Euclid: Covariance of weak lensing pseudo-Cl estimates: Calculation, comparison to simulations, and dependence on survey geometry
An accurate covariance matrix is essential for obtaining reliable cosmological results when using a Gaussian likelihood. In this paper we study the covariance of pseudo- C ℓ estimates of tomographic cosmic shear power spectra. Using two existing publicly available codes in combination, we calculate...
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Veröffentlicht in: | Astronomy and astrophysics (Berlin) 2022, Vol.660 |
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creator | Upham, Robin E Brown, M.L Whittaker, L Amara, A Auricchio, N Bonino, D Branchini, E Brescia, Massimo Brinchmann, J Capobianco, V Carbone, C Carretero, J Castellano, M Cavuoti, Stefano Cimatti, A Cledassou, R Congedo, G Conversi, L Copin, Y Corcione, L Cropper, M Da Silva, A Degaudenzi, H Douspis, M Dubath, F Duncan, C.A.J Dupac, X Dusini, S Ealet, A Farrens, S Ferriol, S Fosalba, P Frailis, M Franceschi, E Fumana, M Garilli, B Gillis, B Giocoli, C Grupp, F Haugan, Stein Vidar Hagfors Hoekstra, H Holmes, W Hormuth, F Jahnke, K Kermiche, S Kiessling, A Kilbinger, M Kitching, T Kümmel, M Kunz, M Kurki-Suonio, Hannu Ligori, S Lilje, Per Barth Lloro, I Marggraf, O Markovic, K Marulli, F Meneghetti, M Meylan, G Moresco, M Munari, E Niemi, S.M Padilla, C Paltani, S Pasian, F Pedersen, K Pettorino, V Pires, S Raison, F Rhodes, J Rossetti, E Saglia, R Sartoris, B Schneider, P Secroun, A Seidel, G Sirignano, C Sirri, G Stanco, L Starck, J.-L Tallada-Crespí, P Tavagnacco, D Taylor, A.N Tereno, I Toledo-Moreo, R Torradeflot, F Valenziano, L Wang, Y Zamorani, G Zoubian, J Andreon, S Baldi, M Camera, S Cardone, V.F Fabbian, G Polenta, G Joachimi, B Hall, A Loureiro, A Sellentin, E |
description | An accurate covariance matrix is essential for obtaining reliable cosmological results when using a Gaussian likelihood. In this paper we study the covariance of pseudo- C ℓ estimates of tomographic cosmic shear power spectra. Using two existing publicly available codes in combination, we calculate the full covariance matrix, including mode-coupling contributions arising from both partial sky coverage and non-linear structure growth. For three different sky masks, we compare the theoretical covariance matrix to that estimated from publicly available N -body weak lensing simulations, finding good agreement. We find that as a more extreme sky cut is applied, a corresponding increase in both Gaussian off-diagonal covariance and non-Gaussian super-sample covariance is observed in both theory and simulations, in accordance with expectations. Studying the different contributions to the covariance in detail, we find that the Gaussian covariance dominates along the main diagonal and the closest off-diagonals, but farther away from the main diagonal the super-sample covariance is dominant. Forming mock constraints in parameters that describe matter clustering and dark energy, we find that neglecting non-Gaussian contributions to the covariance can lead to underestimating the true size of confidence regions by up to 70 per cent. The dominant non-Gaussian covariance component is the super-sample covariance, but neglecting the smaller connected non-Gaussian covariance can still lead to the underestimation of uncertainties by 10–20 per cent. A real cosmological analysis will require marginalisation over many nuisance parameters, which will decrease the relative importance of all cosmological contributions to the covariance, so these values should be taken as upper limits on the importance of each component. |
doi_str_mv | 10.1051/0004-6361/202142908 |
format | Article |
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In this paper we study the covariance of pseudo- C ℓ estimates of tomographic cosmic shear power spectra. Using two existing publicly available codes in combination, we calculate the full covariance matrix, including mode-coupling contributions arising from both partial sky coverage and non-linear structure growth. For three different sky masks, we compare the theoretical covariance matrix to that estimated from publicly available N -body weak lensing simulations, finding good agreement. We find that as a more extreme sky cut is applied, a corresponding increase in both Gaussian off-diagonal covariance and non-Gaussian super-sample covariance is observed in both theory and simulations, in accordance with expectations. Studying the different contributions to the covariance in detail, we find that the Gaussian covariance dominates along the main diagonal and the closest off-diagonals, but farther away from the main diagonal the super-sample covariance is dominant. Forming mock constraints in parameters that describe matter clustering and dark energy, we find that neglecting non-Gaussian contributions to the covariance can lead to underestimating the true size of confidence regions by up to 70 per cent. The dominant non-Gaussian covariance component is the super-sample covariance, but neglecting the smaller connected non-Gaussian covariance can still lead to the underestimation of uncertainties by 10–20 per cent. A real cosmological analysis will require marginalisation over many nuisance parameters, which will decrease the relative importance of all cosmological contributions to the covariance, so these values should be taken as upper limits on the importance of each component.</description><identifier>ISSN: 0004-6361</identifier><identifier>EISSN: 1432-0746</identifier><identifier>EISSN: 1432-0756</identifier><identifier>DOI: 10.1051/0004-6361/202142908</identifier><language>eng ; nor</language><publisher>EDP Sciences</publisher><subject>Astrophysics ; Instrumentation and Detectors ; Physics</subject><ispartof>Astronomy and astrophysics (Berlin), 2022, Vol.660</ispartof><rights>info:eu-repo/semantics/openAccess</rights><rights>Distributed under a Creative Commons Attribution 4.0 International License</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-0808-6908 ; 0000-0002-0641-3231 ; 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M</creatorcontrib><creatorcontrib>Kitching, T</creatorcontrib><creatorcontrib>Kümmel, M</creatorcontrib><creatorcontrib>Kunz, M</creatorcontrib><creatorcontrib>Kurki-Suonio, Hannu</creatorcontrib><creatorcontrib>Ligori, S</creatorcontrib><creatorcontrib>Lilje, Per Barth</creatorcontrib><creatorcontrib>Lloro, I</creatorcontrib><creatorcontrib>Marggraf, O</creatorcontrib><creatorcontrib>Markovic, K</creatorcontrib><creatorcontrib>Marulli, F</creatorcontrib><creatorcontrib>Meneghetti, M</creatorcontrib><creatorcontrib>Meylan, G</creatorcontrib><creatorcontrib>Moresco, M</creatorcontrib><creatorcontrib>Munari, E</creatorcontrib><creatorcontrib>Niemi, S.M</creatorcontrib><creatorcontrib>Padilla, C</creatorcontrib><creatorcontrib>Paltani, S</creatorcontrib><creatorcontrib>Pasian, F</creatorcontrib><creatorcontrib>Pedersen, K</creatorcontrib><creatorcontrib>Pettorino, V</creatorcontrib><creatorcontrib>Pires, S</creatorcontrib><creatorcontrib>Raison, F</creatorcontrib><creatorcontrib>Rhodes, J</creatorcontrib><creatorcontrib>Rossetti, E</creatorcontrib><creatorcontrib>Saglia, R</creatorcontrib><creatorcontrib>Sartoris, B</creatorcontrib><creatorcontrib>Schneider, P</creatorcontrib><creatorcontrib>Secroun, A</creatorcontrib><creatorcontrib>Seidel, G</creatorcontrib><creatorcontrib>Sirignano, C</creatorcontrib><creatorcontrib>Sirri, G</creatorcontrib><creatorcontrib>Stanco, L</creatorcontrib><creatorcontrib>Starck, J.-L</creatorcontrib><creatorcontrib>Tallada-Crespí, P</creatorcontrib><creatorcontrib>Tavagnacco, D</creatorcontrib><creatorcontrib>Taylor, A.N</creatorcontrib><creatorcontrib>Tereno, I</creatorcontrib><creatorcontrib>Toledo-Moreo, R</creatorcontrib><creatorcontrib>Torradeflot, F</creatorcontrib><creatorcontrib>Valenziano, L</creatorcontrib><creatorcontrib>Wang, Y</creatorcontrib><creatorcontrib>Zamorani, G</creatorcontrib><creatorcontrib>Zoubian, J</creatorcontrib><creatorcontrib>Andreon, S</creatorcontrib><creatorcontrib>Baldi, M</creatorcontrib><creatorcontrib>Camera, S</creatorcontrib><creatorcontrib>Cardone, V.F</creatorcontrib><creatorcontrib>Fabbian, G</creatorcontrib><creatorcontrib>Polenta, G</creatorcontrib><creatorcontrib>Joachimi, B</creatorcontrib><creatorcontrib>Hall, A</creatorcontrib><creatorcontrib>Loureiro, A</creatorcontrib><creatorcontrib>Sellentin, E</creatorcontrib><title>Euclid: Covariance of weak lensing pseudo-Cl estimates: Calculation, comparison to simulations, and dependence on survey geometry</title><title>Astronomy and astrophysics (Berlin)</title><description>An accurate covariance matrix is essential for obtaining reliable cosmological results when using a Gaussian likelihood. In this paper we study the covariance of pseudo- C ℓ estimates of tomographic cosmic shear power spectra. Using two existing publicly available codes in combination, we calculate the full covariance matrix, including mode-coupling contributions arising from both partial sky coverage and non-linear structure growth. For three different sky masks, we compare the theoretical covariance matrix to that estimated from publicly available N -body weak lensing simulations, finding good agreement. We find that as a more extreme sky cut is applied, a corresponding increase in both Gaussian off-diagonal covariance and non-Gaussian super-sample covariance is observed in both theory and simulations, in accordance with expectations. Studying the different contributions to the covariance in detail, we find that the Gaussian covariance dominates along the main diagonal and the closest off-diagonals, but farther away from the main diagonal the super-sample covariance is dominant. Forming mock constraints in parameters that describe matter clustering and dark energy, we find that neglecting non-Gaussian contributions to the covariance can lead to underestimating the true size of confidence regions by up to 70 per cent. The dominant non-Gaussian covariance component is the super-sample covariance, but neglecting the smaller connected non-Gaussian covariance can still lead to the underestimation of uncertainties by 10–20 per cent. A real cosmological analysis will require marginalisation over many nuisance parameters, which will decrease the relative importance of all cosmological contributions to the covariance, so these values should be taken as upper limits on the importance of each component.</description><subject>Astrophysics</subject><subject>Instrumentation and 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Covariance of weak lensing pseudo-Cl estimates: Calculation, comparison to simulations, and dependence on survey geometry</title><author>Upham, Robin E ; Brown, M.L ; Whittaker, L ; Amara, A ; Auricchio, N ; Bonino, D ; Branchini, E ; Brescia, Massimo ; Brinchmann, J ; Capobianco, V ; Carbone, C ; Carretero, J ; Castellano, M ; Cavuoti, Stefano ; Cimatti, A ; Cledassou, R ; Congedo, G ; Conversi, L ; Copin, Y ; Corcione, L ; Cropper, M ; Da Silva, A ; Degaudenzi, H ; Douspis, M ; Dubath, F ; Duncan, C.A.J ; Dupac, X ; Dusini, S ; Ealet, A ; Farrens, S ; Ferriol, S ; Fosalba, P ; Frailis, M ; Franceschi, E ; Fumana, M ; Garilli, B ; Gillis, B ; Giocoli, C ; Grupp, F ; Haugan, Stein Vidar Hagfors ; Hoekstra, H ; Holmes, W ; Hormuth, F ; Jahnke, K ; Kermiche, S ; Kiessling, A ; Kilbinger, M ; Kitching, T ; Kümmel, M ; Kunz, M ; Kurki-Suonio, Hannu ; Ligori, S ; Lilje, Per Barth ; Lloro, I ; Marggraf, O ; Markovic, K ; Marulli, F ; Meneghetti, M ; Meylan, G ; Moresco, M ; Munari, E ; Niemi, S.M ; Padilla, C ; Paltani, S ; Pasian, F ; Pedersen, K ; Pettorino, V ; Pires, S ; Raison, F ; Rhodes, J ; Rossetti, E ; Saglia, R ; Sartoris, B ; Schneider, P ; Secroun, A ; Seidel, G ; Sirignano, C ; Sirri, G ; Stanco, L ; Starck, J.-L ; Tallada-Crespí, P ; Tavagnacco, D ; Taylor, A.N ; Tereno, I ; Toledo-Moreo, R ; Torradeflot, F ; Valenziano, L ; Wang, Y ; Zamorani, G ; Zoubian, J ; Andreon, S ; Baldi, M ; Camera, S ; Cardone, V.F ; Fabbian, G ; Polenta, G ; Joachimi, B ; Hall, A ; Loureiro, A ; Sellentin, E</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c581-7ec29aebf6451ee101415daab0fa20ff0efe6a1191af5744480419284d4a88dd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng ; nor</language><creationdate>2022</creationdate><topic>Astrophysics</topic><topic>Instrumentation and Detectors</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Upham, 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G</creatorcontrib><creatorcontrib>Zoubian, J</creatorcontrib><creatorcontrib>Andreon, S</creatorcontrib><creatorcontrib>Baldi, M</creatorcontrib><creatorcontrib>Camera, S</creatorcontrib><creatorcontrib>Cardone, V.F</creatorcontrib><creatorcontrib>Fabbian, G</creatorcontrib><creatorcontrib>Polenta, G</creatorcontrib><creatorcontrib>Joachimi, B</creatorcontrib><creatorcontrib>Hall, A</creatorcontrib><creatorcontrib>Loureiro, A</creatorcontrib><creatorcontrib>Sellentin, E</creatorcontrib><collection>NORA - Norwegian Open Research Archives</collection><collection>Hyper Article en Ligne (HAL)</collection><collection>Hyper Article en Ligne (HAL) (Open Access)</collection><jtitle>Astronomy and astrophysics (Berlin)</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Upham, Robin E</au><au>Brown, M.L</au><au>Whittaker, L</au><au>Amara, A</au><au>Auricchio, N</au><au>Bonino, D</au><au>Branchini, E</au><au>Brescia, Massimo</au><au>Brinchmann, J</au><au>Capobianco, V</au><au>Carbone, C</au><au>Carretero, J</au><au>Castellano, M</au><au>Cavuoti, Stefano</au><au>Cimatti, A</au><au>Cledassou, R</au><au>Congedo, G</au><au>Conversi, L</au><au>Copin, Y</au><au>Corcione, L</au><au>Cropper, M</au><au>Da Silva, A</au><au>Degaudenzi, H</au><au>Douspis, M</au><au>Dubath, F</au><au>Duncan, C.A.J</au><au>Dupac, X</au><au>Dusini, S</au><au>Ealet, A</au><au>Farrens, S</au><au>Ferriol, S</au><au>Fosalba, P</au><au>Frailis, M</au><au>Franceschi, E</au><au>Fumana, M</au><au>Garilli, B</au><au>Gillis, B</au><au>Giocoli, C</au><au>Grupp, F</au><au>Haugan, Stein Vidar Hagfors</au><au>Hoekstra, H</au><au>Holmes, W</au><au>Hormuth, F</au><au>Jahnke, K</au><au>Kermiche, S</au><au>Kiessling, A</au><au>Kilbinger, M</au><au>Kitching, T</au><au>Kümmel, M</au><au>Kunz, M</au><au>Kurki-Suonio, Hannu</au><au>Ligori, S</au><au>Lilje, Per Barth</au><au>Lloro, I</au><au>Marggraf, O</au><au>Markovic, K</au><au>Marulli, F</au><au>Meneghetti, M</au><au>Meylan, G</au><au>Moresco, M</au><au>Munari, E</au><au>Niemi, S.M</au><au>Padilla, C</au><au>Paltani, S</au><au>Pasian, F</au><au>Pedersen, K</au><au>Pettorino, V</au><au>Pires, S</au><au>Raison, F</au><au>Rhodes, J</au><au>Rossetti, E</au><au>Saglia, R</au><au>Sartoris, B</au><au>Schneider, P</au><au>Secroun, A</au><au>Seidel, G</au><au>Sirignano, C</au><au>Sirri, G</au><au>Stanco, L</au><au>Starck, J.-L</au><au>Tallada-Crespí, P</au><au>Tavagnacco, D</au><au>Taylor, A.N</au><au>Tereno, I</au><au>Toledo-Moreo, R</au><au>Torradeflot, F</au><au>Valenziano, L</au><au>Wang, Y</au><au>Zamorani, G</au><au>Zoubian, J</au><au>Andreon, S</au><au>Baldi, M</au><au>Camera, S</au><au>Cardone, V.F</au><au>Fabbian, G</au><au>Polenta, G</au><au>Joachimi, B</au><au>Hall, A</au><au>Loureiro, A</au><au>Sellentin, E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Euclid: Covariance of weak lensing pseudo-Cl estimates: Calculation, comparison to simulations, and dependence on survey geometry</atitle><jtitle>Astronomy and astrophysics (Berlin)</jtitle><date>2022</date><risdate>2022</risdate><volume>660</volume><issn>0004-6361</issn><eissn>1432-0746</eissn><eissn>1432-0756</eissn><abstract>An accurate covariance matrix is essential for obtaining reliable cosmological results when using a Gaussian likelihood. In this paper we study the covariance of pseudo- C ℓ estimates of tomographic cosmic shear power spectra. Using two existing publicly available codes in combination, we calculate the full covariance matrix, including mode-coupling contributions arising from both partial sky coverage and non-linear structure growth. For three different sky masks, we compare the theoretical covariance matrix to that estimated from publicly available N -body weak lensing simulations, finding good agreement. We find that as a more extreme sky cut is applied, a corresponding increase in both Gaussian off-diagonal covariance and non-Gaussian super-sample covariance is observed in both theory and simulations, in accordance with expectations. Studying the different contributions to the covariance in detail, we find that the Gaussian covariance dominates along the main diagonal and the closest off-diagonals, but farther away from the main diagonal the super-sample covariance is dominant. Forming mock constraints in parameters that describe matter clustering and dark energy, we find that neglecting non-Gaussian contributions to the covariance can lead to underestimating the true size of confidence regions by up to 70 per cent. The dominant non-Gaussian covariance component is the super-sample covariance, but neglecting the smaller connected non-Gaussian covariance can still lead to the underestimation of uncertainties by 10–20 per cent. A real cosmological analysis will require marginalisation over many nuisance parameters, which will decrease the relative importance of all cosmological contributions to the covariance, so these values should be taken as upper limits on the importance of each component.</abstract><pub>EDP Sciences</pub><doi>10.1051/0004-6361/202142908</doi><orcidid>https://orcid.org/0000-0002-0808-6908</orcidid><orcidid>https://orcid.org/0000-0002-0641-3231</orcidid><orcidid>https://orcid.org/0000-0002-2318-301X</orcidid><orcidid>https://orcid.org/0000-0003-1225-7084</orcidid><orcidid>https://orcid.org/0000-0002-7616-7136</orcidid><orcidid>https://orcid.org/0000-0002-8108-9179</orcidid><orcidid>https://orcid.org/0000-0002-4485-8549</orcidid><orcidid>https://orcid.org/0000-0002-5094-2245</orcidid><orcidid>https://orcid.org/0000-0003-3399-3574</orcidid><orcidid>https://orcid.org/0000-0001-9875-8263</orcidid><orcidid>https://orcid.org/0000-0002-9594-9387</orcidid><orcidid>https://orcid.org/0000-0001-7455-8750</orcidid><orcidid>https://orcid.org/0000-0003-2508-0046</orcidid><orcidid>https://orcid.org/0000-0002-8850-0303</orcidid><orcidid>https://orcid.org/0000-0003-1962-9805</orcidid><orcidid>https://orcid.org/0000-0002-4409-5633</orcidid><orcidid>https://orcid.org/0000-0003-0378-7032</orcidid><orcidid>https://orcid.org/0000-0003-4359-8797</orcidid><orcidid>https://orcid.org/0000-0002-9590-7961</orcidid><orcidid>https://orcid.org/0000-0001-9513-7138</orcidid><orcidid>https://orcid.org/0000-0002-5317-7518</orcidid><orcidid>https://orcid.org/0000-0002-1510-5214</orcidid><orcidid>https://orcid.org/0000-0003-3804-2137</orcidid><orcidid>https://orcid.org/0000-0001-7951-0166</orcidid><orcidid>https://orcid.org/0000-0003-4145-1943</orcidid><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0004-6361 |
ispartof | Astronomy and astrophysics (Berlin), 2022, Vol.660 |
issn | 0004-6361 1432-0746 1432-0756 |
language | eng ; nor |
recordid | cdi_hal_primary_oai_HAL_hal_03601240v1 |
source | Bacon EDP Sciences France Licence nationale-ISTEX-PS-Journals-PFISTEX; EDP Sciences; NORA - Norwegian Open Research Archives; Elektronische Zeitschriftenbibliothek - Frei zugängliche E-Journals |
subjects | Astrophysics Instrumentation and Detectors Physics |
title | Euclid: Covariance of weak lensing pseudo-Cl estimates: Calculation, comparison to simulations, and dependence on survey geometry |
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