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Neutrinoless double-beta decay is practically the only way to establish the Majorana nature of the neutrino mass and its decay rate provides a probe of an effective neutrino mass. Double beta experiments are long-running underground…

Nuclear Experiment · Physics 2008-12-08 Oleg Chkvorets

The zero neutrino mode of the double beta decay in heavy deformed nuclei is investigated in the framework of the pseudo SU(3) model, which has provided an accurate description of collective nuclear structure and predicted half-lives for the…

Nuclear Theory · Physics 2009-10-28 Jorge G. Hirsch , O. Castaños , P. O. Hess

The GERmanium Detector Array, GERDA, is designed to search for neutrinoless double beta (0$\nu\beta\beta$) decay of $^{76}$Ge and it is installed in the Laboratori Nazionali del Gran Sasso (LNGS) of INFN, Italy. In this review, the…

High Energy Physics - Experiment · Physics 2013-12-30 Carla Macolino

The \MJ\ Collaboration is operating an array of high purity Ge detectors to search for neutrinoless double-beta decay in $^{76}$Ge. The \MJ\ \DEM\ comprises 44.1~kg of Ge detectors (29.7 kg enriched in $^{76}$Ge) split between two modules…

Nuclear Experiment · Physics 2018-04-04 C. E. Aalseth , N. Abgrall , E. Aguayo , S. I. Alvis , M. Amman , I. J. Arnquist , F. T. Avignone , H. O. Back , A. S. Barabash , P. S. Barbeau , C. J. Barton , P. J. Barton , F. E. Bertrand , T. Bode , B. Bos , M. Boswell , R. L. Brodzinski , A. W. Bradley , V. Brudanin , M. Busch , M. Buuck , A. S. Caldwell , T. S. Caldwell , Y-D. Chan , C. D. Christofferson , P. -H. Chu , J. I. Collar , D. C. Combs , R. J. Cooper , C. Cuesta , J. A. Detwiler , P. J. Doe , J. A. Dunmore , Yu. Efremenko , H. Ejiri , S. R. Elliott , J. E. Fast , P. Finnerty , F. M. Fraenkle , Z. Fu , B. K. Fujikawa , E. Fuller , A. Galindo-Uribarri , V. M. Gehman , T. Gilliss , G. K. Giovanetti , J. Goett , M. P. Green , J. Gruszko , I. S. Guinn , V. E. Guiseppe , A. L. Hallin , C. R. Haufe , L. Hehn , R. Henning , E. W. Hoppe , T. W. Hossbach , M. A. Howe , B. R. Jasinski , R. A. Johnson , K. J. Keeter , J. D. Kephart , M. F. Kidd , A. Knecht , S. I. Konovalov , R. T. Kouzes , K. T. Lesko , B. D. LaFerriere , J. Leon , L. E. Leviner , J. C. Loach , A. M. Lopez , P. N. Luke , J. MacMullin , S. MacMullin , M. G. Marino , R. D. Martin , R. Massarczyk , A. B. McDonald , D. -M. Mei , S. J. Meijer , J. H. Merriman , S. Mertens , H. S. Miley , M. L. Miller , J. Myslik , J. L. Orrell , C. O'Shaughnessy , G. Othman , N. R. Overman , W. Pettus , D. G. Phillips , A. W. P. Poon , G. Perumpilly , K. Pushkin , D. C. Radford , J. Rager , J. H. Reeves , A. L. Reine , K. Rielage , R. G. H. Robertson , M. C. Ronquest , N. W. Ruof , A. G. Schubert , B. Shanks , M. Shirchenko , K. J. Snavely , N. Snyder , D. Steele , A. M. Suriano , D. Tedeschi , W. Tornow , J. E. Trimble , R. L. Varner , S. Vasilyev , K. Vetter , K. Vorren , B. R. White , J. F. Wilkerson , C. Wiseman , W. Xu , E. Yakushev , H. Yaver , A. R. Young , C. -H. Yu , V. Yumatov , I. Zhitnikov , B. X. Zhu , S. Zimmermann

The development of the NEMO3 detector, which is now running in the Frejus Underground Laboratory (L.S.M. Laboratoire Souterrain de Modane), was begun more than ten years ago. The NEMO3 detector uses a tracking-calorimeter technique in order…

Instrumentation and Detectors · Physics 2009-09-29 the NEMO Collaboration , R. Arnold

Weak interaction in nuclei represents a well-known venue for testing many of the fundamental symmetries of the Standard Model. In particular, neutrinoless double-beta decay offers the possibility to test Beyond Standard Model theories…

High Energy Physics - Phenomenology · Physics 2017-10-03 Mihai Horoi , Andrei Neacsu

The objective of the Majorana Experiment is to study neutrinoless double beta decay (0nbb) with an effective Majorana-neutrino mass sensitivity below 50 meV in order to characterize the Majorana nature of the neutrino, the Majorana mass…

Nuclear Experiment · Physics 2012-08-27 The Majorana collaboration

Neutrinoless double beta decay is the most powerful tool to probe not only for Majorana neutrino masses but for lepton number violating physics in general. We discuss relations between lepton number violation, double beta decay and neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-11 Frank F. Deppisch , Martin Hirsch , Heinrich Päs

The CUORE experiment, a ton-scale cryogenic bolometer array, recently began operation at the Laboratori Nazionali del Gran Sasso in Italy. The array represents a significant advancement in this technology, and in this work we apply it for…

Nuclear Experiment · Physics 2018-04-03 CUORE Collaboration , C. Alduino , K. Alfonso , E. Andreotti , C. Arnaboldi , F. T. Avignone , O. Azzolini , I. Bandac , T. I. Banks , G. Bari , M. Barucci , J. W. Beeman , F. Bellini , G. Benato , A. Bersani , D. Biare , M. Biassoni , A. Branca , C. Brofferio , A. Bryant , A. Buccheri , C. Bucci , C. Bulfon , A. Camacho , A. Caminata , L. Canonica , X. G. Cao , S. Capelli , M. Capodiferro , L. Cappelli , L. Cardani , P. Carniti , M. Carrettoni , N. Casali , L. Cassina , G. Ceruti , A. Chiarini , D. Chiesa , N. Chott , M. Clemenza , S. Copello , C. Cosmelli , O. Cremonesi , C. Crescentini , R. J. Creswick , J. S. Cushman , A. D'Addabbo , D. D'Aguanno , I. Dafinei , C. J. Davis , F. Del Corso , S. Dell'Oro , M. M. Deninno , S. Di Domizio , M. L. Di Vacri , L. Di Paolo , A. Drobizhev , L. Ejzak , R. Faccini , D. Q. Fang , M. Faverzani , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , B. K. Fujikawa , A. Giachero , L. Gironi , A. Giuliani , L. Gladstone , J. Goett , P. Gorla , C. Gotti , C. Guandalini , M. Guerzoni , T. D. Gutierrez , E. E. Haller , K. Han , E. V. Hansen , K. M. Heeger , R. Hennings-Yeomans , K. P. Hickerson , H. Z. Huang , M. Iannone , R. Kadel , G. Keppel , L. Kogler , Yu. G. Kolomensky , A. Leder , C. Ligi , K. E. Lim , Y. G. Ma , C. Maiano , L. Marini , M. Martinez , C. Martinez Amaya , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , P. J. Mosteiro , S. S. Nagorny , T. Napolitano , M. Nastasi , C. Nones , E. B. Norman , V. Novati , A. Nucciotti , I. Nutini , T. O'Donnell , E. Olivieri , F. Orio , J. L. Ouellet , C. E. Pagliarone , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , A. Pelosi , G. Pessina , V. Pettinacci , G. Piperno , C. Pira , S. Pirro , S. Pozzi , E. Previtali , F. Reindl , F. Rimondi , L. Risegari , C. Rosenfeld , C. Rusconi , M. Sakai , E. Sala , C. Salvioni , S. Sangiorgio , D. Santone , D. Schaeffer , B. Schmidt , J. Schmidt , N. D. Scielzo , V. Singh , M. Sisti , A. R. Smith , F. Stivanello , L. Taffarello , M. Tenconi , F. Terranova , C. Tomei , G. Ventura , M. Vignati , S. L. Wagaarachchi , B. S. Wang , H. W. Wang , B. Welliver , J. Wilson , K. Wilson , L. A. Winslow , T. Wise , L. Zanotti , G. Q. Zhang , B. X. Zhu , S. Zimmermann , S. Zucchelli

Neutrino accompanied double beta-decay of Ge-76 can populate the ground state and the excited states of Se-76. While the decay to the ground state has been observed with a half-life of 1.74 +0.18 -0.16 10^21 years, decays to the excited…

Nuclear Experiment · Physics 2008-11-26 K. Kroeninger , L. Pandola , V. Tretyak

The purpose of the NEMO3 experiment is to detect neutrinoless double beta decay in order to determine the nature of neutrino and its absolute mass. We analysed the 389 effective days of data from the $\sim 7$ kg of $^{100}$Mo and $\sim 1$…

High Energy Physics - Experiment · Physics 2016-08-31 J. S Ricol

SNO+ will search for neutrinoless double beta decay by loading 780 tonnes of linear alkylbenzene liquid scintillator with O(tonne) of neodymium. Using natural Nd at 0.1% loading will provide 43.7 kg of 150Nd given its 5.6% abundance and…

Instrumentation and Detectors · Physics 2019-08-14 J. Hartnell

The recent neutrino oscillation experimental results indicate that at least one neutrino has a mass greater than 50 meV. The next generation of double-beta decay experiments will very likely have a sensitivity to an effective Majorana…

Nuclear Experiment · Physics 2011-07-19 Steven R. Elliott

There is a general consensus that detection of a double-beta decay without any neutrino involved would mark physics beyond the Standard Model. This is because in such decay modes lepton number conservation would be violated and the neutrino…

High Energy Physics - Experiment · Physics 2009-08-18 D. Frekers

The lepton number violating process of neutrinoless double-beta decay could result from the physics beyond the Standard Model needed to generate the neutrino masses. Taking different approaches, the current generation of $^{76}$Ge…

Instrumentation and Detectors · Physics 2019-08-14 Jordan Myslik

The SuperNEMO experiment will search for neutrinoless double-beta decay ($0\nu\beta\beta$), and study the Standard-Model double-beta decay process ($2\nu\beta\beta$). The SuperNEMO technology can measure the energy of each of the electrons…

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