
Noise properties of gravitational lens mass reconstruction
Author(s) -
Waerbeke Ludovic Van
Publication year - 2000
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1046/j.1365-8711.2000.03259.x
Subject(s) - physics , gravitational lens , weak gravitational lensing , noise (video) , smoothing , statistical physics , galaxy , ansatz , gaussian random field , aperture (computer memory) , gaussian , astrophysics , redshift , statistics , gaussian function , mathematics , quantum mechanics , image (mathematics) , artificial intelligence , computer science , acoustics
Gravitational lensing is potentially able to observe mass‐selected haloes, and to measure the projected cluster mass function. An optimal mass selection requires a quantitative understanding of the noise behaviour in mass maps. This paper is an analysis of the noise properties in mass maps reconstructed from a maximum‐likelihood method. The first part of this work is the derivation of the noise power spectrum and the mass error bars as a straightforward extension of the Kaiser & Squires algorithm for the case of a correlated noise. Very good agreement is found between these calculations and the noise properties measured in the mass reconstructions limited to non‐critical clusters of galaxies. It demonstrates that Kaiser & Squires and maximum‐likelihood methods have similar noise properties and that the weak lensing approximation is valid for describing these properties. In a second stage I show that the statistics of peaks in the noise follows accurately the peak statistics of a two‐dimensional Gaussian random field (using the BBKS techniques) if the smoothing aperture contains enough galaxies. This analysis provides a full procedure for deriving the significance of any convergence peak as a function of its amplitude and profile. I demonstrate that a detailed quantitative analysis of the structures in mass maps can be carried out, and that, to a very good approximation, a mass map is the sum of the lensing signal and known two‐dimensional Gaussian random noise. A straightforward application is the measurement of the projected mass function in wide‐field lensing surveys, down to small mass overdensities that are individually undetectable.