Systematic Errors in Weak Lensing Measurements Jun Zhang, Eiichiro Komatsu (The University of Texas at Austin) IHEP, Nov 8, 2011 arXiv: 1002.3614; 1002.3615;

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Systematic Errors in Weak Lensing Measurements Jun Zhang, Eiichiro Komatsu (The University of Texas at Austin) IHEP, Nov 8, 2011 arXiv: ; ; , Astro-ph/

Outline: Introduction of Weak Lensing Problems in Weak Lensing Measurement ◦ The Form of Cosmic Shear Estimator (general) ◦ The Reduced Shear (general) ◦ The Pixelation Effect (specific) ◦ The Photon Noise (specific) Summary

Introduction Credit: NASA / WMAP Science Team

Introduction Credit: NASA/WMAP

Introduction Credit: Wittman et al., (LSST team)

Introduction Image Credit: Hoekstra & Jain (2008) Credit: Clowe et al. (2006)

Introduction

Introduction y x y’ x’ Lensing

Introduction y x y’ x’ Lensing y x y’ x’ Lensing y x y’ x’ Lensing

Introduction

Introduction DES LSST WFIRST EUCLID HSC KDUST

Problems in Weak Lensing Measurements How to accurately measure the cosmic shear? The shear signal: a few percent V.S. Intrinsic variance of the galaxy ellipticity (shape noise): of order one Systematic errors are not tolerable!!!

引力透镜所致形变观测所致图像模糊 光子噪音 有限像素 LensingPSF Pixelation Noise Image Credit: GREAT08 team

Problems in Weak Lensing Measurements

Credit: Huterer et al. 2006, MNRAS, 366, 101

Problems in Weak Lensing Measurements Credit: Huterer et al. 2006, MNRAS, 366, 101

Problems in Weak Lensing Measurements Sources of Systematic Errors: Corrections due to the Point Spread Function (PSF); Photon Noise; Pixelation Effect; High Order Terms in Shear/Convergence; Charge Transfer Inefficiency; PSF determination from Star Shapes; Source Selection Bias; Photometric Redshift Errors; Galaxy Intrinsic Alignment.

Problems in Weak Lensing Measurements Sources of Systematic Errors: Corrections due to the Point Spread Function (PSF); Photon Noise; Pixelation Effect; High Order Terms in Shear/Convergence; Charge Transfer Inefficiency; PSF determination from Star Shapes; Source Selection Bias; Photometric Redshift Errors; Galaxy Intrinsic Alignment.

Problems in Weak Lensing Measurements The Form of Cosmic Shear Estimator (general) The Reduced Shear (general) The Pixelation Effect (specific) The Photon Noise (specific)

The Form of Shear Estimator STEP I, STEP II, GREAT 08, GREAT 10 ?

The Form of Shear Estimator

✗ ✔

Warming Up Exercise The Form of Shear Estimator

Warming Up Exercise The Form of Shear Estimator

Are there ideal/conventional shear estimators existing in convenient forms? ? The Form of Shear Estimator

Coordinate Rotation: The Form of Shear Estimator

Indeed, we only need to consider spin-2 shear estimators because of the following: The Form of Shear Estimator

On spin-2 shear estimators: The Form of Shear Estimator

On spin-2 shear estimators: Scalar Pseudo-Scalar Spin-4 The Form of Shear Estimator

On spin-2 shear estimators: The Form of Shear Estimator

Consider a special type of galaxies: (, ) The Form of Shear Estimator

Consider a special type of galaxies: The Form of Shear Estimator

Consider a special type of galaxies: The Form of Shear Estimator

Consider a special type of galaxies: The Form of Shear Estimator

Consider a special type of galaxies: The Form of Shear Estimator

Consider a special type of galaxies: Bartelmann & Schneider 2001, Phys. Rept., 340, 291 The Form of Shear Estimator

In the Presence of PSF: ? ✗ The Form of Shear Estimator

✗ ✔

✗ ✔

✗ ✔

Ref: Astro-ph/ , arXiv: , arXiv: The Form of Shear Estimator

Ref: Astro-ph/ , arXiv: , arXiv: The Form of Shear Estimator

 Correct for the Point Spread Function;  No Assumptions on the Morphologies of the Galaxies or the PSF;  Exact & Simple Math;  Well Defined Treatment of Background Noise;  Accurate to the 2nd Order in Shear/Convergence;  Immune to Misidentification of Sources (faint/small galaxies, stars)  < seconds/Galaxy  S / N per galaxy Increased. The Form of Shear Estimator

The Reduced Shear

If one plans to calibrate the multiplicative factor “a+b κ ”, one should pay attention to its dependence on “ κ ”, which, though, is not known a priori in observations.

The Reduced Shear Theorem:,

The Pixelation Effect (specific) Moffat PSFGaussian PSF FWHM of both PSF = 12

The Pixelation Effect (specific) FWHM (PSF) = 12

The Photon Noise (specific)

In fact :

A Fun Thing to Share

Summary The Form of Shear Estimator (general) The Reduced Shear (general) The Pixelation Effect (specific) The Photon Noise (specific)