The importance of magnification effects in galaxy-galaxy lensing
The importance of magnification effects in galaxy-galaxy lensing
复制标题
星系-星系透镜效应中放大效应的重要性
DOI:
10.1051/0004-6361/201936915
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发表时间:
2020
影响因子:
6.5
通讯作者:
Corella Puertas
中科院分区:
文献类型:
--
作者:
Schneider;Hilbert;Martin;Corella Puertas
Magnification changes the observed local number density of galaxies on the sky. This biases the observed tangential shear profiles around galaxies: the so-called galaxy-galaxy lensing (GGL) signal. Inference of physical quantities, such as the mean mass profile of halos around galaxies, are correspondingly affected by magnification effects. We used simulated shear and galaxy data from the Millennium Simulation to quantify the effect on shear and mass estimates from the magnified lens and source number counts. The former is due to the large-scale matter distribution in the foreground of the lenses; the latter is caused by magnification of the source population by the matter associated with the lenses. The GGL signal is calculated from the simulations by an efficient fast Fourier transform, which can also be applied to real data. The numerical treatment is complemented by a leading-order analytical description of the magnification effects, which is shown to fit the numerical shear data well. We find the magnification effect is strongest for steep galaxy luminosity functions and high redshifts. For a KiDS+VIKING+GAMA-like survey with lens galaxies at redshiftzd= 0.36 and source galaxies in the last three redshift bins with a mean redshift of , the magnification correction changes the shear profile up to 2%, and the mass is biased by up to 8%. We further considered an even higher redshift fiducial lens sample atzd= 0.83, with a limited magnitude of 22 mag in ther-band and a source redshift ofzs= 0.99. Through this, we find that a magnification correction changes the shear profile up to 45% and that the mass is biased by up to 55%. As expected, the sign of the bias depends on the local slope of the lens luminosity functionαd, where the mass is biased low forαd< 1 and biased high forαd> 1. While the magnification effect of sources is rarely more than 1% of the measured GGL signal, the statistical power of future weak lensing surveys warrants correction for this effect.
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