期刊文献+

Note on Redshift Distortion in Fourier Space

Note on Redshift Distortion in Fourier Space
下载PDF
导出
摘要 We explore features of redshift distortion in Fourier analysis of N-body simulations. The phases of the Fourier modes of dark matter density fluctuation are generally shifted by the peculiar motion along the line of sight, the induced phase shift is stochastic and has a probability distribution function (PDF) that is symmetric about the peak at zero shift and whose exact shape depends on the wave vector, except on very large scales where phases are invariant by linear perturbation theory. Analysis of the phase shifts motivates our phenomenological models for the bispectrum in redshift space. Comparison with simulations shows that our toy models are very successful in modeling bispectrum of equilateral and isosceles trian- gles at large scales. In the second part we compare the monopole of the power spectrum and bispectrum in the radial and plane-parallel distortion to test the plane-parallel approximation. We confirm the results of Scoccimarro that difference of power spectrum is at the level of 10%, and, in the reduced bispectrum, the difference is as small as a few percent. However, on the plane perpendicular to the line of sight of kz = 0, the difference in power spectrum be- tween the radial and plane-parallel approximation can be more than - 10%, and even worse on very small scales. Such difference is prominent for bispectrum, especially for configura- tions of tilted triangles. Non-Ganssian signals under the radial distortion on small scales are systematically biased downside than are in the plane-parallel approximation, with amplitudes depending on the opening angle of the sample point to the observer. This observation gives warning to the practice of using the power spectrum and bispectrum measured on the kz = 0 plane as estimates of the real space statistics. We explore features of redshift distortion in Fourier analysis of N-body simulations. The phases of the Fourier modes of dark matter density fluctuation are generally shifted by the peculiar motion along the line of sight, the induced phase shift is stochastic and has a probability distribution function (PDF) that is symmetric about the peak at zero shift and whose exact shape depends on the wave vector, except on very large scales where phases are invariant by linear perturbation theory. Analysis of the phase shifts motivates our phenomenological models for the bispectrum in redshift space. Comparison with simulations shows that our toy models are very successful in modeling bispectrum of equilateral and isosceles trian- gles at large scales. In the second part we compare the monopole of the power spectrum and bispectrum in the radial and plane-parallel distortion to test the plane-parallel approximation. We confirm the results of Scoccimarro that difference of power spectrum is at the level of 10%, and, in the reduced bispectrum, the difference is as small as a few percent. However, on the plane perpendicular to the line of sight of kz = 0, the difference in power spectrum be- tween the radial and plane-parallel approximation can be more than - 10%, and even worse on very small scales. Such difference is prominent for bispectrum, especially for configura- tions of tilted triangles. Non-Ganssian signals under the radial distortion on small scales are systematically biased downside than are in the plane-parallel approximation, with amplitudes depending on the opening angle of the sample point to the observer. This observation gives warning to the practice of using the power spectrum and bispectrum measured on the kz = 0 plane as estimates of the real space statistics.
出处 《Chinese Journal of Astronomy and Astrophysics》 CSCD 2007年第1期51-62,共12页 中国天文和天体物理学报(英文版)
基金 Supported by the National Natural Science Foundation of China.
关键词 COSMOLOGY theory-large-scale structure of universe-methods STATISTICAL cosmology theory-large-scale structure of universe-methods statistical
  • 相关文献

参考文献36

  • 1Chiang L.,2001,MNRAS,325,405
  • 2Chiang L.,2004,MNRAS,350,1310
  • 3Chiang L.,Coles P.,2000,MNRAS,311,809
  • 4Chiang L.,Coles P.,Naselsky P.,2002,MNRAS,337,488
  • 5Cole S.,Fisher K.B.,Weinberg D.H.,1995,MNRAS,275,515
  • 6Cole S.,Fisher K.B.,Weinberg D.H.,1994,MNRAS,267,785
  • 7Davis M.,Peebles P.J.E.,1983,ApJ,267,465
  • 8Ballinger W.E.,Heavens A.F.,Taylor A.N.,1995,MNRAS,276,59
  • 9Fisher K.B.,Davis M.,Strauss M.A.et al.,1994,MNRAS,266,50
  • 10Fisher K.B.,Lahav O.,Hoffman Y.et al.,1995,MNRAS,272,885

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部