The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects
Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the...
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Gespeichert in:
| Autor*in: |
E. Armengaud [verfasserIn] C. Augier [verfasserIn] A. S. Barabash [verfasserIn] F. Bellini [verfasserIn] G. Benato [verfasserIn] A. Benoît [verfasserIn] M. Beretta [verfasserIn] L. Bergé [verfasserIn] J. Billard [verfasserIn] Yu. A. Borovlev [verfasserIn] Ch. Bourgeois [verfasserIn] M. Briere [verfasserIn] V. B. Brudanin [verfasserIn] P. Camus [verfasserIn] L. Cardani [verfasserIn] N. Casali [verfasserIn] A. Cazes [verfasserIn] M. Chapellier [verfasserIn] F. Charlieux [verfasserIn] M. de Combarieu [verfasserIn] I. Dafinei [verfasserIn] F. A. Danevich [verfasserIn] M. De Jesus [verfasserIn] L. Dumoulin [verfasserIn] K. Eitel [verfasserIn] E. Elkhoury [verfasserIn] F. Ferri [verfasserIn] B. K. Fujikawa [verfasserIn] J. Gascon [verfasserIn] L. Gironi [verfasserIn] A. Giuliani [verfasserIn] V. D. Grigorieva [verfasserIn] M. Gros [verfasserIn] E. Guerard [verfasserIn] D. L. Helis [verfasserIn] H. Z. Huang [verfasserIn] R. Huang [verfasserIn] J. Johnston [verfasserIn] A. Juillard [verfasserIn] H. Khalife [verfasserIn] M. Kleifges [verfasserIn] V. V. Kobychev [verfasserIn] Yu. G. Kolomensky [verfasserIn] S. I. Konovalov [verfasserIn] A. Leder [verfasserIn] P. Loaiza [verfasserIn] L. Ma [verfasserIn] E. P. Makarov [verfasserIn] P. de Marcillac [verfasserIn] L. Marini [verfasserIn] S. Marnieros [verfasserIn] D. Misiak [verfasserIn] X. -F. Navick [verfasserIn] C. Nones [verfasserIn] V. Novati [verfasserIn] E. Olivieri [verfasserIn] J. L. Ouellet [verfasserIn] L. Pagnanini [verfasserIn] P. Pari [verfasserIn] L. Pattavina [verfasserIn] B. Paul [verfasserIn] M. Pavan [verfasserIn] H. Peng [verfasserIn] G. Pessina [verfasserIn] S. Pirro [verfasserIn] D. V. Poda [verfasserIn] O. G. Polischuk [verfasserIn] E. Previtali [verfasserIn] Th. Redon [verfasserIn] S. Rozov [verfasserIn] C. Rusconi [verfasserIn] V. Sanglard [verfasserIn] K. Schäffner [verfasserIn] B. Schmidt [verfasserIn] Y. Shen [verfasserIn] V. N. Shlegel [verfasserIn] B. Siebenborn [verfasserIn] V. Singh [verfasserIn] S. Sorbino [verfasserIn] C. Tomei [verfasserIn] V. I. Tretyak [verfasserIn] V. I. Umatov [verfasserIn] L. Vagneron [verfasserIn] M. Velázquez [verfasserIn] M. Weber [verfasserIn] B. Welliver [verfasserIn] L. Winslow [verfasserIn] M. Xue [verfasserIn] E. Yakushev [verfasserIn] A. S. Zolotarova [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2020 |
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| Übergeordnetes Werk: |
In: European Physical Journal C: Particles and Fields - SpringerOpen, 2017, 80(2020), 1, Seite 15 |
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| Übergeordnetes Werk: |
volume:80 ; year:2020 ; number:1 ; pages:15 |
| Links: |
Link aufrufen |
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| DOI / URN: |
10.1140/epjc/s10052-019-7578-6 |
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| Katalog-ID: |
DOAJ056032013 |
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| 245 | 1 | 4 | |a The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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| 520 | |a Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. | ||
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| 653 | 0 | |a Nuclear and particle physics. Atomic energy. Radioactivity | |
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10.1140/epjc/s10052-019-7578-6 doi (DE-627)DOAJ056032013 (DE-599)DOAJ885ed12ff85b43d48cb17b3b97e342a2 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Armengaud verfasserin aut The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity C. Augier verfasserin aut A. S. Barabash verfasserin aut F. Bellini verfasserin aut G. Benato verfasserin aut A. Benoît verfasserin aut M. Beretta verfasserin aut L. Bergé verfasserin aut J. Billard verfasserin aut Yu. A. Borovlev verfasserin aut Ch. Bourgeois verfasserin aut M. Briere verfasserin aut V. B. Brudanin verfasserin aut P. Camus verfasserin aut L. Cardani verfasserin aut N. Casali verfasserin aut A. Cazes verfasserin aut M. Chapellier verfasserin aut F. Charlieux verfasserin aut M. de Combarieu verfasserin aut I. Dafinei verfasserin aut F. A. Danevich verfasserin aut M. De Jesus verfasserin aut L. Dumoulin verfasserin aut K. Eitel verfasserin aut E. Elkhoury verfasserin aut F. Ferri verfasserin aut B. K. Fujikawa verfasserin aut J. Gascon verfasserin aut L. Gironi verfasserin aut A. Giuliani verfasserin aut V. D. Grigorieva verfasserin aut M. Gros verfasserin aut E. Guerard verfasserin aut D. L. Helis verfasserin aut H. Z. Huang verfasserin aut R. Huang verfasserin aut J. Johnston verfasserin aut A. Juillard verfasserin aut H. Khalife verfasserin aut M. Kleifges verfasserin aut V. V. Kobychev verfasserin aut Yu. G. Kolomensky verfasserin aut S. I. Konovalov verfasserin aut A. Leder verfasserin aut P. Loaiza verfasserin aut L. Ma verfasserin aut E. P. Makarov verfasserin aut P. de Marcillac verfasserin aut L. Marini verfasserin aut S. Marnieros verfasserin aut D. Misiak verfasserin aut X. -F. Navick verfasserin aut C. Nones verfasserin aut V. Novati verfasserin aut E. Olivieri verfasserin aut J. L. Ouellet verfasserin aut L. Pagnanini verfasserin aut P. Pari verfasserin aut L. Pattavina verfasserin aut B. Paul verfasserin aut M. Pavan verfasserin aut H. Peng verfasserin aut G. Pessina verfasserin aut S. Pirro verfasserin aut D. V. Poda verfasserin aut O. G. Polischuk verfasserin aut E. Previtali verfasserin aut Th. Redon verfasserin aut S. Rozov verfasserin aut C. Rusconi verfasserin aut V. Sanglard verfasserin aut K. Schäffner verfasserin aut B. Schmidt verfasserin aut Y. Shen verfasserin aut V. N. Shlegel verfasserin aut B. Siebenborn verfasserin aut V. Singh verfasserin aut S. Sorbino verfasserin aut C. Tomei verfasserin aut V. I. Tretyak verfasserin aut V. I. Umatov verfasserin aut L. Vagneron verfasserin aut M. Velázquez verfasserin aut M. Weber verfasserin aut B. Welliver verfasserin aut L. Winslow verfasserin aut M. Xue verfasserin aut E. Yakushev verfasserin aut A. S. Zolotarova verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 1, Seite 15 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:1 pages:15 https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/article/885ed12ff85b43d48cb17b3b97e342a2 kostenfrei https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 1 15 |
| spelling |
10.1140/epjc/s10052-019-7578-6 doi (DE-627)DOAJ056032013 (DE-599)DOAJ885ed12ff85b43d48cb17b3b97e342a2 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Armengaud verfasserin aut The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity C. Augier verfasserin aut A. S. Barabash verfasserin aut F. Bellini verfasserin aut G. Benato verfasserin aut A. Benoît verfasserin aut M. Beretta verfasserin aut L. Bergé verfasserin aut J. Billard verfasserin aut Yu. A. Borovlev verfasserin aut Ch. Bourgeois verfasserin aut M. Briere verfasserin aut V. B. Brudanin verfasserin aut P. Camus verfasserin aut L. Cardani verfasserin aut N. Casali verfasserin aut A. Cazes verfasserin aut M. Chapellier verfasserin aut F. Charlieux verfasserin aut M. de Combarieu verfasserin aut I. Dafinei verfasserin aut F. A. Danevich verfasserin aut M. De Jesus verfasserin aut L. Dumoulin verfasserin aut K. Eitel verfasserin aut E. Elkhoury verfasserin aut F. Ferri verfasserin aut B. K. Fujikawa verfasserin aut J. Gascon verfasserin aut L. Gironi verfasserin aut A. Giuliani verfasserin aut V. D. Grigorieva verfasserin aut M. Gros verfasserin aut E. Guerard verfasserin aut D. L. Helis verfasserin aut H. Z. Huang verfasserin aut R. Huang verfasserin aut J. Johnston verfasserin aut A. Juillard verfasserin aut H. Khalife verfasserin aut M. Kleifges verfasserin aut V. V. Kobychev verfasserin aut Yu. G. Kolomensky verfasserin aut S. I. Konovalov verfasserin aut A. Leder verfasserin aut P. Loaiza verfasserin aut L. Ma verfasserin aut E. P. Makarov verfasserin aut P. de Marcillac verfasserin aut L. Marini verfasserin aut S. Marnieros verfasserin aut D. Misiak verfasserin aut X. -F. Navick verfasserin aut C. Nones verfasserin aut V. Novati verfasserin aut E. Olivieri verfasserin aut J. L. Ouellet verfasserin aut L. Pagnanini verfasserin aut P. Pari verfasserin aut L. Pattavina verfasserin aut B. Paul verfasserin aut M. Pavan verfasserin aut H. Peng verfasserin aut G. Pessina verfasserin aut S. Pirro verfasserin aut D. V. Poda verfasserin aut O. G. Polischuk verfasserin aut E. Previtali verfasserin aut Th. Redon verfasserin aut S. Rozov verfasserin aut C. Rusconi verfasserin aut V. Sanglard verfasserin aut K. Schäffner verfasserin aut B. Schmidt verfasserin aut Y. Shen verfasserin aut V. N. Shlegel verfasserin aut B. Siebenborn verfasserin aut V. Singh verfasserin aut S. Sorbino verfasserin aut C. Tomei verfasserin aut V. I. Tretyak verfasserin aut V. I. Umatov verfasserin aut L. Vagneron verfasserin aut M. Velázquez verfasserin aut M. Weber verfasserin aut B. Welliver verfasserin aut L. Winslow verfasserin aut M. Xue verfasserin aut E. Yakushev verfasserin aut A. S. Zolotarova verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 1, Seite 15 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:1 pages:15 https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/article/885ed12ff85b43d48cb17b3b97e342a2 kostenfrei https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 1 15 |
| allfields_unstemmed |
10.1140/epjc/s10052-019-7578-6 doi (DE-627)DOAJ056032013 (DE-599)DOAJ885ed12ff85b43d48cb17b3b97e342a2 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Armengaud verfasserin aut The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity C. Augier verfasserin aut A. S. Barabash verfasserin aut F. Bellini verfasserin aut G. Benato verfasserin aut A. Benoît verfasserin aut M. Beretta verfasserin aut L. Bergé verfasserin aut J. Billard verfasserin aut Yu. A. Borovlev verfasserin aut Ch. Bourgeois verfasserin aut M. Briere verfasserin aut V. B. Brudanin verfasserin aut P. Camus verfasserin aut L. Cardani verfasserin aut N. Casali verfasserin aut A. Cazes verfasserin aut M. Chapellier verfasserin aut F. Charlieux verfasserin aut M. de Combarieu verfasserin aut I. Dafinei verfasserin aut F. A. Danevich verfasserin aut M. De Jesus verfasserin aut L. Dumoulin verfasserin aut K. Eitel verfasserin aut E. Elkhoury verfasserin aut F. Ferri verfasserin aut B. K. Fujikawa verfasserin aut J. Gascon verfasserin aut L. Gironi verfasserin aut A. Giuliani verfasserin aut V. D. Grigorieva verfasserin aut M. Gros verfasserin aut E. Guerard verfasserin aut D. L. Helis verfasserin aut H. Z. Huang verfasserin aut R. Huang verfasserin aut J. Johnston verfasserin aut A. Juillard verfasserin aut H. Khalife verfasserin aut M. Kleifges verfasserin aut V. V. Kobychev verfasserin aut Yu. G. Kolomensky verfasserin aut S. I. Konovalov verfasserin aut A. Leder verfasserin aut P. Loaiza verfasserin aut L. Ma verfasserin aut E. P. Makarov verfasserin aut P. de Marcillac verfasserin aut L. Marini verfasserin aut S. Marnieros verfasserin aut D. Misiak verfasserin aut X. -F. Navick verfasserin aut C. Nones verfasserin aut V. Novati verfasserin aut E. Olivieri verfasserin aut J. L. Ouellet verfasserin aut L. Pagnanini verfasserin aut P. Pari verfasserin aut L. Pattavina verfasserin aut B. Paul verfasserin aut M. Pavan verfasserin aut H. Peng verfasserin aut G. Pessina verfasserin aut S. Pirro verfasserin aut D. V. Poda verfasserin aut O. G. Polischuk verfasserin aut E. Previtali verfasserin aut Th. Redon verfasserin aut S. Rozov verfasserin aut C. Rusconi verfasserin aut V. Sanglard verfasserin aut K. Schäffner verfasserin aut B. Schmidt verfasserin aut Y. Shen verfasserin aut V. N. Shlegel verfasserin aut B. Siebenborn verfasserin aut V. Singh verfasserin aut S. Sorbino verfasserin aut C. Tomei verfasserin aut V. I. Tretyak verfasserin aut V. I. Umatov verfasserin aut L. Vagneron verfasserin aut M. Velázquez verfasserin aut M. Weber verfasserin aut B. Welliver verfasserin aut L. Winslow verfasserin aut M. Xue verfasserin aut E. Yakushev verfasserin aut A. S. Zolotarova verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 1, Seite 15 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:1 pages:15 https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/article/885ed12ff85b43d48cb17b3b97e342a2 kostenfrei https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 1 15 |
| allfieldsGer |
10.1140/epjc/s10052-019-7578-6 doi (DE-627)DOAJ056032013 (DE-599)DOAJ885ed12ff85b43d48cb17b3b97e342a2 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Armengaud verfasserin aut The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity C. Augier verfasserin aut A. S. Barabash verfasserin aut F. Bellini verfasserin aut G. Benato verfasserin aut A. Benoît verfasserin aut M. Beretta verfasserin aut L. Bergé verfasserin aut J. Billard verfasserin aut Yu. A. Borovlev verfasserin aut Ch. Bourgeois verfasserin aut M. Briere verfasserin aut V. B. Brudanin verfasserin aut P. Camus verfasserin aut L. Cardani verfasserin aut N. Casali verfasserin aut A. Cazes verfasserin aut M. Chapellier verfasserin aut F. Charlieux verfasserin aut M. de Combarieu verfasserin aut I. Dafinei verfasserin aut F. A. Danevich verfasserin aut M. De Jesus verfasserin aut L. Dumoulin verfasserin aut K. Eitel verfasserin aut E. Elkhoury verfasserin aut F. Ferri verfasserin aut B. K. Fujikawa verfasserin aut J. Gascon verfasserin aut L. Gironi verfasserin aut A. Giuliani verfasserin aut V. D. Grigorieva verfasserin aut M. Gros verfasserin aut E. Guerard verfasserin aut D. L. Helis verfasserin aut H. Z. Huang verfasserin aut R. Huang verfasserin aut J. Johnston verfasserin aut A. Juillard verfasserin aut H. Khalife verfasserin aut M. Kleifges verfasserin aut V. V. Kobychev verfasserin aut Yu. G. Kolomensky verfasserin aut S. I. Konovalov verfasserin aut A. Leder verfasserin aut P. Loaiza verfasserin aut L. Ma verfasserin aut E. P. Makarov verfasserin aut P. de Marcillac verfasserin aut L. Marini verfasserin aut S. Marnieros verfasserin aut D. Misiak verfasserin aut X. -F. Navick verfasserin aut C. Nones verfasserin aut V. Novati verfasserin aut E. Olivieri verfasserin aut J. L. Ouellet verfasserin aut L. Pagnanini verfasserin aut P. Pari verfasserin aut L. Pattavina verfasserin aut B. Paul verfasserin aut M. Pavan verfasserin aut H. Peng verfasserin aut G. Pessina verfasserin aut S. Pirro verfasserin aut D. V. Poda verfasserin aut O. G. Polischuk verfasserin aut E. Previtali verfasserin aut Th. Redon verfasserin aut S. Rozov verfasserin aut C. Rusconi verfasserin aut V. Sanglard verfasserin aut K. Schäffner verfasserin aut B. Schmidt verfasserin aut Y. Shen verfasserin aut V. N. Shlegel verfasserin aut B. Siebenborn verfasserin aut V. Singh verfasserin aut S. Sorbino verfasserin aut C. Tomei verfasserin aut V. I. Tretyak verfasserin aut V. I. Umatov verfasserin aut L. Vagneron verfasserin aut M. Velázquez verfasserin aut M. Weber verfasserin aut B. Welliver verfasserin aut L. Winslow verfasserin aut M. Xue verfasserin aut E. Yakushev verfasserin aut A. S. Zolotarova verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 1, Seite 15 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:1 pages:15 https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/article/885ed12ff85b43d48cb17b3b97e342a2 kostenfrei https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 1 15 |
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10.1140/epjc/s10052-019-7578-6 doi (DE-627)DOAJ056032013 (DE-599)DOAJ885ed12ff85b43d48cb17b3b97e342a2 DE-627 ger DE-627 rakwb eng QB460-466 QC770-798 E. Armengaud verfasserin aut The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects 2020 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. Astrophysics Nuclear and particle physics. Atomic energy. Radioactivity C. Augier verfasserin aut A. S. Barabash verfasserin aut F. Bellini verfasserin aut G. Benato verfasserin aut A. Benoît verfasserin aut M. Beretta verfasserin aut L. Bergé verfasserin aut J. Billard verfasserin aut Yu. A. Borovlev verfasserin aut Ch. Bourgeois verfasserin aut M. Briere verfasserin aut V. B. Brudanin verfasserin aut P. Camus verfasserin aut L. Cardani verfasserin aut N. Casali verfasserin aut A. Cazes verfasserin aut M. Chapellier verfasserin aut F. Charlieux verfasserin aut M. de Combarieu verfasserin aut I. Dafinei verfasserin aut F. A. Danevich verfasserin aut M. De Jesus verfasserin aut L. Dumoulin verfasserin aut K. Eitel verfasserin aut E. Elkhoury verfasserin aut F. Ferri verfasserin aut B. K. Fujikawa verfasserin aut J. Gascon verfasserin aut L. Gironi verfasserin aut A. Giuliani verfasserin aut V. D. Grigorieva verfasserin aut M. Gros verfasserin aut E. Guerard verfasserin aut D. L. Helis verfasserin aut H. Z. Huang verfasserin aut R. Huang verfasserin aut J. Johnston verfasserin aut A. Juillard verfasserin aut H. Khalife verfasserin aut M. Kleifges verfasserin aut V. V. Kobychev verfasserin aut Yu. G. Kolomensky verfasserin aut S. I. Konovalov verfasserin aut A. Leder verfasserin aut P. Loaiza verfasserin aut L. Ma verfasserin aut E. P. Makarov verfasserin aut P. de Marcillac verfasserin aut L. Marini verfasserin aut S. Marnieros verfasserin aut D. Misiak verfasserin aut X. -F. Navick verfasserin aut C. Nones verfasserin aut V. Novati verfasserin aut E. Olivieri verfasserin aut J. L. Ouellet verfasserin aut L. Pagnanini verfasserin aut P. Pari verfasserin aut L. Pattavina verfasserin aut B. Paul verfasserin aut M. Pavan verfasserin aut H. Peng verfasserin aut G. Pessina verfasserin aut S. Pirro verfasserin aut D. V. Poda verfasserin aut O. G. Polischuk verfasserin aut E. Previtali verfasserin aut Th. Redon verfasserin aut S. Rozov verfasserin aut C. Rusconi verfasserin aut V. Sanglard verfasserin aut K. Schäffner verfasserin aut B. Schmidt verfasserin aut Y. Shen verfasserin aut V. N. Shlegel verfasserin aut B. Siebenborn verfasserin aut V. Singh verfasserin aut S. Sorbino verfasserin aut C. Tomei verfasserin aut V. I. Tretyak verfasserin aut V. I. Umatov verfasserin aut L. Vagneron verfasserin aut M. Velázquez verfasserin aut M. Weber verfasserin aut B. Welliver verfasserin aut L. Winslow verfasserin aut M. Xue verfasserin aut E. Yakushev verfasserin aut A. S. Zolotarova verfasserin aut In European Physical Journal C: Particles and Fields SpringerOpen, 2017 80(2020), 1, Seite 15 (DE-627)253722934 (DE-600)1459069-4 14346052 nnns volume:80 year:2020 number:1 pages:15 https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/article/885ed12ff85b43d48cb17b3b97e342a2 kostenfrei https://doi.org/10.1140/epjc/s10052-019-7578-6 kostenfrei https://doaj.org/toc/1434-6044 Journal toc kostenfrei https://doaj.org/toc/1434-6052 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_150 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_267 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2018 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2031 GBV_ILN_2038 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2113 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 80 2020 1 15 |
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E. Armengaud @@aut@@ C. Augier @@aut@@ A. S. Barabash @@aut@@ F. Bellini @@aut@@ G. Benato @@aut@@ A. Benoît @@aut@@ M. Beretta @@aut@@ L. Bergé @@aut@@ J. Billard @@aut@@ Yu. A. Borovlev @@aut@@ Ch. Bourgeois @@aut@@ M. Briere @@aut@@ V. B. Brudanin @@aut@@ P. Camus @@aut@@ L. Cardani @@aut@@ N. Casali @@aut@@ A. Cazes @@aut@@ M. Chapellier @@aut@@ F. Charlieux @@aut@@ M. de Combarieu @@aut@@ I. Dafinei @@aut@@ F. A. Danevich @@aut@@ M. De Jesus @@aut@@ L. Dumoulin @@aut@@ K. Eitel @@aut@@ E. Elkhoury @@aut@@ F. Ferri @@aut@@ B. K. Fujikawa @@aut@@ J. Gascon @@aut@@ L. Gironi @@aut@@ A. Giuliani @@aut@@ V. D. Grigorieva @@aut@@ M. Gros @@aut@@ E. Guerard @@aut@@ D. L. Helis @@aut@@ H. Z. Huang @@aut@@ R. Huang @@aut@@ J. Johnston @@aut@@ A. Juillard @@aut@@ H. Khalife @@aut@@ M. Kleifges @@aut@@ V. V. Kobychev @@aut@@ Yu. G. Kolomensky @@aut@@ S. I. Konovalov @@aut@@ A. Leder @@aut@@ P. Loaiza @@aut@@ L. Ma @@aut@@ E. P. Makarov @@aut@@ P. de Marcillac @@aut@@ L. Marini @@aut@@ S. Marnieros @@aut@@ D. Misiak @@aut@@ X. -F. Navick @@aut@@ C. Nones @@aut@@ V. Novati @@aut@@ E. Olivieri @@aut@@ J. L. Ouellet @@aut@@ L. Pagnanini @@aut@@ P. Pari @@aut@@ L. Pattavina @@aut@@ B. Paul @@aut@@ M. Pavan @@aut@@ H. Peng @@aut@@ G. Pessina @@aut@@ S. Pirro @@aut@@ D. V. Poda @@aut@@ O. G. Polischuk @@aut@@ E. Previtali @@aut@@ Th. Redon @@aut@@ S. Rozov @@aut@@ C. Rusconi @@aut@@ V. Sanglard @@aut@@ K. Schäffner @@aut@@ B. Schmidt @@aut@@ Y. Shen @@aut@@ V. N. Shlegel @@aut@@ B. Siebenborn @@aut@@ V. Singh @@aut@@ S. Sorbino @@aut@@ C. Tomei @@aut@@ V. I. Tretyak @@aut@@ V. I. Umatov @@aut@@ L. Vagneron @@aut@@ M. Velázquez @@aut@@ M. Weber @@aut@@ B. Welliver @@aut@@ L. Winslow @@aut@@ M. Xue @@aut@@ E. Yakushev @@aut@@ A. S. Zolotarova @@aut@@ |
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In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . 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Q - Science |
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E. Armengaud |
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E. Armengaud misc QB460-466 misc QC770-798 misc Astrophysics misc Nuclear and particle physics. Atomic energy. Radioactivity The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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QB460-466 |
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14346052 |
| topic_title |
QB460-466 QC770-798 The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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E. Armengaud |
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E. Armengaud C. Augier A. S. Barabash F. Bellini G. Benato A. Benoît M. Beretta L. Bergé J. Billard Yu. A. Borovlev Ch. Bourgeois M. Briere V. B. Brudanin P. Camus L. Cardani N. Casali A. Cazes M. Chapellier F. Charlieux M. de Combarieu I. Dafinei F. A. Danevich M. De Jesus L. Dumoulin K. Eitel E. Elkhoury F. Ferri B. K. Fujikawa J. Gascon L. Gironi A. Giuliani V. D. Grigorieva M. Gros E. Guerard D. L. Helis H. Z. Huang R. Huang J. Johnston A. Juillard H. Khalife M. Kleifges V. V. Kobychev Yu. G. Kolomensky S. I. Konovalov A. Leder P. Loaiza L. Ma E. P. Makarov P. de Marcillac L. Marini S. Marnieros D. Misiak X. -F. Navick C. Nones V. Novati E. Olivieri J. L. Ouellet L. Pagnanini P. Pari L. Pattavina B. Paul M. Pavan H. Peng G. Pessina S. Pirro D. V. Poda O. G. Polischuk E. Previtali Th. Redon S. Rozov C. Rusconi V. Sanglard K. Schäffner B. Schmidt Y. Shen V. N. Shlegel B. Siebenborn V. Singh S. Sorbino C. Tomei V. I. Tretyak V. I. Umatov L. Vagneron M. Velázquez M. Weber B. Welliver L. Winslow M. Xue E. Yakushev A. S. Zolotarova |
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cupid-mo experiment for neutrinoless double-beta decay: performance and prospects |
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The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. |
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Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. |
| abstract_unstemmed |
Abstract CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$ 0νββ ) of $$^{100}\hbox {Mo}$$ 100Mo . In this article, we detail the CUPID-Mo detector concept, assembly and installation in the Modane underground laboratory, providing results from the first datasets. The CUPID-Mo detector consists of an array of 20 $$^{100}\hbox {Mo}$$ 100Mo -enriched 0.2 kg $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals operated as scintillating bolometers at $$\sim 20\hbox { mK}$$ ∼20mK . The $$\hbox {Li}_2\hbox {MoO}_4$$ Li2MoO4 crystals are complemented by 20 thin Ge optical bolometers to reject $$\alpha $$ α events by the simultaneous detection of heat and scintillation light. We observe a good detector uniformity and an excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Light collection ensures the rejection of $$\alpha $$ α particles at a level much higher than 99.9% – with equally high acceptance for $$\gamma $$ γ /$$\beta $$ β events – in the region of interest for $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ . We present limits on the crystals’ radiopurity: $$\le 3~\mu \hbox {Bq/kg}$$ ≤3μBq/kg of $$^{226}\hbox {Ra}$$ 226Ra and $$\le 2~\mu \hbox {Bq/kg}$$ ≤2μBq/kg of $$^{232}\hbox {Th}$$ 232Th . We discuss the science reach of CUPID-Mo, which can set the most stringent half-life limit on the $$^{100}\hbox {Mo}$$ 100Mo $$0\nu \beta \beta $$ 0νββ decay in half-a-year’s livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology developed by the LUMINEU project and subsequently selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale bolometric $$0\nu \beta \beta $$ 0νββ experiment. |
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The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects |
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C. Augier A. S. Barabash F. Bellini G. Benato A. Benoît M. Beretta L. Bergé J. Billard Yu. A. Borovlev Ch. Bourgeois M. Briere V. B. Brudanin P. Camus L. Cardani N. Casali A. Cazes M. Chapellier F. Charlieux M. de Combarieu I. Dafinei F. A. Danevich M. De Jesus L. Dumoulin K. Eitel E. Elkhoury F. Ferri B. K. Fujikawa J. Gascon L. Gironi A. Giuliani V. D. Grigorieva M. Gros E. Guerard D. L. Helis H. Z. Huang R. Huang J. Johnston A. Juillard H. Khalife M. Kleifges V. V. Kobychev Yu. G. Kolomensky S. I. Konovalov A. Leder P. Loaiza L. Ma E. P. Makarov P. de Marcillac L. Marini S. Marnieros D. Misiak X. -F. Navick C. Nones V. Novati E. Olivieri J. L. Ouellet L. Pagnanini P. Pari L. Pattavina B. Paul M. Pavan H. Peng G. Pessina S. Pirro D. V. Poda O. G. Polischuk E. Previtali Th. Redon S. Rozov C. Rusconi V. Sanglard K. Schäffner B. Schmidt Y. Shen V. N. Shlegel B. Siebenborn V. Singh S. Sorbino C. Tomei V. I. Tretyak V. I. Umatov L. Vagneron M. Velázquez M. Weber B. Welliver L. Winslow M. Xue E. Yakushev A. S. Zolotarova |
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C. Augier A. S. Barabash F. Bellini G. Benato A. Benoît M. Beretta L. Bergé J. Billard Yu. A. Borovlev Ch. Bourgeois M. Briere V. B. Brudanin P. Camus L. Cardani N. Casali A. Cazes M. Chapellier F. Charlieux M. de Combarieu I. Dafinei F. A. Danevich M. De Jesus L. Dumoulin K. Eitel E. Elkhoury F. Ferri B. K. Fujikawa J. Gascon L. Gironi A. Giuliani V. D. Grigorieva M. Gros E. Guerard D. L. Helis H. Z. Huang R. Huang J. Johnston A. Juillard H. Khalife M. Kleifges V. V. Kobychev Yu. G. Kolomensky S. I. Konovalov A. Leder P. Loaiza L. Ma E. P. Makarov P. de Marcillac L. Marini S. Marnieros D. Misiak X. -F. Navick C. Nones V. Novati E. Olivieri J. L. Ouellet L. Pagnanini P. Pari L. Pattavina B. Paul M. Pavan H. Peng G. Pessina S. Pirro D. V. Poda O. G. Polischuk E. Previtali Th. Redon S. Rozov C. Rusconi V. Sanglard K. Schäffner B. Schmidt Y. Shen V. N. Shlegel B. Siebenborn V. Singh S. Sorbino C. Tomei V. I. Tretyak V. I. Umatov L. Vagneron M. Velázquez M. Weber B. Welliver L. Winslow M. Xue E. Yakushev A. S. Zolotarova |
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| score |
7.399867 |