Brighter-fatter Effect in Near-infrared Detectors. I. Theory of Flat Autocorrelations

Weak gravitational lensing studies aim to measure small distortions in the shapes of distant galaxies, and thus place very tight demands on the understanding of detector-induced systematic effects in astronomical images. The Wide-Field Infrared Survey Telescope (WFIRST) will carry out weak lensing measurements in the near infrared using the new Teledyne H4RG-10 detector arrays, which makes the range of possible detector systematics very different from traditional weak lensing measurements using optical CCDs. One of the non-linear detector effects observed in CCDs is the brighter-fatter effect (BFE), in which charge already accumulated in a pixel alters the electric field geometry and causes new charge to be deflected away from brighter pixels. Here we describe the formalism for measuring the BFE using flat field correlation functions in infrared detector arrays. The auto-correlation of CCD flat fields is often used to measure the BFE, but because the infrared detector arrays are read out with the charge "in place," the flat field correlations are dominated by capacitive cross-talk between neighboring pixels (the inter-pixel capacitance, or IPC). Conversely, if the BFE is present and one does not account for it, it can bias correlation measurements of the IPC and photon transfer measurements of the gain. We show that because the infrared detector arrays can be read out non-destructively, one can compute numerous cross-correlation functions between different time slices of the same flat exposures, and that correlations due to IPC and BFE leave distinct imprints. We generate a suite of simulated flat fields and show that the underlying IPC and BFE parameters can be extracted, even when both are present in the simulation. There are some biases in the BFE coefficients up to 12%, which are likely caused by higher order terms that are dropped from this analysis.

[1]  Cheryl Pavlovsky,et al.  Persistence and count-rate nonlinearity in the HST WFC3 IR detector , 2010, Astronomical Telescopes + Instrumentation.

[2]  Gary M. Bernstein,et al.  Characterization and correction of charge-induced pixel shifts in DECam , 2015, 1501.02802.

[3]  Awad Aubad,et al.  Towards a framework building for social systems modelling , 2020 .

[4]  Bernard J. Rauscher Teledyne H1RG, H2RG, and H4RG Noise Generator , 2015 .

[5]  Prasanth H. Nair,et al.  Astropy: A community Python package for astronomy , 2013, 1307.6212.

[6]  Kendrick M. Smith,et al.  Exploring the Brighter-fatter Effect with the Hyper Suprime-Cam , 2017, The Astronomical Journal.

[7]  C. B. D'Andrea,et al.  Cosmology from cosmic shear with Dark Energy Survey science verification data , 2015, 1507.05552.

[8]  Peter Sinclaire,et al.  CCD riddle: a) signal vs time: linear; b) signal vs variance: non-linear , 2006, SPIE Astronomical Telescopes + Instrumentation.

[9]  John D. Hunter,et al.  Matplotlib: A 2D Graphics Environment , 2007, Computing in Science & Engineering.

[10]  John Auyeung,et al.  Progress in development of H4RG-10 infrared focal plane arrays for WFIRST-AFTA , 2013, Astronomical Telescopes and Instrumentation.

[11]  E. al.,et al.  Detectors for the James Webb Space Telescope near-infrared spectrograph. I. Readout mode, noise model, and calibration considerations , 2007, 0706.2344.

[12]  Robert J. Hill,et al.  Reciprocity failure in 1.7 μm cut-off HgCdTe detectors , 2010, Astronomical Telescopes + Instrumentation.

[13]  Adam G. Riess,et al.  Grism Sensitivities and Apparent Non-Linearity , 2005 .

[14]  Mark Cropper,et al.  Measuring a charge-coupled device point spread function , 2014, 1412.5382.

[15]  Jeffrey W. Kruk,et al.  The Impact of Interpixel Capacitance in CMOS Detectors on PSF Shapes and Implications for WFIRST , 2015, 1512.01570.

[16]  Rachel Mandelbaum,et al.  The Effect of Detector Nonlinearity on WFIRST PSF Profiles for Weak Gravitational Lensing Measurements , 2016, 1605.01001.

[17]  J. Beletic OPTICAL AND INFRARED DETECTORS FOR ASTRONOMY , 2006 .

[18]  Peter Rankin McCullough,et al.  Quantum Efficiency and Quantum Yield of an HgCdTe Infrared Sensor Array , 2008 .

[19]  J. Rhodes,et al.  Laboratory Measurement of the Brighter-fatter Effect in an H2RG Infrared Detector , 2017, 1712.06642.

[20]  P. Astier,et al.  The brighter-fatter effect and pixel correlations in CCD sensors , 2014, 1402.0725.

[21]  Z. Ninkov,et al.  Point-spread Function Ramifications and Deconvolution of a Signal Dependent Blur Kernel Due to Interpixel Capacitive Coupling , 2018, Publications of the Astronomical Society of the Pacific.

[22]  Markus Loose,et al.  Teledyne Imaging Sensors: infrared imaging technologies for astronomy and civil space , 2008, Astronomical Telescopes + Instrumentation.

[23]  P. Schneider,et al.  KiDS-450: cosmological parameter constraints from tomographic weak gravitational lensing , 2016, 1606.05338.

[24]  Ori Dosovitz Fox,et al.  The 55Fe X-Ray Energy Response of Mercury Cadmium Telluride Near-Infrared Detector Arrays , 2008, Astronomical Telescopes + Instrumentation.

[25]  Yannick Mellier,et al.  CFHTLenS tomographic weak lensing cosmological parameter constraints: Mitigating the impact of intrinsic galaxy alignments , 2013, 1303.1808.

[26]  Kevan Donlon,et al.  Modeling of hybridized infrared arrays for characterization of interpixel capacitive coupling , 2017, 1701.07062.

[27]  Eric Jones,et al.  SciPy: Open Source Scientific Tools for Python , 2001 .

[28]  Pierre Astier,et al.  The shape of the photon transfer curve of CCD sensors , 2019, Astronomy & Astrophysics.

[29]  L. Mortara,et al.  Evaluations Of Charge-Coupled Device (CCD) Performance For Astronomical Use , 1981, Other Conferences.

[30]  Edward J. Wollack,et al.  Wide-Field InfrarRed Survey Telescope-Astrophysics Focused Telescope Assets WFIRST-AFTA 2015 Report , 2015, 1503.03757.

[31]  G. Tarle,et al.  Correlated Noise and Gain in Unfilled and Epoxy‐Underfilled Hybridized HgCdTe Detectors , 2006 .

[32]  Andrew Bradshaw,et al.  Measurements and simulations of the brighter-fatter effect in CCD sensors , 2017, 1703.05823.

[33]  J. Rhodes,et al.  Nonlinearity and pixel shifting effects in HXRG infrared detectors , 2017, 1703.08205.

[34]  Miguel de Val-Borro,et al.  The Astropy Project: Building an Open-science Project and Status of the v2.0 Core Package , 2018, The Astronomical Journal.

[35]  P. Astier,et al.  Evidence for self-interaction of charge distribution in charge-coupled devices , 2015, 1501.01577.

[36]  D. J. Fixsen,et al.  Principal component analysis of up-the-ramp sampled infrared array data , 2019, Journal of Astronomical Telescopes, Instruments, and Systems.

[37]  James R. Janesick,et al.  CCD Charge Collection Efficiency And The Photon Transfer Technique , 1985, Optics & Photonics.

[38]  D. Martin,et al.  Characterization of HAWAII-2RG detector and SIDECAR ASIC for the Euclid mission at ESA , 2012, Other Conferences.

[39]  Zoran Ninkov,et al.  Quantum efficiency overestimation and deterministic cross talk resulting from interpixel capacitance , 2006 .

[40]  S. P. Littlefair,et al.  THE ASTROPY PROJECT: BUILDING AN INCLUSIVE, OPEN-SCIENCE PROJECT AND STATUS OF THE V2.0 CORE PACKAGE , 2018 .

[41]  Aaron Roodman,et al.  Intrinsic Pixel Size Variation in an LSST Prototype Sensor , 2015 .

[42]  Zoran Ninkov,et al.  Interpixel capacitance in nondestructive focal plane arrays , 2004, SPIE Optics + Photonics.

[43]  Kevan Donlon,et al.  Signal dependence of inter-pixel capacitance in hybridized HgCdTe H2RG arrays for use in James Webb space telescope's NIRcam , 2016, Astronomical Telescopes + Instrumentation.

[44]  Anirban DasGupta,et al.  Probability for Statistics and Machine Learning , 2011 .