HOD2.M_low); }
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}
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/* If M1<=0 then use the specified galaxy density to calculate M1
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*/
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if(HOD2.M1<=0)
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{
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HOD2.M_low = -1;
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if(SOFT_CENTRAL_CUTOFF)
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HOD2.M_low = exp(zbrent(func_mlow2,log(HOD2.M_min)-5*HOD2.sigma_logM*2.3,
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log(HOD2.M_min*1.1),1.0E-5));
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else
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HOD2.M_low = HOD2.M_min;
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if(HOD2.M_low<1.0E7)HOD2.M_low=1.0E+7;
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HOD2.M1=pow(10.0,zbrent(fixfunc2_2,log10(HOD2.M_low),15.8,1.0E-5));
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if(OUTPUT) {
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fprintf(stdout,"M1 %e [ng= %e]\n",HOD2.M1,GALAXY_DENSITY2);
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fprintf(stdout,"M_min = %e M_low= %e\n",HOD2.M_min,HOD2.M_low); }
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}
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HOD2.M_hi = set_high_central_mass2();
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return;
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}
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/* If soft central cutoff, then put a lower limit on mass integrals
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* that begins at the mass where N_cen=0.001.
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*/
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double func_mlow2(double m)
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{
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/* Have a check in case the passed mass is equal to M_min, but the value of
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* N_cen is < 0.001 (which might be the case for very small sigma_logM)
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*/
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if(fabs(exp(m)-HOD2.M_min)<0.001*HOD2.M_min)
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if(N_cen2(exp(m))<0.001)return(0);
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/* fprintf(stderr,"MLO %e %e %e %e %e\n",exp(m),N_cen(exp(m)),HOD2.M_min,HOD2.M_cen_max,HOD2.M_low); */
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return(N_cen2(exp(m))-0.001);
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}
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/* It is straightforward to calculate what M_low
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* should be given the other parameters on N_cen.
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*/
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double set_low_mass2()
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{
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double m;
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if(!SOFT_CENTRAL_CUTOFF)return(HOD2.M_min);
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switch(HOD2.pdfc){
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case 8:
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case 6:
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m = log10(HOD2.M_min) - sqrt(-2*HOD2.sigma_logM*HOD2.sigma_logM*log(0.001));
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m = pow(10.0,m);
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return(m);
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default:
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m = exp(zbrent(func_mlow2,log(HOD2.M_min)-5*HOD2.sigma_logM*2.3,
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log(HOD2.M_min),1.0E-5));
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return(m);
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}
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return(0);
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}
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/* If modeling magnitude bin samples, then there will be a high mass
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* scale for central galaxies as well as a low mass scale. This finds
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* the mass at which N_cen(m)=0.001, where m>M_min.
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*/
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double set_high_central_mass2()
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{
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double m,n;
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if(HOD2.pdfc==7)
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return(HOD2.M_cen_max);
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if(!(HOD2.pdfc==6 || HOD2.pdfc==8 || HOD2.pdfc==9))
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return(HOD2.M_max);
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m = HOD2.M_min;
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n = N_cen(m);
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while(n>0.001)
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{
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m*=2;
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n = N_cen(m);
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if(m>HOD2.M_max)return(HOD2.M_max);
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}
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m = exp(zbrent(func_mhi2,log(m/2),log(m),1.0E-5));
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return(m);
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}
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double func_mhi2(double m)
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{
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m=exp(m);
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return(N_cen2(m)-0.001);
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}
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/* This is a copy of the above function that can be called from any routine.
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* (But this one integrates over dlogm
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*/
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double func_galaxy_density2(double m)
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{
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double n1,n2,m0;
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m=exp(m);
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n1=dndM_interp(m);
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n2=N_avg2(m);
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return(n1*n2*m);
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}
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/* This is the equation for zbrent to solve. What value
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* of M_min gives the correct galaxy density?
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* For HODs that have sharp central cutoffs, use M_min as the lower
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* limit of the integration. For soft cutoffs, first find M_low.
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*/
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double fixfunc1_2(double m)
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{
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double n,mlo;
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HOD2.M_min=m=pow(10.0,m);
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HOD2.M_low=0;
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if(SOFT_CENTRAL_CUTOFF)
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mlo = (zbrent(func_mlow2,log(HOD2.M_min)-5*HOD2.sigma_logM*2.3,log(HOD2.M_min),1.0E-5));
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else
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mlo = log(HOD2.M_min);
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if(exp(mlo)<1.0E7)mlo=log(1.0E+7);
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n=qromo(func_galaxy_density,mlo,log(HOD2.M_max),midpnt);
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/* fprintf(stderr,"MMIN %e %e %e %e\n",m,exp(mlo),n,GALAXY_DENSITY2); */
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return(GALAXY_DENSITY2-n);
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}
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/* This function is sent to zbrent to determine what M1 is based
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* on the number density. Both M_min and M_low have already been specified.
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*/
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double fixfunc2_2(double m)
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{
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double n;
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HOD2.M1=m=pow(10.0,m);
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n=qromo(func_galaxy_density,log(HOD2.M_low),log(HOD2.M_max),midpnt);
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return(GALAXY_DENSITY2-n);
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}
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/* This function is to be passed to qromo to integrate the number density
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* of satellite galaxies.
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*/
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double func_satfrac2(double m)
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{
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m=exp(m);
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return(N_sat2(m)*dndM_interp(m)*m);
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}
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/* This function is to be passed to qromo to integrate the number density
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* of satellite galaxies.
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*/
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double func_satellite_density2(double m)
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{
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m=exp(m);
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return(N_sat2(m)*dndM_interp(m)*m);
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}
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/* This function is to be passed to qromo to integrate the number density
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* of satellite galaxies.
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*/
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double func_central_density2(double m)
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{
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m=exp(m);
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return(N_cen2(m)*dndM_interp(m)*m);
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}
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