Abstract

In the hierarchical structure formation model cosmic halos are supposed to form by accretion of smaller units along anisotropic direction, defined by large-scale filamentary structures. After the epoch of primary mass aggregation (which depend on the cosmological model), violent relaxation processes will tend to alter the halo phase-space configuration producing quasi-spherical halos with a relatively smooth density profiles. Here we attempt to investigate the relation between halos shapes, their environment and their dynamical state. To this end we have run a large (L=500h−1L=500 h^{-1} Mpc, Np=5123N_{p}=512^3 particles) N-body simulation of a flat low-density cold dark matter model with a matter density Ωm=1−ΩΛ=0.3Ω_{\rm m}=1-Ω_Λ=0.3, Hubble constant H∘=70H_{\circ}=70 km s−1^{-1} Mpc−1^{-1} and a normalization parameter of σ8=0.9σ_{8}=0.9. The particle mass is mp≥7.7×1010h−1M⊙m_{\rm p}\ge 7.7\times 10^{10} h^{-1} M_{\odot} comparable to the mass of one single galaxy. The halos are defined using a friends-of-friend algorithm with a linking length given by l=0.17νˉl=0.17\barν where νˉ\barν is the mean density. This linking length corresponds to an overdensity ρ/ρmean≃200ρ/ρ_{\rm mean}\simeq 200 at the present epoch (z=0z=0) and the total number of halos with more than 130 particles (M>3×1013h−1M⊙M>3 \times 10^{13} h^{-1} M_{\odot}) is 57524.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.