Combining weak-lensing tomography and spectroscopic redshift surveys
Article first published online: 15 MAR 2012
DOI: 10.1111/j.1365-2966.2012.20676.x
© 2012 The Authors Monthly Notices of the Royal Astronomical Society © 2012 RAS
Issue

Monthly Notices of the Royal Astronomical Society
Volume 422, Issue 2, pages 1045–1056, May 2012
Additional Information
How to Cite
Cai, Y.-C. and Bernstein, G. (2012), Combining weak-lensing tomography and spectroscopic redshift surveys. Monthly Notices of the Royal Astronomical Society, 422: 1045–1056. doi: 10.1111/j.1365-2966.2012.20676.x
Publication History
- Issue published online: 25 APR 2012
- Article first published online: 15 MAR 2012
- Accepted 2012 February 1. Received 2012 January 25; in original form 2011 December 19
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Keywords:
- gravitational lensing: weak – methods: statistical – large-scale structure of Universe
ABSTRACT
Redshift space distortion (RSD) is a powerful way of measuring the growth of structure and testing General Relativity, but it is limited by cosmic variance and the degeneracy between the galaxy bias b and the growth rate factor f. The cross-correlation of lensing shear with the galaxy density field can in principle measure b in a manner free from cosmic variance limits, breaking the f - b degeneracy and allowing inference of the matter power spectrum from the galaxy survey. We analyse the growth constraints from a realistic tomographic weak-lensing photo-z survey combined with a spectroscopic galaxy redshift survey over the same sky area. For sky coverage fsky= 0.5, analysis of the transverse modes measures b to 2–3 per cent accuracy per Δz= 0.1 bin at z < 1 when ∼10 galaxies arcmin−2 are measured in the lensing survey and all haloes with M > Mmin= 1013 h−1 M⊙ have spectra. For the gravitational growth parameter parameter γ (
, combining the lensing information with RSD analysis of non-transverse modes yields accuracy σ(γ) ≈ 0.01. Adding lensing information to the RSD survey improves σ(γ) by an amount equivalent to a 3 × (10 ×) increase in the RSD survey area when the spectroscopic survey extends down to halo mass 1013.5 (1014) h−1 M⊙. We also find that the σ(γ) of overlapping surveys is equivalent to that of surveys 1.5–2× larger if they are separated on the sky. This gain is greatest when the spectroscopic mass threshold is 1013–1014 h−1 M⊙, similar to Luminous Red Galaxy surveys. The gain of overlapping surveys is reduced for very deep or very shallow spectroscopic surveys, but any practical surveys are more powerful when overlapped than when separated. The gain of overlapped surveys is larger in the case when the primordial power spectrum normalization is uncertain by >0.5 per cent.

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