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Treating observational systematics for LSS in photometric surveys

Rodriguez-Monroy, Martin

Abstract

Given the huge amount of data that stage IV cosmology surveys, such as LSST-DESC and Euclid will provide, statistical errors will shrink even lower than in previous stage surveys, such as DES, so systematic errors will become the main sources of uncertainty. Therefore it will be essential to know in detail the different sources of systematic effects and to correct for them appropriately in order to avoid significant biases on the results from different probes. In this sense, galaxy clustering measurements are not an exception to this problem, with observational systematics being of particular relevance. In this contribution we present how we can apply different methodologies to the treat the observational systematics in the galaxy clustering measurements from coming and current surveys.

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Treating observational systematics for LSS in photometric surveys X Meeting on Fundamental Cosmology Seville, 18-10-2024 Martín Rodríguez Monroy IFT, Madrid, Spain The Dark Energy Survey 2 DES survey evolution 3 Sevilla-Noarbe et al. 2021 Rodríguez-Monroy et al. 2021 DES-Y3 results: galaxy clustering 4 DES Collaboration et al. 2021 DES-Y3 cosmology and Y6 BAO results 5 DES Collaboration: Abbott et al., 2024 Stage IV surveys: LSST and Euclid 6 Bianco et al., 2021 Stage IV surveys: LSST and Euclid Using the current baseline cadence, LSST ten-year survey will take more than five million exposures, collecting over 50 petabytes of raw image data to produce a deep, time-dependent, movie of about 20,000 square degrees of sky. 7 Euclid Wide Survey (EWS) coverage and colour-coded yearly progress. Blue borders = 16000 deg2 region of interest that contains the 13416 deg2 observed sky of the EWS. Euclid. I. Overview of the Euclid mission Image credit: Elisa Chisari and Nacho Sevilla 8 LSST and Euclid: cosmology forecasts Euclid. I. Overview of the Euclid mission LSST-DESC Euclid Pushing the limits of statistical error! 9 LSST and Euclid: cosmology forecasts Euclid. I. Overview of the Euclid mission LSST-DESC Euclid Pushing the limits of statistical error! Image credit: Elisa Chisari and Nacho Sevilla 16 ● Stacking of images ⇒ need summary statistic (weighted mean, min., max., variance….) ● Several photometric bands ○ DES: griz ○ LSST: ugrizY ○ Euclid: YE, JE, HE Pearson’s coeff. ● Several astrophysical foregrounds: stars, dust extinction, HI…. ● Many maps are (highly) correlated → dimensionality reduction: ○ PCA ○ SOMs ● Risks = under / overcorrection ●Must use data-driven selections Observational systematics: template selection 16 DES-Y3 contamination templates (i-band) Mitigation methods for observational systematics 17 18 Modeling of observational systematic contamination: δg obs = f(s) + δg true , so δg true is the residual from the fit ●What is the form of f(s)? ○ 1-dimensional regression ■ Iterative process ○ Multi-dimensional regression ○ More complex method δg syst 1 e.g. PSF syst 2 e.g. depth Healpix pixels s = template of contamination Observational systematics: modeling 19 Modeling of observational systematic contamination: δg obs = f(s) + δg true , so δg true is the residual from the fit δg syst 1 e.g. PSF syst 2 e.g. depth Healpix pixels s = template of contamination 19 Observational systematics: modeling True density field Net systematic contaminant Observed density field Set of systematic maps Weaverdyck & Huterer 2007.14499 ⨉ δg obs = f(s) + δg true δg true Preliminary cleaning: ● Identify and mask out extreme regions (pixels) Use available SP maps to model δg obs and mitigate contamination. How? ● Act at the observable / estimator level (e.g. w(θ)) ● Modify randoms used by estimator (e.g. Landy-Szalay) ●Act at the map level (e.g. δg field) → weight map Observed on the ground Back to truth 20 Correcting for observational systematics DES correction methods: ENet Elastic Net (ENet) regularization = LASSO + ridge regressions (Zou & Hastie 2005) ● Multilinear fit in N-dim space (N SP maps) ●All SP maps are associated a contamination amplitude, αi ● Avoid over correction: ○ ○LASSO (L1) term: penalises non-zero αi ⇒ favours scarcity of explanatory variables ○ ○Ridge (L2) term: penalises correlated variables ○ ● ENet ⇒ minimize loss function: ● Estimate λ1 and λ2 with cross-validation on data subsets LASSO Ridge OLS 21 DES correction methods: ISD Apply the weight map to our galaxy sample 23 Identify most significant SP map 4 Iterative systematics decontamination (ISD) in a nutshell: ●Fix a threshold for 1D contamination ● Iterative process: ○5 Re-evaluate significance of SPs until process converges ○1 Define 1D significance by evaluating against log-normal mocks 22 23 ●SOM systematics ○ Reduces dimensionality ○ Considers all maps at once ○ Non-linear parameterization ●Neural net(s) ○ First steps in the use of AI for systematics ○ Problem reframing for exploiting AI capabilities → solutions can vary from neural networks to evolutionary algorithms ●Alternative regularisation method ●Random-level method ○ Recovering and updating old method based on depth (DARTH-systematics) Ongoing work at IFT: new methods for LSST-DESC / Euclid on DES Methods validation Validation on simulations and data: ●Methods performance / configuration ●Completeness of SP map set ●Methodological blind spots ●Systematic contribution to covariance: ○Over / undercorrection ○Difference between methods ●Impact on cosmology ●Cross-correlation with external tracers Rodríguez-Monroy, Weaverdyck+. 2105.13540 24 Summary 25 Methods validation Validation on simulations and data: ●Methods performance / configuration ●Completeness of SP map set ●Methodological blind spots Rodríguez-Monroy, Weaverdyck+. 2105.13540 ●Different method assumptions → different corrections 32 Additional robustness tests Similar results for MagLim 33 Correlations with LSS 34 Correlations with LSS 35