QUBIC: The QU Bolometric Interferometer for Cosmology
One of the major challenges of modern cosmology is the detection of B-mode polarization anisotropies in the CMB. These originate from tensor fluctuations of the metric produced during the inflationary phase. Their detection would therefore constitute a major step towards understanding the primordial...
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creator | The QUBIC collaboration Battistelli, E Baù, A Bennett, D Bergé, L -Ph Bernard, J de Bernardis, P Bounab, A Bréelle, É Bunn, E F Calvo, M Charlassier, R Collin, S Cruciani, A Curran, G Dumoulin, L Gault, A Gervasi, M Ghribi, A Giard, M Giordano, C Giraud-Héraud, Y Gradziel, M Guglielmi, L J -Ch Hamilton Haynes, V Kaplan, J Korotkov, A Landé, J Maffei, B Maiello, M Malu, S Marnieros, S Masi, S Murphy, A Nati, F O'Sullivan, C Pajot, F Passerini, A Peterzen, S Piacentini, F Piat, M Piccirillo, L Pisano, G Polenta, G Prêle, D Romano, D Rosset, C Salatino, M Schillacci, A Sironi, G Sordini, R Spinelli, S Tartari, A Timbie, P Tucker, G Vibert, L Voisin, F Watson, R A Zannoni, M |
description | One of the major challenges of modern cosmology is the detection of B-mode polarization anisotropies in the CMB. These originate from tensor fluctuations of the metric produced during the inflationary phase. Their detection would therefore constitute a major step towards understanding the primordial Universe. The expected level of these anisotropies is however so small that it requires a new generation of instruments with high sensitivity and extremely good control of systematic effects. We propose the QUBIC instrument based on the novel concept of bolometric interferometry, bringing together the sensitivity advantages of bolometric detectors with the systematics effects advantages of interferometry. Methods: The instrument will directly observe the sky through an array of entry horns whose signals will be combined together using an optical combiner. The whole set-up is located inside a cryostat. Polarization modulation will be achieved using a rotating half-wave plate and interference fringes will be imaged on two focal planes (separated by a polarizing grid) tiled with bolometers. We show that QUBIC can be considered as a synthetic imager, exactly similar to a usual imager but with a synthesized beam formed by the array of entry horns. Scanning the sky provides an additional modulation of the signal and improve the sky coverage shape. The usual techniques of map-making and power spectrum estimation can then be applied. We show that the sensitivity of such an instrument is comparable with that of an imager with the same number of horns. We anticipate a low level of beam-related systematics thanks to the fact that the synthesized beam is determined by the location of the primary horns. Other systematics should be under good control thanks to an autocalibration technique, specific to our concept, that will permit the accurate determination of most of the systematics parameters. |
doi_str_mv | 10.48550/arxiv.1010.0645 |
format | Article |
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These originate from tensor fluctuations of the metric produced during the inflationary phase. Their detection would therefore constitute a major step towards understanding the primordial Universe. The expected level of these anisotropies is however so small that it requires a new generation of instruments with high sensitivity and extremely good control of systematic effects. We propose the QUBIC instrument based on the novel concept of bolometric interferometry, bringing together the sensitivity advantages of bolometric detectors with the systematics effects advantages of interferometry. Methods: The instrument will directly observe the sky through an array of entry horns whose signals will be combined together using an optical combiner. The whole set-up is located inside a cryostat. Polarization modulation will be achieved using a rotating half-wave plate and interference fringes will be imaged on two focal planes (separated by a polarizing grid) tiled with bolometers. We show that QUBIC can be considered as a synthetic imager, exactly similar to a usual imager but with a synthesized beam formed by the array of entry horns. Scanning the sky provides an additional modulation of the signal and improve the sky coverage shape. The usual techniques of map-making and power spectrum estimation can then be applied. We show that the sensitivity of such an instrument is comparable with that of an imager with the same number of horns. We anticipate a low level of beam-related systematics thanks to the fact that the synthesized beam is determined by the location of the primary horns. Other systematics should be under good control thanks to an autocalibration technique, specific to our concept, that will permit the accurate determination of most of the systematics parameters.</description><identifier>EISSN: 2331-8422</identifier><identifier>DOI: 10.48550/arxiv.1010.0645</identifier><language>eng</language><publisher>Ithaca: Cornell University Library, arXiv.org</publisher><subject>Anisotropy ; Beamforming ; Bolometers ; Control equipment ; Cosmology ; Horns ; Interference fringes ; Interferometry ; Low level ; Physics - Instrumentation and Methods for Astrophysics ; Polarization modulation ; Sensitivity ; Synthesis ; Tensors ; Universe ; Variations ; Wave plates</subject><ispartof>arXiv.org, 2010-10</ispartof><rights>2010. This work is published under http://arxiv.org/licenses/nonexclusive-distrib/1.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</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/10.48550/arXiv.1010.0645$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1016/j.astropartphys.2011.01.012$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>The QUBIC collaboration</creatorcontrib><creatorcontrib>Battistelli, E</creatorcontrib><creatorcontrib>Baù, A</creatorcontrib><creatorcontrib>Bennett, D</creatorcontrib><creatorcontrib>Bergé, L</creatorcontrib><creatorcontrib>-Ph Bernard, J</creatorcontrib><creatorcontrib>de Bernardis, P</creatorcontrib><creatorcontrib>Bounab, A</creatorcontrib><creatorcontrib>Bréelle, É</creatorcontrib><creatorcontrib>Bunn, E F</creatorcontrib><creatorcontrib>Calvo, M</creatorcontrib><creatorcontrib>Charlassier, R</creatorcontrib><creatorcontrib>Collin, S</creatorcontrib><creatorcontrib>Cruciani, A</creatorcontrib><creatorcontrib>Curran, G</creatorcontrib><creatorcontrib>Dumoulin, L</creatorcontrib><creatorcontrib>Gault, A</creatorcontrib><creatorcontrib>Gervasi, M</creatorcontrib><creatorcontrib>Ghribi, A</creatorcontrib><creatorcontrib>Giard, M</creatorcontrib><creatorcontrib>Giordano, C</creatorcontrib><creatorcontrib>Giraud-Héraud, Y</creatorcontrib><creatorcontrib>Gradziel, M</creatorcontrib><creatorcontrib>Guglielmi, L</creatorcontrib><creatorcontrib>J -Ch Hamilton</creatorcontrib><creatorcontrib>Haynes, V</creatorcontrib><creatorcontrib>Kaplan, J</creatorcontrib><creatorcontrib>Korotkov, A</creatorcontrib><creatorcontrib>Landé, J</creatorcontrib><creatorcontrib>Maffei, B</creatorcontrib><creatorcontrib>Maiello, M</creatorcontrib><creatorcontrib>Malu, S</creatorcontrib><creatorcontrib>Marnieros, S</creatorcontrib><creatorcontrib>Masi, S</creatorcontrib><creatorcontrib>Murphy, A</creatorcontrib><creatorcontrib>Nati, F</creatorcontrib><creatorcontrib>O'Sullivan, C</creatorcontrib><creatorcontrib>Pajot, F</creatorcontrib><creatorcontrib>Passerini, A</creatorcontrib><creatorcontrib>Peterzen, S</creatorcontrib><creatorcontrib>Piacentini, F</creatorcontrib><creatorcontrib>Piat, M</creatorcontrib><creatorcontrib>Piccirillo, L</creatorcontrib><creatorcontrib>Pisano, G</creatorcontrib><creatorcontrib>Polenta, G</creatorcontrib><creatorcontrib>Prêle, D</creatorcontrib><creatorcontrib>Romano, D</creatorcontrib><creatorcontrib>Rosset, C</creatorcontrib><creatorcontrib>Salatino, M</creatorcontrib><creatorcontrib>Schillacci, A</creatorcontrib><creatorcontrib>Sironi, G</creatorcontrib><creatorcontrib>Sordini, R</creatorcontrib><creatorcontrib>Spinelli, S</creatorcontrib><creatorcontrib>Tartari, A</creatorcontrib><creatorcontrib>Timbie, P</creatorcontrib><creatorcontrib>Tucker, G</creatorcontrib><creatorcontrib>Vibert, L</creatorcontrib><creatorcontrib>Voisin, F</creatorcontrib><creatorcontrib>Watson, R A</creatorcontrib><creatorcontrib>Zannoni, M</creatorcontrib><title>QUBIC: The QU Bolometric Interferometer for Cosmology</title><title>arXiv.org</title><description>One of the major challenges of modern cosmology is the detection of B-mode polarization anisotropies in the CMB. These originate from tensor fluctuations of the metric produced during the inflationary phase. Their detection would therefore constitute a major step towards understanding the primordial Universe. The expected level of these anisotropies is however so small that it requires a new generation of instruments with high sensitivity and extremely good control of systematic effects. We propose the QUBIC instrument based on the novel concept of bolometric interferometry, bringing together the sensitivity advantages of bolometric detectors with the systematics effects advantages of interferometry. Methods: The instrument will directly observe the sky through an array of entry horns whose signals will be combined together using an optical combiner. The whole set-up is located inside a cryostat. Polarization modulation will be achieved using a rotating half-wave plate and interference fringes will be imaged on two focal planes (separated by a polarizing grid) tiled with bolometers. We show that QUBIC can be considered as a synthetic imager, exactly similar to a usual imager but with a synthesized beam formed by the array of entry horns. Scanning the sky provides an additional modulation of the signal and improve the sky coverage shape. The usual techniques of map-making and power spectrum estimation can then be applied. We show that the sensitivity of such an instrument is comparable with that of an imager with the same number of horns. We anticipate a low level of beam-related systematics thanks to the fact that the synthesized beam is determined by the location of the primary horns. Other systematics should be under good control thanks to an autocalibration technique, specific to our concept, that will permit the accurate determination of most of the systematics parameters.</description><subject>Anisotropy</subject><subject>Beamforming</subject><subject>Bolometers</subject><subject>Control equipment</subject><subject>Cosmology</subject><subject>Horns</subject><subject>Interference fringes</subject><subject>Interferometry</subject><subject>Low level</subject><subject>Physics - Instrumentation and Methods for Astrophysics</subject><subject>Polarization modulation</subject><subject>Sensitivity</subject><subject>Synthesis</subject><subject>Tensors</subject><subject>Universe</subject><subject>Variations</subject><subject>Wave plates</subject><issn>2331-8422</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><sourceid>BENPR</sourceid><sourceid>GOX</sourceid><recordid>eNotj01Lw0AQhhdBsNTePcmC59TZ2Y_serNBa6AghfQc8rGrKU23blqx_96N9TTM8LzD-xByx2AutJTwWIWf7nvOIB5ACXlFJsg5S7RAvCGzYdgCAKoUpeQTItebRZ490eLT0vWGLvzO9_YYuobm-6MNzoZxt4E6H2jmhz4CH-dbcu2q3WBn_3NKiteXIntLVu_LPHteJZVkPLFoFEOu20aq2jjbtNAw5ZhshFRoWpNyl4rWpdaI2EgB6ro2RvIWtIWYnJL7y9s_pfIQur4K53JUK0e1CDxcgEPwXyc7HMutP4V9rFQiaBRoUHP-Cws0ToM</recordid><startdate>20101004</startdate><enddate>20101004</enddate><creator>The QUBIC collaboration</creator><creator>Battistelli, E</creator><creator>Baù, A</creator><creator>Bennett, D</creator><creator>Bergé, L</creator><creator>-Ph Bernard, J</creator><creator>de Bernardis, P</creator><creator>Bounab, A</creator><creator>Bréelle, É</creator><creator>Bunn, E F</creator><creator>Calvo, M</creator><creator>Charlassier, R</creator><creator>Collin, 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Cosmology</atitle><jtitle>arXiv.org</jtitle><date>2010-10-04</date><risdate>2010</risdate><eissn>2331-8422</eissn><abstract>One of the major challenges of modern cosmology is the detection of B-mode polarization anisotropies in the CMB. These originate from tensor fluctuations of the metric produced during the inflationary phase. Their detection would therefore constitute a major step towards understanding the primordial Universe. The expected level of these anisotropies is however so small that it requires a new generation of instruments with high sensitivity and extremely good control of systematic effects. We propose the QUBIC instrument based on the novel concept of bolometric interferometry, bringing together the sensitivity advantages of bolometric detectors with the systematics effects advantages of interferometry. Methods: The instrument will directly observe the sky through an array of entry horns whose signals will be combined together using an optical combiner. The whole set-up is located inside a cryostat. Polarization modulation will be achieved using a rotating half-wave plate and interference fringes will be imaged on two focal planes (separated by a polarizing grid) tiled with bolometers. We show that QUBIC can be considered as a synthetic imager, exactly similar to a usual imager but with a synthesized beam formed by the array of entry horns. Scanning the sky provides an additional modulation of the signal and improve the sky coverage shape. The usual techniques of map-making and power spectrum estimation can then be applied. We show that the sensitivity of such an instrument is comparable with that of an imager with the same number of horns. We anticipate a low level of beam-related systematics thanks to the fact that the synthesized beam is determined by the location of the primary horns. Other systematics should be under good control thanks to an autocalibration technique, specific to our concept, that will permit the accurate determination of most of the systematics parameters.</abstract><cop>Ithaca</cop><pub>Cornell University Library, arXiv.org</pub><doi>10.48550/arxiv.1010.0645</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext |
identifier | EISSN: 2331-8422 |
ispartof | arXiv.org, 2010-10 |
issn | 2331-8422 |
language | eng |
recordid | cdi_arxiv_primary_1010_0645 |
source | arXiv.org; Free E- Journals |
subjects | Anisotropy Beamforming Bolometers Control equipment Cosmology Horns Interference fringes Interferometry Low level Physics - Instrumentation and Methods for Astrophysics Polarization modulation Sensitivity Synthesis Tensors Universe Variations Wave plates |
title | QUBIC: The QU Bolometric Interferometer for Cosmology |
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