Next, I thought it would be interesting to place mass thresholds on the subhalos used. This is interesting because we believe that different morphological types of galaxies live in dark matter halos of different masses, e.g. big old red dead ellipticals can be expected to have a higher characteristic dark halo mass than young star-forming spirals.
Below is a sequence of subhalo thresholding, ranging from 1e10 to 1e12. Note that the y axis on the 5e11 and 1e12 plots have been significantly expanded.
What we see is that as we go to larger subhalos, the velocity dispersion is a much less accurate tracer of host halo mass. Assuming the brightest galaxies live in the largest subhalos, this means it's unlikely that choosing the brightest few galaxies to compute the velocity dispersion will yeild a result that correlates at all tightly with the mass.
Originally we were thinking of generating light cylinders and computing the velocity dispersion among all galaxies along the line of sight, but to me, the scatter for the bright guys looks large enough that there may not be a point.
Notes to own self: Procedure for getting these plots:
1) modified tree19/apps/etc/haloproc.c to dump a separate file for every halo in the .find file of lcdm_pe simulation
2) ran isodensity subhalo finder tree16/vfind64/pos/vfind.x86_64-mpi on each halo from step 1
3) ran original tree19/apps/etc/haloproc.corei7 on the .find files from step 2
4) to get subhalo masses ran ~mswarren/tree16/apps/hmassr/hmassr.x86_64 to generate .halos files
5) code to make these plots lives in projects/velfunc/hproc/shvdvsmass




































































