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DM halo properties for clusters #147
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Colossus doesn't appear to have velocity dispersion. (closest thing was spashback and a reference to circular velocities) |
Ideas for list
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It seems like Colossus is the closest thing for this? |
There is an issue regarding the implementation of COLOSSUS here #16. |
Probably we may need velocity dispersions (at fixed halo mass) characterized from N-body simulations. Velocity anisotropy beta(r) in halos is quite substantial and strongly radially dependent. According to N-body simulations, it seems not that complicated for DM particles: Munari+13 I suppose it is also sensitive to assembly histories (or dynamical state). Velocity anisotropy beta(r) = 1-sigma_theta(r)^2/sigma_r(r)^2 (sigma_theta=sigma_phi assumed) |
@umetic For the first simplest working version, should we consider the cluster properties as the thing we need to make sure we can achieve and work backward to halo properties? |
I think it's a good idea. We may work out the best way of characterizing cluster halos while working through. |
Thanks for the list! From the point of view of population modeling of DM halos as a whole, for a given cosmology and a mass function N(M200m,z) [+assuming an NFW profile], we should be able to specify and draw from PDFs(M, z) all relevant properties: halo concentration c200c=R200c/rs, ellipsoidal axis ratios (a/c, b/c), ... This picture ignores a lot of underlying physics (formation epochs, assembly histories), which is replaced by a set of intrinsic scatters. Regarding the angular momentum, it is related with the orbital velocity anisotropy beta(r) and also the central cusp slope of DM density (or the Einasto shape parameter). These quantities are more difficult to link with halo mass etc. If we are to model ellipsoidal halos, their orientations should be in phase with their surrounding large-scale environment (coupled with the mass accretion rate) - at least statistically. |
Come up with a minimal list of the dark matter properties that are needed to model clusters.
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