Published June 2022 | Version Published + Accepted Version
Journal Article Open

Euclid preparation. XVIII. The NISP photometric system

Creators

Abstract

Euclid will be the first space mission to survey most of the extragalactic sky in the 0.95–2.02 µm range, to a 5 σ point-source median depth of 24.4 AB mag. This unique photometric dataset 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 for, among other factors, spatially variable filter transmission and variations in 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 zero points 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.

Additional Information

© Euclid Collaboration 2022. Open Access article, published by EDP Sciences, under the terms of the Creative Commons Attribution License (https://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Open Access funding provided by Max Planck Society. Received: 13 December 2021 Accepted: 31 March 2022. The Euclid Consortium acknowledges the European Space Agency and a number of agencies and institutes that have supported the development of Euclid, in particular the Academy of Finland, the Agenzia Spaziale Italiana, the Belgian Science Policy, the Canadian Euclid Consortium, the French Centre National d'Etudes Spatiales, the Deutsches Zentrum für Luft- und Raumfahrt, the Danish Space Research Institute, the Fundação para a Ciência e a Tecnologia, the Ministerio de Economia y Competitividad, the National Aeronautics and Space Administration, the National Astronomical Observatory of Japan, the Netherlandse Onderzoekschool Voor Astronomie, the Norwegian Space Agency, the Romanian Space Agency, the State Secretariat for Education, Research and Innovation (SERI) at the Swiss Space Office (SSO), and the United Kingdom Space Agency. A complete and detailed list is available on the Euclid web site (http://www.euclid-ec.org). The first group of authors (up to and including M. Weiler) worked directly on this paper. The other authors made substantial, multi-year contributions totheEuclid project that enabled this paper in the first place. The authors at MPIA acknowledge funding by the German Space Agency DLR under grant numbers 50 OR 1202 and 50 QE 2003. The work by J.M. Carrasco and M. Weiler was (partially) funded by the Spanish MICIN/AEI/10.13039/501100011033 and by "ERDF A way of making Europe" by the European Union through grant RTI2018-095076-B-C21, and the Institute of Cosmos Sciences University of Barcelona (ICCUB, Unidad de Excelencia "Maria de Maeztu") through grant CEX2019-000918-M. The authors thank Thomas Weber (OBJ; now Materion Balzers Optics) for the technical support with the transmission measurements of the NISP filter substrates, and the anonymous referee for their useful comments. The plots in this publication were prepared with TOPCAT (Taylor 2005) and Matplotlib (Hunter 2007).

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Accepted Version - 2203.01650.pdf

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Additional details

Identifiers

Eprint ID
115738
Resolver ID
CaltechAUTHORS:20220721-8585000

Related works

Funding

Deutsches Zentrum für Luft- und Raumfahrt (DLR)
50 OR 1202
Deutsches Zentrum für Luft- und Raumfahrt (DLR)
50 QE 2003
Ministerio de Economía, Industria y Competitividad (MINECO)
10.13039/501100011033
Ministerio de Economía, Industria y Competitividad (MINECO)
RTI2018-095076-B-C21
Severo Ochoa
CEX2019-000918-M
European Space Agency (ESA)
Academy of Finland
Agenzia Spaziale Italiana (ASI)
Belgian Federal Science Policy Office (BELSPO)
Canadian Euclid Consortium
Centre National d'Études Spatiales (CNES)
Danish Space Research Institute
Fundação para a Ciência e a Tecnologia (FCT)
NASA
National Astronomical Observatory of Japan
Nederlandse Onderzoekschool voor de Astronomie (NOVA)
Norwegian Space Agency
Romanian Space Agency
Swiss Space Office (SSO)
United Kingdom Space Agency (UKSA)
Max Planck Society

Dates

Created
2022-07-26
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Updated
2022-07-26
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