Euclid preparation. XVIII. The NISP photometric system

Euclid will be the first space mission to survey most of the extragalactic sky in the 0.95-2.02 \(\mu\)m range, to a 5\(\sigma\) point-source median depth of 24.4 AB mag. This unique photometric data set will find wide use beyond Euclid's core science. In this paper, we present accurate computa...

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Veröffentlicht in:arXiv.org 2022-03
Hauptverfasser: Collaboration, Euclid, Schirmer, M, Jahnke, K, Seidel, G, Bodendorf, C, Grupp, F, Hormuth, F, Wachter, S, Barbier, R, Ganga, K, Hudelot, P, Auricchio, N, Balestra, A, Bender, R, Branchini, E, Cavuoti, S, Congedo, G, Conversi, L, Copin, Y, Courbin, F, Douspis, M, Dubath, F, Farrens, S, Garilli, B, Gillard, W, Guzzo, L, Hoekstra, H, Hornstrup, A, Kiessling, A, Kümmel, M, Kurki-Suonio, H, Laureijs, R, Ligori, S, Maiorano, E, Marggraf, O, Markovic, K, Marulli, F, Maurogordato, S, Mellier, Y, Merlin, E, Meylan, G, Nakajima, R, Nichol, R C, Niemi, S M, Padilla, C, Pasian, F, Poncet, M, Pozzetti, L, H -W Rix, Saglia, R, Scaramella, R, Schneider, P, Stanco, L, Toledo-Moreo, R, Torradeflot, F, Trifoglio, M, Valentijn, E A, Wang, Y, Weller, J, Zamorani, G, Zoubian, J, Farinelli, R, Medinaceli, E, Morisset, N, Polenta, G, Tenti, M, Balaguera-Antolínez, A, Biviano, A, Bozzo, E, Burigana, C, Cappi, A, Castignani, G, Cooray, A R, Courtois, H M, Crocce, M, Davini, S, de la Torre, S, Escartin, J A, Finelli, F, Garcia-Bellido, J, Gaztanaga, E, Hook, I M, Ilić, S, Kansal, V, Keihanen, E, McCracken, H J, Metcalf, R B, Monaco, P, Morgante, G, Nightingale, J, Patrizii, L, Popa, V, Porciani, C, Sánchez, A G, Sapone, D, Scottez, V, Sefusatti, E, Tutusaus, I, Valiviita, J, Viel, M
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creator Collaboration, Euclid
Schirmer, M
Jahnke, K
Seidel, G
Bodendorf, C
Grupp, F
Hormuth, F
Wachter, S
Barbier, R
Ganga, K
Hudelot, P
Auricchio, N
Balestra, A
Bender, R
Branchini, E
Cavuoti, S
Congedo, G
Conversi, L
Copin, Y
Courbin, F
Douspis, M
Dubath, F
Farrens, S
Garilli, B
Gillard, W
Guzzo, L
Hoekstra, H
Hornstrup, A
Kiessling, A
Kümmel, M
Kurki-Suonio, H
Laureijs, R
Ligori, S
Maiorano, E
Marggraf, O
Markovic, K
Marulli, F
Maurogordato, S
Mellier, Y
Merlin, E
Meylan, G
Nakajima, R
Nichol, R C
Niemi, S M
Padilla, C
Pasian, F
Poncet, M
Pozzetti, L
H -W Rix
Saglia, R
Scaramella, R
Schneider, P
Stanco, L
Toledo-Moreo, R
Torradeflot, F
Trifoglio, M
Valentijn, E A
Wang, Y
Weller, J
Zamorani, G
Zoubian, J
Farinelli, R
Medinaceli, E
Morisset, N
Polenta, G
Tenti, M
Balaguera-Antolínez, A
Biviano, A
Bozzo, E
Burigana, C
Cappi, A
Castignani, G
Cooray, A R
Courtois, H M
Crocce, M
Davini, S
de la Torre, S
Escartin, J A
Finelli, F
Garcia-Bellido, J
Gaztanaga, E
Hook, I M
Ilić, S
Kansal, V
Keihanen, E
McCracken, H J
Metcalf, R B
Monaco, P
Morgante, G
Nightingale, J
Patrizii, L
Popa, V
Porciani, C
Sánchez, A G
Sapone, D
Scottez, V
Sefusatti, E
Tutusaus, I
Valiviita, J
Viel, M
description Euclid will be the first space mission to survey most of the extragalactic sky in the 0.95-2.02 \(\mu\)m range, to a 5\(\sigma\) point-source median depth of 24.4 AB mag. This unique photometric data set will find wide use beyond Euclid's core science. In this paper, we present accurate computations of the Euclid Y_E, J_E and H_E passbands used by the Near-Infrared Spectrometer and Photometer (NISP), and the associated photometric system. We pay particular attention to passband variations in the field of view, accounting among others for spatially variable filter transmission, and variations of the angle of incidence on the filter substrate using optical ray tracing. The response curves' cut-on and cut-off wavelengths - and their variation in the field of view - are determined with 0.8 nm accuracy, essential for the photometric redshift accuracy required by Euclid. After computing the photometric zeropoints in the AB mag system, we present linear transformations from and to common ground-based near-infrared photometric systems, for normal stars, red and brown dwarfs, and galaxies separately. A Python tool to compute accurate magnitudes for arbitrary passbands and spectral energy distributions is provided. We discuss various factors from space weathering to material outgassing that may slowly alter Euclid's spectral response. At the absolute flux scale, the Euclid in-flight calibration program connects the NISP photometric system to Hubble Space Telescope spectrophotometric white dwarf standards; at the relative flux scale, the chromatic evolution of the response is tracked at the milli-mag level. In this way, we establish an accurate photometric system that is fully controlled throughout Euclid's lifetime.
doi_str_mv 10.48550/arxiv.2203.01650
format Article
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The NISP photometric system</title><source>arXiv.org</source><source>Free E- Journals</source><creator>Collaboration, Euclid ; Schirmer, M ; Jahnke, K ; Seidel, G ; Bodendorf, C ; Grupp, F ; Hormuth, F ; Wachter, S ; Barbier, R ; Ganga, K ; Hudelot, P ; Auricchio, N ; Balestra, A ; Bender, R ; Branchini, E ; Cavuoti, S ; Congedo, G ; Conversi, L ; Copin, Y ; Courbin, F ; Douspis, M ; Dubath, F ; Farrens, S ; Garilli, B ; Gillard, W ; Guzzo, L ; Hoekstra, H ; Hornstrup, A ; Kiessling, A ; Kümmel, M ; Kurki-Suonio, H ; Laureijs, R ; Ligori, S ; Maiorano, E ; Marggraf, O ; Markovic, K ; Marulli, F ; Maurogordato, S ; Mellier, Y ; Merlin, E ; Meylan, G ; Nakajima, R ; Nichol, R C ; Niemi, S M ; Padilla, C ; Pasian, F ; Poncet, M ; Pozzetti, L ; H -W Rix ; Saglia, R ; Scaramella, R ; Schneider, P ; Stanco, L ; Toledo-Moreo, R ; Torradeflot, F ; Trifoglio, M ; Valentijn, E A ; Wang, Y ; Weller, J ; Zamorani, G ; Zoubian, J ; Farinelli, R ; Medinaceli, E ; Morisset, N ; Polenta, G ; Tenti, M ; Balaguera-Antolínez, A ; Biviano, A ; Bozzo, E ; Burigana, C ; Cappi, A ; Castignani, G ; Cooray, A R ; Courtois, H M ; Crocce, M ; Davini, S ; de la Torre, S ; Escartin, J A ; Finelli, F ; Garcia-Bellido, J ; Gaztanaga, E ; Hook, I M ; Ilić, S ; Kansal, V ; Keihanen, E ; McCracken, H J ; Metcalf, R B ; Monaco, P ; Morgante, G ; Nightingale, J ; Patrizii, L ; Popa, V ; Porciani, C ; Sánchez, A G ; Sapone, D ; Scottez, V ; Sefusatti, E ; Tutusaus, I ; Valiviita, J ; Viel, M</creator><creatorcontrib>Collaboration, Euclid ; Schirmer, M ; Jahnke, K ; Seidel, G ; Bodendorf, C ; Grupp, F ; Hormuth, F ; Wachter, S ; Barbier, R ; Ganga, K ; Hudelot, P ; Auricchio, N ; Balestra, A ; Bender, R ; Branchini, E ; Cavuoti, S ; Congedo, G ; Conversi, L ; Copin, Y ; Courbin, F ; Douspis, M ; Dubath, F ; Farrens, S ; Garilli, B ; Gillard, W ; Guzzo, L ; Hoekstra, H ; Hornstrup, A ; Kiessling, A ; Kümmel, M ; Kurki-Suonio, H ; Laureijs, R ; Ligori, S ; Maiorano, E ; Marggraf, O ; Markovic, K ; Marulli, F ; Maurogordato, S ; Mellier, Y ; Merlin, E ; Meylan, G ; Nakajima, R ; Nichol, R C ; Niemi, S M ; Padilla, C ; Pasian, F ; Poncet, M ; Pozzetti, L ; H -W Rix ; Saglia, R ; Scaramella, R ; Schneider, P ; Stanco, L ; Toledo-Moreo, R ; Torradeflot, F ; Trifoglio, M ; Valentijn, E A ; Wang, Y ; Weller, J ; Zamorani, G ; Zoubian, J ; Farinelli, R ; Medinaceli, E ; Morisset, N ; Polenta, G ; Tenti, M ; Balaguera-Antolínez, A ; Biviano, A ; Bozzo, E ; Burigana, C ; Cappi, A ; Castignani, G ; Cooray, A R ; Courtois, H M ; Crocce, M ; Davini, S ; de la Torre, S ; Escartin, J A ; Finelli, F ; Garcia-Bellido, J ; Gaztanaga, E ; Hook, I M ; Ilić, S ; Kansal, V ; Keihanen, E ; McCracken, H J ; Metcalf, R B ; Monaco, P ; Morgante, G ; Nightingale, J ; Patrizii, L ; Popa, V ; Porciani, C ; Sánchez, A G ; Sapone, D ; Scottez, V ; Sefusatti, E ; Tutusaus, I ; Valiviita, J ; Viel, M</creatorcontrib><description>Euclid will be the first space mission to survey most of the extragalactic sky in the 0.95-2.02 \(\mu\)m range, to a 5\(\sigma\) point-source median depth of 24.4 AB mag. This unique photometric data set will find wide use beyond Euclid's core science. In this paper, we present accurate computations of the Euclid Y_E, J_E and H_E passbands used by the Near-Infrared Spectrometer and Photometer (NISP), and the associated photometric system. We pay particular attention to passband variations in the field of view, accounting among others for spatially variable filter transmission, and variations of the angle of incidence on the filter substrate using optical ray tracing. The response curves' cut-on and cut-off wavelengths - and their variation in the field of view - are determined with 0.8 nm accuracy, essential for the photometric redshift accuracy required by Euclid. After computing the photometric zeropoints in the AB mag system, we present linear transformations from and to common ground-based near-infrared photometric systems, for normal stars, red and brown dwarfs, and galaxies separately. A Python tool to compute accurate magnitudes for arbitrary passbands and spectral energy distributions is provided. We discuss various factors from space weathering to material outgassing that may slowly alter Euclid's spectral response. At the absolute flux scale, the Euclid in-flight calibration program connects the NISP photometric system to Hubble Space Telescope spectrophotometric white dwarf standards; at the relative flux scale, the chromatic evolution of the response is tracked at the milli-mag level. In this way, we establish an accurate photometric system that is fully controlled throughout Euclid's lifetime.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.2203.01650</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Field of view ; Galaxies ; Hubble Space Telescope ; Incidence angle ; Infrared photometry ; Infrared spectra ; Infrared spectrometers ; Linear transformations ; Near infrared radiation ; Outgassing ; Photometry ; Physics - Cosmology and Nongalactic Astrophysics ; Physics - Instrumentation and Methods for Astrophysics ; Point sources ; Ray tracing ; Red shift ; Sky surveys (astronomy) ; Space missions ; Space telescopes ; Spectral sensitivity ; Spectrophotometry ; Substrates ; White dwarf stars</subject><ispartof>arXiv.org, 2022-03</ispartof><rights>2022. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,776,780,881,27902</link.rule.ids><backlink>$$Uhttps://doi.org/10.1051/0004-6361/202142897$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.2203.01650$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Collaboration, Euclid</creatorcontrib><creatorcontrib>Schirmer, M</creatorcontrib><creatorcontrib>Jahnke, K</creatorcontrib><creatorcontrib>Seidel, G</creatorcontrib><creatorcontrib>Bodendorf, 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A</creatorcontrib><creatorcontrib>Kiessling, A</creatorcontrib><creatorcontrib>Kümmel, M</creatorcontrib><creatorcontrib>Kurki-Suonio, H</creatorcontrib><creatorcontrib>Laureijs, R</creatorcontrib><creatorcontrib>Ligori, S</creatorcontrib><creatorcontrib>Maiorano, E</creatorcontrib><creatorcontrib>Marggraf, O</creatorcontrib><creatorcontrib>Markovic, K</creatorcontrib><creatorcontrib>Marulli, F</creatorcontrib><creatorcontrib>Maurogordato, S</creatorcontrib><creatorcontrib>Mellier, Y</creatorcontrib><creatorcontrib>Merlin, E</creatorcontrib><creatorcontrib>Meylan, G</creatorcontrib><creatorcontrib>Nakajima, R</creatorcontrib><creatorcontrib>Nichol, R C</creatorcontrib><creatorcontrib>Niemi, S M</creatorcontrib><creatorcontrib>Padilla, C</creatorcontrib><creatorcontrib>Pasian, F</creatorcontrib><creatorcontrib>Poncet, M</creatorcontrib><creatorcontrib>Pozzetti, L</creatorcontrib><creatorcontrib>H -W Rix</creatorcontrib><creatorcontrib>Saglia, R</creatorcontrib><creatorcontrib>Scaramella, R</creatorcontrib><creatorcontrib>Schneider, P</creatorcontrib><creatorcontrib>Stanco, L</creatorcontrib><creatorcontrib>Toledo-Moreo, R</creatorcontrib><creatorcontrib>Torradeflot, F</creatorcontrib><creatorcontrib>Trifoglio, M</creatorcontrib><creatorcontrib>Valentijn, E A</creatorcontrib><creatorcontrib>Wang, Y</creatorcontrib><creatorcontrib>Weller, J</creatorcontrib><creatorcontrib>Zamorani, G</creatorcontrib><creatorcontrib>Zoubian, J</creatorcontrib><creatorcontrib>Farinelli, R</creatorcontrib><creatorcontrib>Medinaceli, E</creatorcontrib><creatorcontrib>Morisset, N</creatorcontrib><creatorcontrib>Polenta, G</creatorcontrib><creatorcontrib>Tenti, M</creatorcontrib><creatorcontrib>Balaguera-Antolínez, A</creatorcontrib><creatorcontrib>Biviano, A</creatorcontrib><creatorcontrib>Bozzo, E</creatorcontrib><creatorcontrib>Burigana, C</creatorcontrib><creatorcontrib>Cappi, A</creatorcontrib><creatorcontrib>Castignani, G</creatorcontrib><creatorcontrib>Cooray, A R</creatorcontrib><creatorcontrib>Courtois, H M</creatorcontrib><creatorcontrib>Crocce, M</creatorcontrib><creatorcontrib>Davini, S</creatorcontrib><creatorcontrib>de la Torre, S</creatorcontrib><creatorcontrib>Escartin, J A</creatorcontrib><creatorcontrib>Finelli, F</creatorcontrib><creatorcontrib>Garcia-Bellido, J</creatorcontrib><creatorcontrib>Gaztanaga, E</creatorcontrib><creatorcontrib>Hook, I M</creatorcontrib><creatorcontrib>Ilić, S</creatorcontrib><creatorcontrib>Kansal, V</creatorcontrib><creatorcontrib>Keihanen, E</creatorcontrib><creatorcontrib>McCracken, H J</creatorcontrib><creatorcontrib>Metcalf, R B</creatorcontrib><creatorcontrib>Monaco, P</creatorcontrib><creatorcontrib>Morgante, G</creatorcontrib><creatorcontrib>Nightingale, J</creatorcontrib><creatorcontrib>Patrizii, L</creatorcontrib><creatorcontrib>Popa, V</creatorcontrib><creatorcontrib>Porciani, C</creatorcontrib><creatorcontrib>Sánchez, A G</creatorcontrib><creatorcontrib>Sapone, D</creatorcontrib><creatorcontrib>Scottez, V</creatorcontrib><creatorcontrib>Sefusatti, E</creatorcontrib><creatorcontrib>Tutusaus, I</creatorcontrib><creatorcontrib>Valiviita, J</creatorcontrib><creatorcontrib>Viel, M</creatorcontrib><title>Euclid preparation. XVIII. The NISP photometric system</title><title>arXiv.org</title><description>Euclid will be the first space mission to survey most of the extragalactic sky in the 0.95-2.02 \(\mu\)m range, to a 5\(\sigma\) point-source median depth of 24.4 AB mag. This unique photometric data set will find wide use beyond Euclid's core science. In this paper, we present accurate computations of the Euclid Y_E, J_E and H_E passbands used by the Near-Infrared Spectrometer and Photometer (NISP), and the associated photometric system. We pay particular attention to passband variations in the field of view, accounting among others for spatially variable filter transmission, and variations of the angle of incidence on the filter substrate using optical ray tracing. The response curves' cut-on and cut-off wavelengths - and their variation in the field of view - are determined with 0.8 nm accuracy, essential for the photometric redshift accuracy required by Euclid. After computing the photometric zeropoints in the AB mag system, we present linear transformations from and to common ground-based near-infrared photometric systems, for normal stars, red and brown dwarfs, and galaxies separately. A Python tool to compute accurate magnitudes for arbitrary passbands and spectral energy distributions is provided. We discuss various factors from space weathering to material outgassing that may slowly alter Euclid's spectral response. At the absolute flux scale, the Euclid in-flight calibration program connects the NISP photometric system to Hubble Space Telescope spectrophotometric white dwarf standards; at the relative flux scale, the chromatic evolution of the response is tracked at the milli-mag level. In this way, we establish an accurate photometric system that is fully controlled throughout Euclid's lifetime.</description><subject>Field of view</subject><subject>Galaxies</subject><subject>Hubble Space Telescope</subject><subject>Incidence angle</subject><subject>Infrared photometry</subject><subject>Infrared spectra</subject><subject>Infrared spectrometers</subject><subject>Linear transformations</subject><subject>Near infrared radiation</subject><subject>Outgassing</subject><subject>Photometry</subject><subject>Physics - Cosmology and Nongalactic Astrophysics</subject><subject>Physics - Instrumentation and Methods for Astrophysics</subject><subject>Point sources</subject><subject>Ray tracing</subject><subject>Red shift</subject><subject>Sky surveys (astronomy)</subject><subject>Space missions</subject><subject>Space telescopes</subject><subject>Spectral sensitivity</subject><subject>Spectrophotometry</subject><subject>Substrates</subject><subject>White dwarf 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arXiv.org</general><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>L6V</scope><scope>M7S</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>GOX</scope></search><sort><creationdate>20220331</creationdate><title>Euclid preparation. XVIII. The NISP photometric system</title><author>Collaboration, Euclid ; Schirmer, M ; Jahnke, K ; Seidel, G ; Bodendorf, C ; Grupp, F ; Hormuth, F ; Wachter, S ; Barbier, R ; Ganga, K ; Hudelot, P ; Auricchio, N ; Balestra, A ; Bender, R ; Branchini, E ; Cavuoti, S ; Congedo, G ; Conversi, L ; Copin, Y ; Courbin, F ; Douspis, M ; Dubath, F ; Farrens, S ; Garilli, B ; Gillard, W ; Guzzo, L ; Hoekstra, H ; Hornstrup, A ; Kiessling, A ; Kümmel, M ; Kurki-Suonio, H ; Laureijs, R ; Ligori, S ; Maiorano, E ; Marggraf, O ; Markovic, K ; Marulli, F ; Maurogordato, S ; Mellier, Y ; Merlin, E ; Meylan, G ; Nakajima, R ; Nichol, R C ; Niemi, S M ; Padilla, C ; Pasian, F ; Poncet, M ; Pozzetti, L ; H -W Rix ; Saglia, R ; Scaramella, R ; Schneider, P ; Stanco, L ; Toledo-Moreo, R ; Torradeflot, F ; Trifoglio, M ; Valentijn, E A ; Wang, Y ; Weller, J ; Zamorani, G ; Zoubian, J ; Farinelli, R ; Medinaceli, E ; Morisset, N ; Polenta, G ; Tenti, M ; Balaguera-Antolínez, A ; Biviano, A ; Bozzo, E ; Burigana, C ; Cappi, A ; Castignani, G ; Cooray, A R ; Courtois, H M ; Crocce, M ; Davini, S ; de la Torre, S ; Escartin, J A ; Finelli, F ; Garcia-Bellido, J ; Gaztanaga, E ; Hook, I M ; Ilić, S ; Kansal, V ; Keihanen, E ; McCracken, H J ; Metcalf, R B ; Monaco, P ; Morgante, G ; Nightingale, J ; Patrizii, L ; Popa, V ; Porciani, C ; Sánchez, A G ; Sapone, D ; Scottez, V ; Sefusatti, E ; Tutusaus, I ; Valiviita, J ; Viel, M</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a527-35ca43a2674fbf80513be4e56d7fd8c67d8534dc0234497994bf491a1bcb74f03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2022</creationdate><topic>Field of view</topic><topic>Galaxies</topic><topic>Hubble Space Telescope</topic><topic>Incidence angle</topic><topic>Infrared photometry</topic><topic>Infrared spectra</topic><topic>Infrared spectrometers</topic><topic>Linear transformations</topic><topic>Near infrared radiation</topic><topic>Outgassing</topic><topic>Photometry</topic><topic>Physics - Cosmology and Nongalactic Astrophysics</topic><topic>Physics - Instrumentation and Methods for Astrophysics</topic><topic>Point sources</topic><topic>Ray tracing</topic><topic>Red shift</topic><topic>Sky surveys (astronomy)</topic><topic>Space missions</topic><topic>Space telescopes</topic><topic>Spectral sensitivity</topic><topic>Spectrophotometry</topic><topic>Substrates</topic><topic>White dwarf stars</topic><toplevel>online_resources</toplevel><creatorcontrib>Collaboration, Euclid</creatorcontrib><creatorcontrib>Schirmer, M</creatorcontrib><creatorcontrib>Jahnke, K</creatorcontrib><creatorcontrib>Seidel, G</creatorcontrib><creatorcontrib>Bodendorf, C</creatorcontrib><creatorcontrib>Grupp, F</creatorcontrib><creatorcontrib>Hormuth, F</creatorcontrib><creatorcontrib>Wachter, S</creatorcontrib><creatorcontrib>Barbier, R</creatorcontrib><creatorcontrib>Ganga, K</creatorcontrib><creatorcontrib>Hudelot, 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China</collection><collection>Engineering Collection</collection><collection>arXiv.org</collection><jtitle>arXiv.org</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Collaboration, Euclid</au><au>Schirmer, M</au><au>Jahnke, K</au><au>Seidel, G</au><au>Bodendorf, C</au><au>Grupp, F</au><au>Hormuth, F</au><au>Wachter, S</au><au>Barbier, R</au><au>Ganga, K</au><au>Hudelot, P</au><au>Auricchio, N</au><au>Balestra, A</au><au>Bender, R</au><au>Branchini, E</au><au>Cavuoti, S</au><au>Congedo, G</au><au>Conversi, L</au><au>Copin, Y</au><au>Courbin, F</au><au>Douspis, M</au><au>Dubath, F</au><au>Farrens, S</au><au>Garilli, B</au><au>Gillard, W</au><au>Guzzo, L</au><au>Hoekstra, H</au><au>Hornstrup, A</au><au>Kiessling, A</au><au>Kümmel, M</au><au>Kurki-Suonio, H</au><au>Laureijs, R</au><au>Ligori, S</au><au>Maiorano, E</au><au>Marggraf, O</au><au>Markovic, K</au><au>Marulli, F</au><au>Maurogordato, S</au><au>Mellier, Y</au><au>Merlin, E</au><au>Meylan, G</au><au>Nakajima, R</au><au>Nichol, R C</au><au>Niemi, S M</au><au>Padilla, C</au><au>Pasian, F</au><au>Poncet, M</au><au>Pozzetti, L</au><au>H -W Rix</au><au>Saglia, R</au><au>Scaramella, R</au><au>Schneider, P</au><au>Stanco, L</au><au>Toledo-Moreo, R</au><au>Torradeflot, F</au><au>Trifoglio, M</au><au>Valentijn, E A</au><au>Wang, Y</au><au>Weller, J</au><au>Zamorani, G</au><au>Zoubian, J</au><au>Farinelli, R</au><au>Medinaceli, E</au><au>Morisset, N</au><au>Polenta, G</au><au>Tenti, M</au><au>Balaguera-Antolínez, A</au><au>Biviano, A</au><au>Bozzo, E</au><au>Burigana, C</au><au>Cappi, A</au><au>Castignani, G</au><au>Cooray, A R</au><au>Courtois, H M</au><au>Crocce, M</au><au>Davini, S</au><au>de la Torre, S</au><au>Escartin, J A</au><au>Finelli, F</au><au>Garcia-Bellido, J</au><au>Gaztanaga, E</au><au>Hook, I M</au><au>Ilić, S</au><au>Kansal, V</au><au>Keihanen, E</au><au>McCracken, H J</au><au>Metcalf, R B</au><au>Monaco, P</au><au>Morgante, G</au><au>Nightingale, J</au><au>Patrizii, L</au><au>Popa, V</au><au>Porciani, C</au><au>Sánchez, A G</au><au>Sapone, D</au><au>Scottez, V</au><au>Sefusatti, E</au><au>Tutusaus, I</au><au>Valiviita, J</au><au>Viel, M</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Euclid preparation. XVIII. The NISP photometric system</atitle><jtitle>arXiv.org</jtitle><date>2022-03-31</date><risdate>2022</risdate><eissn>2331-8422</eissn><abstract>Euclid will be the first space mission to survey most of the extragalactic sky in the 0.95-2.02 \(\mu\)m range, to a 5\(\sigma\) point-source median depth of 24.4 AB mag. This unique photometric data set will find wide use beyond Euclid's core science. In this paper, we present accurate computations of the Euclid Y_E, J_E and H_E passbands used by the Near-Infrared Spectrometer and Photometer (NISP), and the associated photometric system. We pay particular attention to passband variations in the field of view, accounting among others for spatially variable filter transmission, and variations of the angle of incidence on the filter substrate using optical ray tracing. The response curves' cut-on and cut-off wavelengths - and their variation in the field of view - are determined with 0.8 nm accuracy, essential for the photometric redshift accuracy required by Euclid. After computing the photometric zeropoints in the AB mag system, we present linear transformations from and to common ground-based near-infrared photometric systems, for normal stars, red and brown dwarfs, and galaxies separately. A Python tool to compute accurate magnitudes for arbitrary passbands and spectral energy distributions is provided. We discuss various factors from space weathering to material outgassing that may slowly alter Euclid's spectral response. At the absolute flux scale, the Euclid in-flight calibration program connects the NISP photometric system to Hubble Space Telescope spectrophotometric white dwarf standards; at the relative flux scale, the chromatic evolution of the response is tracked at the milli-mag level. In this way, we establish an accurate photometric system that is fully controlled throughout Euclid's lifetime.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.2203.01650</doi><oa>free_for_read</oa></addata></record>
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subjects Field of view
Galaxies
Hubble Space Telescope
Incidence angle
Infrared photometry
Infrared spectra
Infrared spectrometers
Linear transformations
Near infrared radiation
Outgassing
Photometry
Physics - Cosmology and Nongalactic Astrophysics
Physics - Instrumentation and Methods for Astrophysics
Point sources
Ray tracing
Red shift
Sky surveys (astronomy)
Space missions
Space telescopes
Spectral sensitivity
Spectrophotometry
Substrates
White dwarf stars
title Euclid preparation. XVIII. The NISP photometric system
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