4.7 Article

Near-IR Weak-lensing (NIRWL) Measurements in the CANDELS Fields. I. Point-spread Function Modeling and Systematics

Journal

ASTROPHYSICAL JOURNAL
Volume 958, Issue 1, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.3847/1538-4357/acfafd

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In this study, a near-IR weak-lensing analysis of CANDELS HST/WFC3-IR F160W observations was conducted, with updated astrometry of the mosaics achieving absolute alignment with a high degree of accuracy. Systematic effects in weak-lensing measurements were investigated, highlighting undersampling as a major contributing factor. PSF modeling for weak lensing using principal component analysis was performed, resulting in corrections that are sufficient for future NIRWL searches in the CANDELS fields.
We have undertaken a near-IR weak-lensing (NIRWL) analysis of the CANDELS HST/WFC3-IR F160W observations. With the Gaia proper motion-corrected catalog as an astrometric reference, we updated the astrometry of the five CANDELS mosaics and achieved an absolute alignment within 002 +/- 002, on average, which is a factor of several superior to existing mosaics. These mosaics are available to download (https://drive.google.com/drive/folders/1k9WEV3tBOuRKBlcaTJ0-wTZnUCisS__r). We investigated the systematic effects that need to be corrected for weak-lensing measurements. We find that the largest contributing systematic effect is caused by undersampling. We find a subpixel centroid dependence on the PSF shape that causes the PSF ellipticity and size to vary by up to 0.02% and 3%, respectively. Using the UDS as an example field, we show that undersampling induces a multiplicative shear bias of -0.025. We find that the brighter-fatter effect causes a 2% increase in the size of the PSF and discover a brighter-rounder effect that changes the ellipticity by 0.006. Based on the small range of slopes in a galaxy's spectral energy distribution (SED) within the WFC3-IR bandpasses, we suggest that the impact of the galaxy SED on the PSF is minor. Finally, we model the PSF of WFC3-IR F160W for weak lensing using a principal component analysis. The PSF models account for temporal and spatial variations of the PSF. The PSF corrections result in residual ellipticities and sizes, divided by de(1)divided by < 0.0005 +/- 0.0003, divided by de(2)divided by < 0.0005 +/- 0.0003, and divided by dR divided by < 0.0005 +/- 0.0001, that are sufficient for the upcoming NIRWL search for massive overdensities in the five CANDELS fields.

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