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The NEMO collaboration is looking to measure neutrinoless double beta decay down to a lower limit of 0.1 eV for the effective neutrino mass. The NEMO 3 detector is now operating in the Frejus Underground Laboratory. The expected performance…

High Energy Physics - Experiment · Physics 2007-05-23 F. Piquemal , NEMO collaboration

The observation of neutrinoless double-beta decay would determine whether the neutrino is a Majorana particle and provide information on the absolute scale of neutrino mass. The MAJORANA Collaboration is constructing the DEMONSTRATOR, an…

The potential for using slow-fluor liquid scintillators to study low energy solar neutrinos and neutrinoless double beta decay (0nbb) is explored through a series of simulations. The fluorescence model assumed for the primary fluor has…

Instrumentation and Detectors · Physics 2022-05-24 Jack Dunger , Edward J. Leming , Steven D. Biller

The nEXO neutrinoless double beta decay experiment is designed to use a time projection chamber and 5000 kg of isotopically enriched liquid xenon to search for the decay in $^{136}$Xe. Progress in the detector design, paired with higher…

Nuclear Experiment · Physics 2022-02-24 nEXO Collaboration , G. Adhikari , S. Al Kharusi , E. Angelico , G. Anton , I. J. Arnquist , I. Badhrees , J. Bane , V. Belov , E. P. Bernard , T. Bhatta , A. Bolotnikov , P. A. Breur , J. P. Brodsky , E. Brown , T. Brunner , E. Caden , G. F. Cao , L. Cao , C. Chambers , B. Chana , S. A. Charlebois , D. Chernyak , M. Chiu , B. Cleveland , R. Collister , S. A. Czyz , J. Dalmasson , T. Daniels , L. Darroch , R. DeVoe , M. L. Di Vacri , J. Dilling , Y. Y. Ding , A. Dolgolenko , M. J. Dolinski , A. Dragone , J. Echevers , M. Elbeltagi , L. Fabris , D. Fairbank , W. Fairbank , J. Farine , S. Ferrara , S. Feyzbakhsh , Y. S. Fu , G. Gallina , P. Gautam , G. Giacomini , W. Gillis C. Gingras , D. Goeldi , R. Gornea , G. Gratta , C. A. Hardy , K. Harouaka , M. Heffner , E. W. Hoppe , A. House , A. Iverson , A. Jamil , M. Jewell , X. S. Jiang , A. Karelin , L. J. Kaufman , I. Kotov , R. Krücken , A. Kuchenkov , K. S. Kumar , Y. Lan , A. Larson , K. G. Leach , B. G. Lenardo , D. S. Leonard , G. Li , S. Li , Z. Li , C. Licciardi , R. Lindsay , R. MacLellan , M. Mahtab , P. Martel-Dion , J. Masbou , N. Massacret , T. McElroy , K. McMichael , M. Medina Peregrina , T. Michel , B. Mong , D. C. Moore , K. Murray , J. Nattress , C. R. Natzke , R. J. Newby , K. Ni , F. Nolet , O. Nusair , J. C. Nzobadila Ondze , K. Odgers , A. Odian , J. L. Orrell , G. S. Ortega , C. T. Overman , S. Parent , A. Perna , A. Piepke , A. Pocar , J-F. Pratte , N. Priel , V. Radeka , E. Raguzin , G. J. Ramonnye , T. Rao , H. Rasiwala , S. Rescia , F. Retière , J. Ringuette , V. Riot , T. Rossignol , P. C. Rowson , N. Roy , R. Saldanha , S. Sangiorgio , X. Shang , A. K. Soma , F. Spadoni , V. Stekhanov , X. L. Sun , M. Tarka , S. Thibado , A. Tidball , J. Todd , T. Totev , S. Triambak , R. H. M. Tsang , T. Tsang , F. Vachon , V. Veeraraghavan , S. Viel , C. Vivo-Vilches , P. Vogel , J-L. Vuilleumier , M. Wagenpfeil , T. Wager , M. Walent , K. Wamba , Q. Wang , W. Wei , L. J. Wen , U. Wichoski , S. Wilde , M. Worcester , S. X. Wu , W. H. Wu , X. Wu , Q. Xia , W. Yan , H. Yang , L. Yang , O. Zeldovich , J. Zhao , T. Ziegler

SuperNEMO is a next generation neutrinoless double beta decay experiment with a design capability to reach a half-life sensitivity of $10^{26}$ years corresponding to an effective Majorana neutrino mass of $\langle m_{\beta\beta} \rangle$…

Instrumentation and Detectors · Physics 2015-05-01 Xin Ran Liu

We investigate the predictions for neutrinoless double beta ($(\beta \beta)_{0 \nu}$-) decay effective Majorana mass $\left| \langle \, m \, \rangle \right|$ in the 3+1 and 3+2 schemes with one and two additional sterile neutrinos with…

High Energy Physics - Phenomenology · Physics 2014-06-10 Ivan Girardi , Aurora Meroni , S. T. Petcov

The electron antineutrino spectrum in the Stereo reactor experiment (ILL Grenoble) is measured via the inverse beta decay signals in an organic liquid scintillator. The six target cells of the Stereo detector are filled with about 1800…

Instrumentation and Detectors · Physics 2019-01-30 Christian Buck , Benjamin Gramlich , Manfred Lindner , Christian Roca , Stefan Schoppmann

The review of current experiments on search and studying of double beta decay processes is done. Results of the most sensitive experiments are discussed and values of modern limits on effective Majorana neutrino mass ($<m_{\nu}>) are given.…

Nuclear Experiment · Physics 2012-09-20 A. S. Barabash

One promising approach for future neutrinoless double beta decay ($0\nu\beta\beta$) searches is the incorporation of candidate isotopes into liquid scintillator detectors. In this work, a sample of the high-performance…

Background of germanium and xenon detectors due to the elastic scattering of $^{8}B$ solar neutrinos on electrons have been calculated. The background is 4.6 \times $10^{-4}$ counts/(keV$\cdot t\cdot$y) that defines the sensitivity of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alexander A. Klimenko

The NEMO-3 experiment is searching for neutrinoless double beta decay for 2 main isotopes (100Mo and 82Se) and is studying the two-neutrino double beta decay of seven isotopes. The experiment has been taking data since 2003 and, up to the…

High Energy Physics - Experiment · Physics 2019-08-14 Mathieu BONGRAND

Results are reported from a search for low-multiplicity neutrino bursts in the Sudbury Neutrino Observatory (SNO). Such bursts could indicate detection of a nearby core-collapse supernova explosion. The data were taken from Phase I…

High Energy Physics - Experiment · Physics 2012-08-27 SNO Collaboration

Latest results on $\beta\beta 0 \nu$, $\beta\beta 0 \nu\chi^0$ and $\beta\beta 2 \nu$ decays of different isotopes from NEMO-3 double beta decay experiment are presented. In particular, new limits on neurtinoless double beta decay of…

High Energy Physics - Experiment · Physics 2019-08-14 A. S. Barabash

The Jiangmen Underground Neutrino Observatory (JUNO) is proposed to determine the neutrino mass hierarchy using an underground liquid scintillator detector. It is located 53 km away from both Yangjiang and Taishan Nuclear Power Plants in…

Instrumentation and Detectors · Physics 2015-09-29 T. Adam , F. An , G. An , Q. An , N. Anfimov , V. Antonelli , G. Baccolo , M. Baldoncini , E. Baussan , M. Bellato , L. Bezrukov , D. Bick , S. Blyth , S. Boarin , A. Brigatti , T. Brugière , R. Brugnera , M. Buizza Avanzini , J. Busto , A. Cabrera , H. Cai , X. Cai , A. Cammi , D. Cao , G. Cao , J. Cao , J. Chang , Y. Chang , M. Chen , P. Chen , Q. Chen , S. Chen , S. Chen , S. Chen , X. Chen , Y. Chen , Y. Cheng , D. Chiesa , A. Chukanov , M. Clemenza , B. Clerbaux , D. D'Angelo , H. de Kerret , Z. Deng , Z. Deng , X. Ding , Y. Ding , Z. Djurcic , S. Dmitrievsky , M. Dolgareva , D. Dornic , E. Doroshkevich , M. Dracos , O. Drapier , S. Dusini , M. A. Díaz , T. Enqvist , D. Fan , C. Fang , J. Fang , X. Fang , L. Favart , D. Fedoseev , G. Fiorentini , R. Ford , A. Formozov , R. Gaigher , H. Gan , A. Garfagnini , G. Gaudiot , C. Genster , M. Giammarchi , F. Giuliani , M. Gonchar , G. Gong , H. Gong , M. Gonin , Y. Gornushkin , M. Grassi , C. Grewing , V. Gromov , M. Gu , M. Guan , V. Guarino , W. Guo , X. Guo , Y. Guo , M. Göger-Neff , P. Hackspacher , C. Hagner , R. Han , Z. Han , J. Hao , M. He , D. Hellgartner , Y. Heng , D. Hong , S. Hou , Y. Hsiung , B. Hu , J. Hu , S. Hu , T. Hu , W. Hu , H. Huang , X. Huang , X. Huang , L. Huo , W. Huo , A. Ioannisian , D. Ioannisyan , M. Jeitler , K. Jen , S. Jetter , X. Ji , X. Ji , S. Jian , D. Jiang , X. Jiang , C. Jollet , M. Kaiser , B. Kan , L. Kang , M. Karagounis , N. Kazarian , S. Kettell , D. Korablev , A. Krasnoperov , S. Krokhaleva , Z. Krumshteyn , A. Kruth , P. Kuusiniemi , T. Lachenmaier , L. Lei , R. Lei , X. Lei , R. Leitner , F. Lenz , C. Li , F. Li , F. Li , J. Li , N. Li , S. Li , T. Li , W. Li , W. Li , X. Li , X. Li , X. Li , X. Li , Y. Li , Y. Li , Z. Li , H. Liang , H. Liang , J. Liang , M. Licciardi , G. Lin , S. Lin , T. Lin , Y. Lin , I. Lippi , G. Liu , H. Liu , H. Liu , J. Liu , J. Liu , J. Liu , J. Liu , Q. Liu , Q. Liu , S. Liu , S. Liu , Y. Liu , P. Lombardi , Y. Long , S. Lorenz , C. Lu , F. Lu , H. Lu , J. Lu , J. Lu , J. Lu , B. Lubsandorzhiev , S. Lubsandorzhiev , L. Ludhova , F. Luo , S. Luo , Z. Lv , V. Lyashuk , Q. Ma , S. Ma , X. Ma , X. Ma , Y. Malyshkin , F. Mantovani , Y. Mao , S. Mari , D. Mayilyan , W. McDonough , G. Meng , A. Meregaglia , E. Meroni , M. Mezzetto , J. Min , L. Miramonti , M. Montuschi , N. Morozov , T. Mueller , P. Muralidharan , M. Nastasi , D. Naumov , E. Naumova , I. Nemchenok , Z. Ning , H. Nunokawa , L. Oberauer , J. P. Ochoa-Ricoux , A. Olshevskiy , F. Ortica , H. Pan , A. Paoloni , N. Parkalian , S. Parmeggiano , V. Pec , N. Pelliccia , H. Peng , P. Poussot , S. Pozzi , E. Previtali , S. Prummer , F. Qi , M. Qi , S. Qian , X. Qian , H. Qiao , Z. Qin , G. Ranucci , A. Re , B. Ren , J. Ren , T. Rezinko , B. Ricci , M. Robens , A. Romani , B. Roskovec , X. Ruan , X. Ruan , A. Rybnikov , A. Sadovsky , P. Saggese , G. Salamanna , J. Sawatzki , J. Schuler , A. Selyunin , G. Shi , J. Shi , Y. Shi , V. Sinev , C. Sirignano , M. Sisti , O. Smirnov , M. Soiron , A. Stahl , L. Stanco , J. Steinmann , V. Strati , G. Sun , X. Sun , Y. Sun , Y. Sun , D. Taichenachev , J. Tang , A. Tietzsch , I. Tkachev , W. H. Trzaska , Y. Tung , S. van Waasen , C. Volpe , V. Vorobel , L. Votano , C. Wang , C. Wang , C. Wang , G. Wang , H. Wang , M. Wang , R. Wang , S. Wang , W. Wang , W. Wang , Y. Wang , Y. Wang , Y. Wang , Y. Wang , Z. Wang , Z. Wang , Z. Wang , Z. Wang , Z. Wang , W. Wei , Y. Wei , M. Weifels , L. Wen , Y. Wen , C. Wiebusch , S. Wipperfurth , S. C. Wong , B. Wonsak , C. Wu , Q. Wu , Z. Wu , M. Wurm , J. Wurtz , Y. Xi , D. Xia , J. Xia , M. Xiao , Y. Xie , J. Xu , J. Xu , L. Xu , Y. Xu , B. Yan , X. Yan , C. Yang , C. Yang , H. Yang , L. Yang , M. Yang , Y. Yang , Y. Yang , Y. Yang , E. Yanovich , Y. Yao , M. Ye , X. Ye , U. Yegin , F. Yermia , Z. You , B. Yu , C. Yu , C. Yu , G. Yu , Z. Yu , Y. Yuan , Z. Yuan , M. Zanetti , P. Zeng , S. Zeng , T. Zeng , L. Zhan , C. Zhang , F. Zhang , G. Zhang , H. Zhang , J. Zhang , J. Zhang , J. Zhang , K. Zhang , P. Zhang , Q. Zhang , T. Zhang , X. Zhang , X. Zhang , Y. Zhang , Y. Zhang , Y. Zhang , Y. Zhang , Y. Zhang , Y. Zhang , Z. Zhang , Z. Zhang , J. Zhao , M. Zhao , T. Zhao , Y. Zhao , H. Zheng , M. Zheng , X. Zheng , Y. Zheng , W. Zhong , G. Zhou , J. Zhou , L. Zhou , N. Zhou , R. Zhou , S. Zhou , W. Zhou , X. Zhou , Y. Zhou , H. Zhu , K. Zhu , H. Zhuang , L. Zong , J. Zou

Neutrinoless double-beta decay (0$\nu\beta\beta$) decay is a hypothetical process that violates lepton number, and whose observation would unambiguously indicate that neutrinos are Majorana fermions. In the standard inverted-ordering…

Nuclear Experiment · Physics 2019-12-10 J. M. López-Castaño , I. Guinn

NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double-beta (\beta\beta 0\nu) decay experiment at the Canfranc Underground Laboratory (LSC). It seeks to detect the (\beta\beta 0\nu) decay of Xe-136 using a high pressure xenon…

Instrumentation and Detectors · Physics 2019-08-13 M. Nebot-Guinot

Tremendous efforts are required to scale the summit of observing neutrinoless double beta decay ($0 \nu \beta \beta$). This article quantitatively explores the interplay between exposure (target mass X data taking time) and background…

High Energy Physics - Experiment · Physics 2020-01-28 M. K. Singh , H. T. Wong , L. Singh , V. Sharma , V. Singh , Q. Yue