TY - JOUR
T1 - Virial scaling of massive dark matter halos
T2 - Why clusters prefer a high normalization cosmology
AU - Evrard, A. E.
AU - Bialek, J.
AU - Busha, M.
AU - White, M.
AU - Habib, S.
AU - Heitmann, K.
AU - Warren, M.
AU - Rasia, E.
AU - Tormen, G.
AU - Moscardini, L.
AU - Power, C.
AU - Jenkins, A. R.
AU - Gao, L.
AU - Frenk, C. S.
AU - Springel, V.
AU - White, S. D.M.
AU - Diemand, J.
PY - 2008/1/1
Y1 - 2008/1/1
N2 - We present a precise estimate of the bulk virial scaling relation of halos formed via hierarchical clustering in an ensemble of simulated cold dark matter cosmologies. The result is insensitive to cosmological parameters; the presence of a trace, dissipationless gas component; and numerical resolution down to a limit of ∼ 1000 particles. The dark matter velocity dispersion scales with total mass as log[σDM(M, z)] = log(1082.9 ± 4.0 km s_1) + (0.3361 ± 0.0026)log [h(z)M200 /10 15 M⊙], with h(z) being the dimensionless Hubble parameter. At fixed mass, the velocity dispersion likelihood is nearly lognormal, with scatter σln σ = 0.0426 ± 0.015, except for a tail with higher dispersions containing 10% of the population that are merger transients. We combine this relation with the halo mass function in ACDM models and show that a low normalization condition, S8 = σ8(Ωm/0.3)0.35 = 0.69, favored by recent WMAP and SDSS analysis requires that galaxy and gas-specific energies in rich clusters be 50% larger than that of the underlying dark matter. Such large energetic biases are in conflict with the current generation of direct simulations of cluster formation. A higher normalization, S8 = 0.80, alleviates this tension and implies that the hot gas fraction within r 500 is (0.71 ± 0.09) h70-3/2 Ωb/Ωm, a value consistent with recent Sunyaev-Zel'dovich observations.
AB - We present a precise estimate of the bulk virial scaling relation of halos formed via hierarchical clustering in an ensemble of simulated cold dark matter cosmologies. The result is insensitive to cosmological parameters; the presence of a trace, dissipationless gas component; and numerical resolution down to a limit of ∼ 1000 particles. The dark matter velocity dispersion scales with total mass as log[σDM(M, z)] = log(1082.9 ± 4.0 km s_1) + (0.3361 ± 0.0026)log [h(z)M200 /10 15 M⊙], with h(z) being the dimensionless Hubble parameter. At fixed mass, the velocity dispersion likelihood is nearly lognormal, with scatter σln σ = 0.0426 ± 0.015, except for a tail with higher dispersions containing 10% of the population that are merger transients. We combine this relation with the halo mass function in ACDM models and show that a low normalization condition, S8 = σ8(Ωm/0.3)0.35 = 0.69, favored by recent WMAP and SDSS analysis requires that galaxy and gas-specific energies in rich clusters be 50% larger than that of the underlying dark matter. Such large energetic biases are in conflict with the current generation of direct simulations of cluster formation. A higher normalization, S8 = 0.80, alleviates this tension and implies that the hot gas fraction within r 500 is (0.71 ± 0.09) h70-3/2 Ωb/Ωm, a value consistent with recent Sunyaev-Zel'dovich observations.
KW - Cosmology: miscellaneous
KW - Cosmology: theory
KW - Dark matter
KW - Galaxies: clusters: general
KW - Gravitation
KW - Intergalactic medium
UR - http://www.scopus.com/inward/record.url?scp=40249092899&partnerID=8YFLogxK
U2 - 10.1086/521616
DO - 10.1086/521616
M3 - Article
SN - 0004-637X
VL - 672
SP - 122
EP - 137
JO - The Astrophysical Journal
JF - The Astrophysical Journal
IS - 1
ER -