A Universal Density Profile from Hierarchical Clustering

We use high-resolution N-body simulations to study the equilibrium density profiles of dark matter halos in hierarchically clustering universes. We find that all such profiles have the same shape, independent of the halo mass, the initial density fluctuation spectrum, and the values of the cosmological parameters. Spherically averaged equilibrium profiles are well fitted over two decades in radius by a simple formula originally proposed to describe the structure of galaxy clusters in a cold dark matter universe. In any particular cosmology, the two scale parameters of the fit, the halo mass and its characteristic density, are strongly correlated. Low-mass halos are significantly denser than more massive systems, a correlation that reflects the higher collapse redshift of small halos. The characteristic density of an equilibrium halo is proportional to the density of the universe at the time it was assembled. A suitable definition of this assembly time allows the same proportionality constant to be used for all the cosmologies that we have tested. We compare our results with previous work on halo density profiles and show that there is good agreement. We also provide a step-by-step analytic procedure, based on the Press-Schechter formalism, that allows accurate equilibrium profiles to be calculated as a function of mass in any hierarchical model.

[1]  F. Bouchet,et al.  The structure and dynamical evolution of dark matter haloes , 1996, astro-ph/9603132.

[2]  S. Tremaine,et al.  Made-to-measure N-body systems , 1996, astro-ph/9605061.

[3]  S. Cole,et al.  The structure of dark matter haloes in hierarchical clustering models , 1995, astro-ph/9510147.

[4]  S. White,et al.  The Structure of cold dark matter halos , 1995, astro-ph/9508025.

[5]  S. White,et al.  Simulations of X-ray clusters , 1994, astro-ph/9408069.

[6]  A. Evrard,et al.  The cosmological dependence of cluster density profiles , 1994, astro-ph/9404030.

[7]  S. White,et al.  Simulations of dissipative galaxy formation in hierarchically clustering universes – I: Tests of the code , 1993 .

[8]  S. Cole,et al.  Merger rates in hierarchical models of galaxy formation – II. Comparison with N-body simulations , 1994, astro-ph/9402069.

[9]  Michael S. Warren,et al.  Dark halos formed via dissipationless collapse. I: Shapes and alignment of angular momentum , 1992 .

[10]  John Dubinski,et al.  The structure of cold dark matter halos , 1991 .

[11]  L. Hernquist,et al.  An Analytical Model for Spherical Galaxies and Bulges , 1990 .

[12]  Carlos S. Frenk,et al.  Gravitational clustering from scale-free initial conditions , 1988 .

[13]  John K. Salmon,et al.  Rotation of halos in open and closed universes: differentiated merging and natural selection of galaxy types , 1988 .

[14]  Y. Hoffman On the Formation and Structure of Galactic Halos , 1988 .

[15]  G. Efstathiou,et al.  The formation of dark halos in a universe dominated by cold dark matter , 1988 .

[16]  M. West,et al.  Profiles of clusters of galaxies - Cosmological scenarios versus observations , 1987 .

[17]  W. H. Zurek,et al.  Primordial density fluctuations and the structure of galactic haloes , 1986, Nature.

[18]  G. Efstathiou,et al.  Cold dark matter, the structure of galactic haloes and the origin of the Hubble sequence , 1985, Nature.

[19]  Y. Hoffman,et al.  Local density maxima - Progenitors of structure , 1985 .

[20]  E. Bertschinger Self-similar secondary infall and accretion in an Einstein-de Sitter universe , 1985 .

[21]  G. Efstathiou,et al.  Numerical techniques for large cosmological N-body simulations , 1985 .

[22]  P. Goldreich,et al.  Self-similar gravitational collapse in an expanding universe , 1984 .

[23]  J. Gunn,et al.  On the Infall of Matter into Clusters of Galaxies and Some Effects on Their Evolution , 1972 .

[24]  D. Lynden-Bell Statistical Mechanics of Violent Relaxation in Stellar Systems , 1967 .