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Microwave background temperature at a redshift of 6.34 from H(2)O absorption

Distortions of the observed cosmic microwave background provide a direct measurement of the microwave background temperature at redshifts from 0 to 1 (refs. (1,2)). Some additional background temperature estimates exist at redshifts from 1.8 to 3.3 based on molecular and atomic line-excitation tempe...

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Autores principales: Riechers, Dominik A., Weiss, Axel, Walter, Fabian, Carilli, Christopher L., Cox, Pierre, Decarli, Roberto, Neri, Roberto
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8810383/
https://www.ncbi.nlm.nih.gov/pubmed/35110755
http://dx.doi.org/10.1038/s41586-021-04294-5
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author Riechers, Dominik A.
Weiss, Axel
Walter, Fabian
Carilli, Christopher L.
Cox, Pierre
Decarli, Roberto
Neri, Roberto
author_facet Riechers, Dominik A.
Weiss, Axel
Walter, Fabian
Carilli, Christopher L.
Cox, Pierre
Decarli, Roberto
Neri, Roberto
author_sort Riechers, Dominik A.
collection PubMed
description Distortions of the observed cosmic microwave background provide a direct measurement of the microwave background temperature at redshifts from 0 to 1 (refs. (1,2)). Some additional background temperature estimates exist at redshifts from 1.8 to 3.3 based on molecular and atomic line-excitation temperatures in quasar absorption-line systems, but are model dependent(3). No deviations from the expected (1 + z) scaling behaviour of the microwave background temperature have been seen(4), but the measurements have not extended deeply into the matter-dominated era of the Universe at redshifts z > 3.3. Here we report observations of submillimetre line absorption from the water molecule against the cosmic microwave background at z = 6.34 in a massive starburst galaxy, corresponding to a lookback time of 12.8 billion years (ref. (5)). Radiative pumping of the upper level of the ground-state ortho-H(2)O(1(10)–1(01)) line due to starburst activity in the dusty galaxy HFLS3 results in a cooling to below the redshifted microwave background temperature, after the transition is initially excited by the microwave background. This implies a microwave background temperature of 16.4–30.2 K (1σ range) at z = 6.34, which is consistent with a background temperature increase with redshift as expected from the standard ΛCDM cosmology(4).
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spelling pubmed-88103832022-02-09 Microwave background temperature at a redshift of 6.34 from H(2)O absorption Riechers, Dominik A. Weiss, Axel Walter, Fabian Carilli, Christopher L. Cox, Pierre Decarli, Roberto Neri, Roberto Nature Article Distortions of the observed cosmic microwave background provide a direct measurement of the microwave background temperature at redshifts from 0 to 1 (refs. (1,2)). Some additional background temperature estimates exist at redshifts from 1.8 to 3.3 based on molecular and atomic line-excitation temperatures in quasar absorption-line systems, but are model dependent(3). No deviations from the expected (1 + z) scaling behaviour of the microwave background temperature have been seen(4), but the measurements have not extended deeply into the matter-dominated era of the Universe at redshifts z > 3.3. Here we report observations of submillimetre line absorption from the water molecule against the cosmic microwave background at z = 6.34 in a massive starburst galaxy, corresponding to a lookback time of 12.8 billion years (ref. (5)). Radiative pumping of the upper level of the ground-state ortho-H(2)O(1(10)–1(01)) line due to starburst activity in the dusty galaxy HFLS3 results in a cooling to below the redshifted microwave background temperature, after the transition is initially excited by the microwave background. This implies a microwave background temperature of 16.4–30.2 K (1σ range) at z = 6.34, which is consistent with a background temperature increase with redshift as expected from the standard ΛCDM cosmology(4). Nature Publishing Group UK 2022-02-02 2022 /pmc/articles/PMC8810383/ /pubmed/35110755 http://dx.doi.org/10.1038/s41586-021-04294-5 Text en © The Author(s) 2022 https://creativecommons.org/licenses/by/4.0/Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/ (https://creativecommons.org/licenses/by/4.0/) .
spellingShingle Article
Riechers, Dominik A.
Weiss, Axel
Walter, Fabian
Carilli, Christopher L.
Cox, Pierre
Decarli, Roberto
Neri, Roberto
Microwave background temperature at a redshift of 6.34 from H(2)O absorption
title Microwave background temperature at a redshift of 6.34 from H(2)O absorption
title_full Microwave background temperature at a redshift of 6.34 from H(2)O absorption
title_fullStr Microwave background temperature at a redshift of 6.34 from H(2)O absorption
title_full_unstemmed Microwave background temperature at a redshift of 6.34 from H(2)O absorption
title_short Microwave background temperature at a redshift of 6.34 from H(2)O absorption
title_sort microwave background temperature at a redshift of 6.34 from h(2)o absorption
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8810383/
https://www.ncbi.nlm.nih.gov/pubmed/35110755
http://dx.doi.org/10.1038/s41586-021-04294-5
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