Nonlinear biasing and redshift-space distortions in Lagrangian resummation theory and N-body simulations

被引:42
作者
Sato, Masanori [1 ]
Matsubara, Takahiko [1 ,2 ]
机构
[1] Nagoya Univ, Dept Phys, Nagoya, Aichi 4648602, Japan
[2] Nagoya Univ, Kobayashi Maskawa Inst Origin Particles & Univers, Nagoya, Aichi 4648602, Japan
关键词
BARYON ACOUSTIC-OSCILLATIONS; FRIEDMAN-LEMAITRE COSMOLOGIES; GALAXY POWER SPECTRUM; LARGE-SCALE STRUCTURE; PROBING DARK ENERGY; MASS FUNCTION; GRAVITATIONAL-INSTABILITY; NEWTONIAN COSMOLOGY; PERTURBATION-THEORY; ANALYTIC MODEL;
D O I
10.1103/PhysRevD.84.043501
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Understanding a behavior of galaxy biasing is crucial for future galaxy redshift surveys. One aim is to measure the baryon acoustic oscillations (BAOs) within the precision of a few percent level. Using 30 large cosmological N-body simulations for a standard Lambda CDM cosmology, we study the halo biasing over a wide redshift range. We compare the simulation results with theoretical predictions proposed by Matsubara [T. Matsubara, Phys. Rev. D 78, 083519 (2008).] which naturally incorporate the halo bias and redshift-space distortions into their formalism of perturbation theory with a resummation technique via the Lagrangian picture. The power spectrum and correlation function of halos obtained from Lagrangian resummation theory (LRT) well agree with N-body simulation results on scales of BAOs. Especially nonlinear effects on the baryon acoustic peak of the halo correlation function are accurately explained both in real and redshift space. We find that nonlinearity and scale dependence of bias are fairly well reproduced by 1-loop LRT up to k = 0.35h Mpc(-1) (z = 2 and 3) within a few percent level in real space and up to k = 0.1h Mpc(-1) (z = 2) and 0.15h Mpc(-1) (z = 3) in redshift space. Thus, the LRT is very powerful for accurately extracting cosmological information in upcoming high redshift BAO surveys.
引用
收藏
页数:15
相关论文
共 121 条
[1]  
ALBRECHT AJ, ARXIV09010721
[2]   Constraints on perfect fluid and scalar field dark energy models from future redshift surveys [J].
Amendola, L ;
Quercellini, C ;
Giallongo, E .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2005, 357 (02) :429-439
[3]   The detectability of baryonic acoustic oscillations in future galaxy surveys [J].
Angulo, R. E. ;
Baugh, C. M. ;
Frenk, C. S. ;
Lacey, C. G. .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 2008, 383 (02) :755-776
[4]  
[Anonymous], ARXIVASTROPH0609591
[5]   THE STATISTICS OF PEAKS OF GAUSSIAN RANDOM-FIELDS [J].
BARDEEN, JM ;
BOND, JR ;
KAISER, N ;
SZALAY, AS .
ASTROPHYSICAL JOURNAL, 1986, 304 (01) :15-61
[6]   Large-scale structure of the Universe and cosmological perturbation theory [J].
Bernardeau, F ;
Colombi, S ;
Gaztañaga, E ;
Scoccimarro, R .
PHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS, 2002, 367 (1-3) :1-248
[7]   MASS FUNCTION PREDICTIONS BEYOND ΛCDM [J].
Bhattacharya, Suman ;
Heitmann, Katrin ;
White, Martin ;
Lukic, Zarija ;
Wagner, Christian ;
Habib, Salman .
ASTROPHYSICAL JOURNAL, 2011, 732 (02)
[8]   Probing dark energy using baryonic oscillations in the galaxy power spectrum as a cosmological ruler [J].
Blake, C ;
Glazebrook, K .
ASTROPHYSICAL JOURNAL, 2003, 594 (02) :665-673
[9]  
BLAKE C, MON NOT R A IN PRESS
[10]   The scale dependence of relative galaxy bias: Encouragement for the "halo model'' description [J].
Blanton, Michael R. ;
Eisenstein, Daniel ;
Hogg, David W. ;
Zehavi, Idit .
ASTROPHYSICAL JOURNAL, 2006, 645 (02) :977-985