Thermal Architecture For The Qubic Cryogenic Receiver

A. J. May,C. Chapron,G. Coppi,G. D'Alessandro,P. de Bernardis,S. Masi,S. Melhuish,M. Piat,L. Piccirillo,A. Schillaci, J.-P. Thermeau, P. Ade,G. Amico,D. Auguste,J. Aumont, S. Banfi, G. Barbarán,P. Battaglia,E. Battistelli,A. Baù, B. Bélier,D. Bennett, L. Bergé,J.-Ph. Bernard,M. Bersanelli,M.-A. Bigot-Sazy,N. Bleurvacq,J. Bonaparte,J. Bonis, G. Bordier, E. Bréelle, E. Bunn,D. Burke, D. Buzi, A. Buzzelli,F. Cavaliere, P. Chanial,R. Charlassier,F. Columbro,A. Coppolecchia,F. Couchot,R. D'Agostino,G. De Gasperis,M. De Leo,M. De Petris,A. Di Donato,L. Dumoulin, A. Etchegoyen,A. Fasciszewski,C. Franceschet,M. M. Gamboa Lerena,B. García,X. Garrido,M. Gaspard,A. Gault,D. Gayer,M. Gervasi,M. Giard, Y. Giraud-Héraud,M. Gómez Berisso, M. González,M. Gradziel,L. Grandsire, E. Guerrard,J.-Ch. Hamilton,D. Harari,V. Haynes,S. Henrot-Versillé,D. T. Hoang,F. Incardona,E. Jules,J. Kaplan,A. Korotkov,C. Kristukat,L. Lamagna, S. Loucatos,T. Louis,A. Lowitz, V. Lukovic,R. Luterstein,B. Maffei,S. Marnieros,A. Mattei, M. A. McCulloch,M. C. Medina,L. Mele,A. Mennella,L. Montier,L. M. Mundo,J. A. Murphy,J. D. Murphy,C. O'Sullivan,E. Olivieri,A. Paiella, F. Pajot,A. Passerini,H. Pastoriza,A. Pelosi,C. Perbost,O. Perdereau,F. Pezzotta,F. Piacentini,G. Pisano,G. Polenta,D. Prêle,R. Puddu,D. Rambaud,P. Ringegni, G. E. Romero,M. Salatino,C. G. Scóccola,S. Scully,S. Spinelli,M. Stolpovskiy,F. Suarez,A. Tartari, P. Timbie,S. A. Torchinsky,M. Tristram, V. Truongcanh,C. Tucker,G. Tucker, S. Vanneste, D. Viganó,N. Vittorio, F. Voisin,B. Watson, F. Wicek,M. Zannoni,A. Zullo

MILLIMETER, SUBMILLIMETER, AND FAR-INFRARED DETECTORS AND INSTRUMENTATION FOR ASTRONOMY IX(2018)

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摘要
QUBIC, the QU Bolometric Interferometer for Cosmology, is a novel forthcoming instrument to measure the B-mode polarization anisotropy of the Cosmic Microwave Background. The detection of the B-mode signal will be extremely challenging; QUBIC has been designed to address this with a novel approach, namely bolometric interferometry. The receiver cryostat is exceptionally large and cools complex optical and detector stages to 40 K, 4 K, 1 K and 350 mK using two pulse tube coolers, a novel He-4 sorption cooler and a double-stage He-3/He-4 sorption cooler. We discuss the thermal and mechanical design of the cryostat, modelling and thermal analysis, and laboratory cryogenic testing.
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QUBIC, experimental cosmology, bolometric interferometry, cryogenics, sorption cooler, heat switch
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