The birth and growth of neutralino haloes

被引:57
作者
Angulo, R. E. [1 ]
White, S. D. M. [1 ]
机构
[1] Max Planck Inst Astrophys, D-85741 Garching, Germany
关键词
cosmology: theory; large-scale structure of Universe; DARK-MATTER HALOES; POWER SPECTRUM; MASS FUNCTIONS; ASSEMBLY BIAS; GALAXIES; UNIVERSE; MODELS; SIMULATION; EVOLUTION; HISTORY;
D O I
10.1111/j.1365-2966.2009.15742.x
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We use the extended Press-Schechter (EPS) formalism to study halo assembly histories in a standard Lambda cold dark matter cosmology. A large ensemble of Monte Carlo random walks provides the entire halo membership histories of a representative set of dark matter particles, which we assume to be neutralinos. The first-generation haloes of most particles do not have a mass similar to the free-streaming cut-off M(fs) of the neutralino power spectrum, nor do they form at high redshift. Median values are M(1) = 10(5)-10(7) M(fs) and z(1) = 13 to 8 depending on the form of the collapse barrier assumed in the EPS model. For almost one third of all particles, the first-generation halo has M(1) > 10(9) M(fs). At redshifts beyond 20, most neutralinos are not yet part of any halo but are still diffuse. These numbers apply with little modification to the neutralinos which are today part of haloes similar to that of the Milky Way. Up to 10 per cent of the particles in such haloes were never part of a smaller object; the typical particle has undergone approximately five 'accretion events' where the halo it was part of falls into a more massive object. Available N-body simulations agree well with the EPS predictions for an 'ellipsoidal' collapse barrier, so these may provide a reliable extension of simulation results to smaller scales. The late formation times and large masses of the first-generation haloes of most neutralinos suggest that they will be disrupted with high efficiency during halo assembly.
引用
收藏
页码:1796 / 1803
页数:8
相关论文
共 29 条
[1]  
Angulo RE, 2008, MON NOT R ASTRON SOC, V387, P921, DOI [10.1111/j.1365-2966.2008.13304.x, 10.1111/J.1365-2966.2008.13304.x]
[2]  
ANGULO RE, 2008, ARXIV08102177
[3]   Particle dark matter: evidence, candidates and constraints [J].
Bertone, G ;
Hooper, D ;
Silk, J .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 2005, 405 (5-6) :279-390
[4]   Effects of cold dark matter decoupling and pair annihilation on cosmological perturbations [J].
Bertschinger, Edmund .
PHYSICAL REVIEW D, 2006, 74 (06)
[5]   EXCURSION SET MASS FUNCTIONS FOR HIERARCHICAL GAUSSIAN FLUCTUATIONS [J].
BOND, JR ;
COLE, S ;
EFSTATHIOU, G ;
KAISER, N .
ASTROPHYSICAL JOURNAL, 1991, 379 (02) :440-460
[6]   THE EVOLUTION OF GROUPS OF GALAXIES IN THE PRESS-SCHECHTER FORMALISM [J].
BOWER, RG .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1991, 248 (02) :332-352
[7]   Resolving cosmic structure formation with the Millennium-II Simulation [J].
Boylan-Kolchin, Michael ;
Springel, Volker ;
White, Simon D. M. ;
Jenkins, Adrian ;
Lemson, Gerard .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2009, 398 (03) :1150-1164
[8]  
BRINGMANN T, 2009, ARXIV09030189
[9]   THE EVOLUTION OF LARGE-SCALE STRUCTURE IN A UNIVERSE DOMINATED BY COLD DARK MATTER [J].
DAVIS, M ;
EFSTATHIOU, G ;
FRENK, CS ;
WHITE, SDM .
ASTROPHYSICAL JOURNAL, 1985, 292 (02) :371-394
[10]   Earth-mass dark-matter haloes as the first structures in the early Universe [J].
Diemand, J ;
Moore, B ;
Stadel, J .
NATURE, 2005, 433 (7024) :389-391