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The lower and upper bounds on the neutrinoless double beta (0nu-2beta) decay rate are obtained, as functions of the parameters of neutrino oscillations and of the lightest neutrino mass. The constraints on these parameters from the search…

High Energy Physics - Phenomenology · Physics 2009-10-31 Francesco Vissani

We study the implications of the Dark-LMA solution to the solar neutrino problem for neutrino-less double beta decay ($0\nu\beta\beta$ ). We show that while the predictions for the effective mass governing $0\nu\beta\beta$ remains unchanged…

High Energy Physics - Phenomenology · Physics 2019-12-17 Vishnudath K. N. , Sandhya Choubey , Srubabati Goswami

\textbf{T}he \textbf{IN}dia's \textbf{TIN} (TIN.TIN) detector is under development in the search for neutrinoless double-$\beta$ decay (0$\nu\beta\beta$) using 90\% enriched $^{124}$Sn isotope as the target mass. This detector will be…

High Energy Physics - Phenomenology · Physics 2019-12-20 Manoj Kumar Singh , Lakhwinder Singh , Vivek Sharma , Manoj Kumar Singh , Abhishek Kumar , Akash Pandey , Venktesh Singh , Henry Tsz-King Wong

A next-generation rare pion decay experiment, PIONEER, is strongly motivated by several inconsistencies between Standard Model (SM) predictions and data pointing towards the potential violation of lepton flavor universality. It will probe…

CUPID-0 is the first pilot experiment of CUPID, a next-generation project for the measurement of neutrinoless double beta decay (0$\nu$DBD) with scintillating bolometers. The detector, consisting of 24 enriched and 2 natural ZnSe crystals,…

CANDLES experiment in Kamioka Underground Observatory aims to obtain the neutrino-less double beta decay ($0\nu\beta\beta$) from $^{48}$Ca. This measurement is a big challenge due to the extremely rare decay rate of $^{48}$Ca. Thus, in…

Instrumentation and Detectors · Physics 2020-10-23 Bui Tuan Khai

The NEMO-3 experiment measured the half-life of the $2\nu\beta\beta$ decay and searched for the $0\nu\beta\beta$ decay of $^{116}$Cd. Using $410$ g of $^{116}$Cd installed in the detector with an exposure of $5.26$ y, ($4968\pm74$) events…

The double beta decay experiment NEMO~3 has been taking data since February 2003. The aim of this experiment is to search for neutrinoless decay and investigate two neutrino double beta decay in seven different enriched isotopes…

Nuclear Experiment · Physics 2009-07-24 A. S. Barabash

NEXT (Neutrino Experiment with a Xenon TPC) is an experimental program whose goals are to discover neutrinoless double beta decay using $^{136}$Xe in high pressure xenon TPCs with electroluminescent readout. In this paper, results from the…

High Energy Physics - Experiment · Physics 2019-06-06 J. J. Gomez-Cadenas

We present a study of the sensitivity and discovery potential of CUORE, a bolometric double-beta decay experiment under construction at the Laboratori Nazionali del Gran Sasso in Italy. Two approaches to the computation of experimental…

Nuclear Experiment · Physics 2013-03-21 F. Alessandria , R. Ardito , D. R. Artusa , F. T. Avignone , O. Azzolini , M. Balata , T. I. Banks , G. Bari , J. Beeman , F. Bellini , A. Bersani , M. Biassoni , T. Bloxham , C. Brofferio , C. Bucci , X. Z. Cai , L. Canonica , X. Cao , S. Capelli , L. Carbone , L. Cardani , M. Carrettoni , N. Casali , D. Chiesa , N. Chott , M. Clemenza , C. Cosmelli , O. Cremonesi , R. J. Creswick , I. Dafinei , A. Dally , V. Datskov , A. De Biasi , M. M. Deninno , S. Di Domizio , M. L. di Vacri , L. Ejzak , R. Faccini , D. Q. Fang , H. A. Farach , M. Faverzani , G. Fernandes , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , B. K. Fujikawa , A. Giachero , L. Gironi , A. Giuliani , J. Goett , P. Gorla , C. Gotti , E. Guardincerri , T. D. Gutierrez , E. E. Haller , K. Han , K. M. Heeger , H. Z. Huang , R. Kadel , K. Kazkaz , G. Keppel , L. Kogler , Yu. G. Kolomensky , D. Lenz , Y. L. Li , C. Ligi , X. Liu , Y. G. Ma , C. Maiano , M. Maino , M. Martinez , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , T. Napolitano , S. Newman , S. Nisi , C. Nones , E. B. Norman , A. Nucciotti , T. O'Donnell , F. Orio , D. Orlandi , J. L. Ouellet , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , G. Pessina , G. Piperno , S. Pirro , E. Previtali , V. Rampazzo , F. Rimondi , C. Rosenfeld , C. Rusconi , E. Sala , S. Sangiorgio , N. D. Scielzo , M. Sisti , A. R. Smith , F. Stivanello , L. Taffarello , M. Tenconi , W. D. Tian , C. Tomei , S. Trentalange , G. Ventura , M. Vignati , B. S. Wang , H. W. Wang , T. Wise , A. Woodcraft , L. Zanotti , C. Zarra , B. X. Zhu , S. Zucchelli

nEXO is a proposed experiment that will search for neutrinoless double-beta decay (0$\nu\beta\beta$) in 5-tonnes of liquid xenon (LXe), isotopically enriched in $^{136}$Xe. A technique called Ba-tagging is being developed as a potential…

The GERmanium Detector Array (GERDA) experiment at the Gran Sasso underground laboratory (LNGS) of INFN is searching for neutrinoless double-beta ($0\nu\beta\beta$) decay of $^{76}$Ge. The technological challenge of GERDA is to operate in a…

Nuclear Experiment · Physics 2020-04-02 GERDA collaboration , Matteo Agostini , Alexander M. Bakalyarov , Marco Balata , Igor Barabanov , Laura Baudis , Christian Bauer , Enrico Bellotti , Sergej Belogurov , Alessandro Bettini , Leonid Bezrukov , Dariusz Borowicz , Elisabetta Bossio , Vikas Bothe , Victor Brudanin , Riccardo Brugnera , Allen Caldwell , Carla Cattadori , Andrey Chernogorov , Tommaso Comellato , Valerio D'Andrea , Elena V. Demidova , Natalia Di Marco , Alexander Domula , Evgenyi Doroshkevich , Viacheslav Egorov , Felix Fischer , Maria Fomina , Albert Gangapshev , Alberto Garfagnini , Chris Gooch , Peter Grabmayr , Valery Gurentsov , Konstantin Gusev , Janina Hakenmüller , Sabine Hemmer , Roman Hiller , Werner Hofmann , Mikael Hult , Lev V. Inzhechik , Jozsef Janicskó Csáthy , Josef Jochum , Matthias Junker , Vladimir Kazalov , Yoann Kermaïdic , Thomas Kihm , Igor V. Kirpichnikov , Alexander Klimenko , Raphael Kneißl , Karl T. Knöpfle , Oleg Kochetov , Vasily N. Kornoukhov , Patrick Krause , Valery V. Kuzminov , Matthias Laubenstein , Andrea Lazzaro , Manfred Lindner , Ivano Lippi , Alexey Lubashevskiy , Bayarto Lubsandorzhiev , Guillaume Lutter , Carla Macolino , Bela Majorovits , Werner Maneschg , Michael Miloradovic , Rizalina Mingazheva , Marcin Misiaszek , Pavel Moseev , Igor Nemchenok , Krysztof Panas , Luciano Pandola , Krysztof Pelczar , Luigi Pertoldi , Paolo Piseri , Alberto Pullia , Chloe Ransom , Stefano Riboldi , Nadezda Rumyantseva , Cinzia Sada , Francesco Salamida , Stefan Schönert , Jochen Schreiner , Mario Schütt , Ann-Katrin Schütz , Oliver Schulz , Mario Schwarz , Bernhard Schwingenheuer , Oleg Selivanenko , Egor Shevchik , Mark Shirchenko , Hardy Simgen , Anatoly Smolnikov , Danila Stukov , Laura Vanhoefer , Andrey A. Vasenko , Anna Veresnikova , Chiara Vignoli , Katharina von Sturm , Thomas Wester , Christoph Wiesinger , Marcin Wojcik , Evgeny Yanovich , Birgit Zatschler , Igor Zhitnikov , Sergey V. Zhukov , Daniya Zinatulina , Andreas Zschocke , Anna J. Zsigmond , Kai Zuber , Grzegorz Zuzel

Searching for neutrinoless double-beta decay (0$\nu$2$\beta$) is one of the main experimental challenges of modern physics. One experimental technique is given by cryogenic detectors named bolometers that are really promising for this…

Instrumentation and Detectors · Physics 2023-01-18 A. Armatol

The NEMO-3 detector, which had been operating in the Modane Underground Laboratory from 2003 to 2010, was designed to search for neutrinoless double $\beta$ ($0\nu\beta\beta$) decay. We report final results of a search for $0\nu\beta\beta$…

The 2 nu double beta decay half-lives of six nuclei, whose decays were previously reported as theoretically forbidden, are calculated by including the pairing interaction, which mixes different occupations and opens up the possibility of…

Nuclear Theory · Physics 2014-11-18 Jorge G. Hirsch , Octavio Castanos , Peter O. Hess , Osvaldo Civitarese

The projected sensitivity of the LUX-ZEPLIN (LZ) experiment to two-neutrino and neutrinoless double beta decay of $^{134}$Xe is presented. LZ is a 10-tonne xenon time projection chamber optimized for the detection of dark matter particles,…

Instrumentation and Detectors · Physics 2022-01-12 The LUX-ZEPLIN , Collaboration , : , D. S. Akerib , A. K. Al Musalhi , S. K. Alsum , C. S. Amarasinghe , A. Ames , T. J. Anderson , N. Angelides , H. M. Araujo , J. E. Armstrong , M. Arthurs , X. Bai , J. Balajthy , S. Balashov , J. Bang , J. W. Bargemann , D. Bauer , A. Baxter , P. Beltrame , E. P. Bernard , A. Bernstein , A. Bhatti , A. Biekert , T. P. Biesiadzinski , H. J. Birch , G. M. Blockinger , E. Bodnia , B. Boxer , C. A. J. Brew , P. Bras , S. Burdin , J. K. Busenitz , M. Buuck , R. Cabrita , M. C. Carmona-Benitez , M. Cascella , C. Chan , N. I. Chott , A. Cole , M. V. Converse , A. Cottle , G. Cox , O. Creaner , J. E. Cutter , C. E. Dahl , L. de Viveiros , J. E. Y. Dobson , E. Druszkiewicz , S. R. Eriksen , A. Fan , S. Fayer , N. M. Fearon , S. Fiorucci , H. Flaecher , E. D. Fraser , T. Fruth , R. J. Gaitskell , J. Genovesi , C. Ghag , E. Gibson , S. Gokhale , M. G. D. van der Grinten , C. B. Gwilliam , C. R. Hall , S. J. Haselschwardt , S. A. Hertel , M. Horn , D. Q. Huang , C. M. Ignarra , O. Jahangir , R. S. James , W. Ji , J. Johnson , A. C. Kaboth , A. C. Kamaha , K. Kamdin , K. Kazkaz , D. Khaitan , A. Khazov , I. Khurana , D. Kodroff , L. Korley , E. V. Korolkova , H. Kraus , S. Kravitz , L. Kreczko , B. Krikler , V. A. Kudryavtsev , E. A. Leason , J. Lee , D. S. Leonard , K. T. Lesko , C. Levy , J. Liao , J. Lin , A. Lindote , R. Linehan , W. H. Lippincott , X. Liu , M. I. Lopes , E. Lopez Asamar , B. Lopez Paredes , W. Lorenzon , S. Luitz , P. A. Majewski , A. Manalaysay , L. Manenti , R. L. Mannino , N. Marangou , M. E. McCarthy , D. N. McKinsey , J. McLaughlin , E. H. Miller , E. Mizrachi , A. Monte , M. E. Monzani , J. A. Morad , J. D. Morales Mendoza , E. Morrison , B. J. Mount , A. St. J. Murphy , D. Naim , A. Naylor , C. Nedlik , H. N. Nelson , F. Neves , J. A. Nikoleyczik , A. Nilima , I. Olcina , K. C. Oliver-Mallory , S. Pal , K. J. Palladino , J. Palmer , S. Patton , N. Parveen , E. K. Pease , B. Penning , G. Pereira , A. Piepke , Y. Qie , J. Reichenbacher , C. A. Rhyne , A. Richards , Q. Riffard , G. R. C. Rischbieter , R. Rosero , P. Rossiter , D. Santone , A. B. M. R. Sazzad , R. W. Schnee , P. R. Scovell , S. Shaw , T. A. Shutt , J. J. Silk , C. Silva , R. Smith , M. Solmaz , V. N. Solovov , P. Sorensen , J. Soria , I. Stancu , A. Stevens , K. Stifter , B. Suerfu , T. J. Sumner , N. Swanson , M. Szydagis , W. C. Taylor , R. Taylor , D. J. Temples , P. A. Terman , D. R. Tiedt , M. Timalsina , W. H. To , D. R. Tovey , M. Tripathi , D. R. Tronstad , W. Turner , U. Utku , A. Vaitkus , B. Wang , J. J. Wang , W. Wang , J. R. Watson , R. C. Webb , R. G. White , T. J. Whitis , M. Williams , F. L. H. Wolfs , D. Woodward , C. J. Wright , X. Xiang , J. Xu , M. Yeh , P. Zarzhitsky

The GERmanium Detector Array (GERDA) experiment at the Gran Sasso underground laboratory (LNGS) of INFN is searching for neutrinoless double beta decay of 76Ge. The signature of the signal is a monoenergetic peak at 2039 keV, the Q-value of…

Instrumentation and Detectors · Physics 2014-04-11 The GERDA collaboration , M. Agostini , M. Allardt , E. Andreotti , A. M. Bakalyarov , M. Balata , I. Barabanov , M. Barnabe Heider , N. Barros , L. Baudis , C. Bauer , N. Becerici-Schmidt , E. Bellotti , S. Belogurov , S. T. Belyaev , G. Benato , A. Bettini , L. Bezrukov , T. Bode , V. Brudanin , R. Brugnera , D. Budjas , A. Caldwell , C. Cattadori , A. Chernogorov , F. Cossavella , E. V. Demidova , A. Domula , V. Egorov , R. Falkenstein , A. Ferella , K. Freund , N. Frodyma , A. Gangapshev , A. Garfagnini , C. Gotti , P. Grabmayr , V. Gurentsov , K. Gusev , K. K. Guthikonda , W. Hampel , A. Hegai , M. Heisel , S. Hemmer , G. Heusser , W. Hofmann , M. Hult , L. V. Inzhechik , L. Ioannucci , J. Janicsko Csathy , J. Jochum , M. Junker , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Klimenko , K. T. Knoepfle , O. Kochetov , V. N. Kornoukhov , V. V. Kuzminov , M. Laubenstein , A. Lazzaro , V. I. Lebedev , B. Lehnert , H. Y. Liao , M. Lindner , I. Lippi , X. Liu , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , A. A. Machado , B. Majorovits , W. Maneschg , I. Nemchenok , S. Nisi , C. O'Shaughnessy , D. Palioselitis , L. Pandola , K. Pelczar , G. Pessina , A. Pullia , S. Riboldi , C. Sada , M. Salathe , C. Schmitt , J. Schreiner , O. Schulz , B. Schwingenheuer , S. Schoenert , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , H. Strecker , M. Tarka , C. A. Ur , A. A. Vasenko , O. Volynets , K. von Sturm , V. Wagner , M. Walter , A. Wegmann , T. Wester , M. Wojcik , E. Yanovich , P. Zavarise , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , K. Zuber , G. Zuzel

NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double beta decay experiment located at the Laboratorio Subterr\'aneo de Canfranc (LSC, Spain). Its aim is to demonstrate that the neutrino is a Majorana particle by detecting…

Instrumentation and Detectors · Physics 2022-09-21 Carmen Romo-Luque

The Standard Model of particle physics cannot explain the dominance of matter over anti-matter in our Universe. In many model extensions this is a very natural consequence of neutrinos being their own anti-particles (Majorana particles)…

Nuclear Experiment · Physics 2017-04-07 M. Agostini , M. Allardt , A. M. Bakalyarov , M. Balata , I. Barabanov , L. Baudis , C. Bauer , E. Bellotti , S. Belogurov , S. T. Belyaev , G. Benato , A. Bettini , L. Bezrukov , T. Bode , D. Borowicz , V. Brudanin , R. Brugnera , A. Caldwell , C. Cattadori , A. Chernogorov , V. D'Andrea , E. V. Demidova , N. DiMarco , A. diVacri , A. Domula , E. Doroshkevich , V. Egorov , R. Falkenstein , O. Fedorova , K. Freund , N. Frodyma , A. Gangapshev , A. Garfagnini , C. Gooch , P. Grabmayr , V. Gurentsov , K. Gusev , J. Hakenmüller , A. Hegai , M. Heisel , S. Hemmer , W. Hofmann , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , J. Jochum , M. Junker , V. Kazalov , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Kish , A. Klimenko , R. Kneißl , K. T. Knöpfle , O. Kochetov , V. N. Kornoukhov , V. V. Kuzminov , M. Laubenstein , A. Lazzaro , V. I. Lebedev , B. Lehnert , H. Y. Liao , M. Lindner , I. Lippi , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , B. Majorovits , W. Maneschg , E. Medinaceli , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , I. Nemchenok , D. Palioselitis , K. Panas , L. Pandola , K. Pelczar , A. Pullia , S. Riboldi , N. Rumyantseva , C. Sada , F. Salamida , M. Salathe , C. Schmitt , B. Schneider , S. Schönert , J. Schreiner , O. Schulz , A. -K. Schütz , B. Schwingenheuer , O. Selivanenko , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , L. Vanhoefer , A. A. Vasenko , A. Veresnikova , K. von Sturm , V. Wagner , M. Walter , A. Wegmann , T. Wester , C. Wiesinger , M. Wojcik , E. Yanovich , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , K. Zuber , G. Zuzel