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The GEM project is designed for the next generation 2 beta decay experiments with 76-Ge. One ton of ''naked'' HP Ge detectors (natural at the first GEM-I phase and enriched in 76-Ge to 86% at the second GEM-II stage) are operating in…

Nuclear Experiment · Physics 2008-11-26 Yu. G. Zdesenko , O. A. Ponkratenko , V. I. Tretyak

The {\sc Majorana} collaboration is searching for neutrinoless double beta decay using $^{76}$Ge, which has been shown to have a number of advantages in terms of sensitivities and backgrounds. The observation of neutrinoless double-beta…

Neutrinoless double beta decay ($0\nu\beta\beta$) is one of the most sensitive approaches to test particle physics beyond the standard model. During the last years, besides the most restrictive limit on the effective Majorana neutrino mass,…

High Energy Physics - Phenomenology · Physics 2015-06-25 H. Päs

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 progress in the development of the new international Gerda (GErmanium Detector Array) experiment is presented. Main purpose of the experiment is to search for the neutrinoless double beta decay of 76Ge. The experimental set up is under…

Nuclear Experiment · Physics 2019-08-13 Anatoly A. Smolnikov

The observation of neutrinoless double-beta decay (0${\nu}{\beta}{\beta}$) would show that lepton number is violated, reveal that neutrinos are Majorana particles, and provide information on neutrino mass. A discovery-capable experiment…

Instrumentation and Detectors · Physics 2018-06-15 LEGEND Collaboration , N. Abgrall , A. Abramov , N. Abrosimov , I. Abt , M. Agostini , M. Agartioglu , A. Ajjaq , S. I. Alvis , F. T. Avignone , X. Bai , M. Balata , I. Barabanov , A. S. Barabash , P. J. Barton , L. Baudis , L. Bezrukov , T. Bode , A. Bolozdynya , D. Borowicz , A. Boston , H. Boston , S. T. P. Boyd , R. Breier , V. Brudanin , R. Brugnera , M. Busch , M. Buuck , A. Caldwell , T. S. Caldwell , T. Camellato , M. Carpenter , C. Cattadori , J. Cederkäll , Y. -D. Chan , S. Chen , A. Chernogorov , C. D. Christofferson , P. -H. Chu , R. J. Cooper , C. Cuesta , E. V. Demidova , Z. Deng , M. Deniz , J. A. Detwiler , N. Di Marco , A. Domula , Q. Du , Yu. Efremenko , V. Egorov , S. R. Elliott , D. Fields , F. Fischer , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , T. Gilliss , M. Giordano , G. K. Giovanetti , M. Gold , P. Golubev , C. Gooch , P. Grabmayr , M. P. Green , J. Gruszko , I. S. Guinn , V. E. Guiseppe , V. Gurentsov , Y. Gurov , K. Gusev , J. Hakenmüeller , L. Harkness-Brennan , Z. R. Harvey , C. R. Haufe , L. Hauertmann , D. Heglund , L. Hehn , A. Heinz , R. Hiller , J. Hinton , R. Hodak , W. Hofmann , S. Howard , M. A. Howe , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , R. Janssens , M. Ješkovský , J. Jochum , H. T. Johansson , D. Judson , M. Junker , J. Kaizer , K. Kang , V. Kazalov , Y. Kermaïdic , F. Kiessling , A. Kirsch , A. Kish , A. Klimenko , K. T. K. T. Knöpfle , O. Kochetov , S. I. Konovalov , I. Kontul , V. N. Kornoukhov , T. Kraetzschmar , K. Kröninger , A. Kumar , V. V. Kuzminov , K. Lang , M. Laubenstein , A. Lazzaro , Y. L. Li , Y. -Y. Li , H. B. Li , S. T. Lin , M. Lindner , I. Lippi , S. K. Liu , X. Liu , J. Liu , D. Loomba , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , H. Ma , B. Majorovits , F. Mamedov , R. D. Martin , R. Massarczyk , J. A. J. Matthews , N. McFadden , D. -M. Mei , H. Mei , S. J. Meijer , D. Mengoni , S. Mertens , W. Miller , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , J. Myslik , I. Nemchenok , T. Nilsson , P. Nolan , C. O'Shaughnessy , G. Othman , K. Panas , L. Pandola , L. Papp , K. Pelczar , D. Peterson , W. Pettus , A. W. P. Poon , P. P. Povinec , A. Pullia , X. C. Quintana , D. C. Radford , J. Rager , C. Ransom , F. Recchia , A. L. Reine , S. Riboldi , K. Rielage , S. Rozov , N. W. Rouf , E. Rukhadze , N. Rumyantseva , R. Saakyan , E. Sala , F. Salamida , V. Sandukovsky , G. Savard , S. Schönert , A. -K. Schütz , O. Schulz , M. Schuster , B. Schwingenheuer , O. Selivanenko , B. Sevda , B. Shanks , E. Shevchik , M. Shirchenko , F. Simkovic , L. Singh , V. Singh , M. Skorokhvatov , K. Smolek , A. Smolnikov , A. Sonay , M. Spavorova , I. Stekl , D. Stukov , D. Tedeschi , J. Thompson , T. Van Wechel , R. L. Varner , A. A. Vasenko , S. Vasilyev , A. Veresnikova , K. Vetter , K. von Sturm , K. Vorren , M. Wagner , G. -J. Wang , D. Waters , W. -Z. Wei , T. Wester , B. R. White , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , H. T. Wong , J. Wyenberg , W. Xu , E. Yakushev , G. Yang , C. -H. Yu , Q. Yue , V. Yumatov , J. Zeman , Z. Zeng , I. Zhitnikov , B. Zhu , D. Zinatulina , A. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

Germanium detectors have very good capabilities for the investigation of rare phenomena like the neutrinoless double beta decay. Rejection of the background entangling the expected signal is one primary goal in this kind of experiments.…

Nuclear Experiment · Physics 2008-11-26 H. Gómez , S. Cebrián , J. Morales , J. A. Villar

In the global landscape of neutrinoless double beta ($0\nu\beta\beta$) decay search, the use of semiconductor germanium detectors provides many advantages. The excellent energy resolution, the negligible intrinsic radioactive contamination,…

High Energy Physics - Experiment · Physics 2021-09-17 V. D'Andrea , N. Di Marco , M. B. Junker , M. Laubenstein , C. Macolino , M. Morella , F. Salamida , C. Vignoli

The search for neutrinoless double beta ($0\nu\beta\beta$) decay is the best way to test lepton number violation and Majorana nature of neutrinos. One of the most promising techniques to discover $0\nu\beta\beta$ decay is by operating…

High Energy Physics - Experiment · Physics 2019-05-17 V. D'Andrea

Neutrinoless double beta decay searches play a major role in determining neutrino properties, in particular the Majorana or Dirac nature of the neutrino and the absolute scale of the neutrino mass. The consequences of these searches go…

The GERmanium Detector Array (GERDA) experiment located at the INFN Gran Sasso Laboratory (Italy), is looking for the neutrinoless double beta decay of Ge76, by using high-purity germanium detectors made from isotopically enriched material.…

Nuclear Experiment · Physics 2020-02-12 GERDA Collaboration , M. Agostini , A. M. Bakalyarov , M. Balata , I. Barabanov , L. Baudis , C. Bauer , E. Bellotti , S. Belogurov , A. Bettini , L. Bezrukov , T. Bode , V. Brudanin , R. Brugnera , A. Caldwell , C. Cattadori , A. Chernogorov , V. D'Andrea , E. V. Demidova , N. Di Marco , A. Domula , E. Doroshkevich , V. Egorov , R. Falkenstein , A. Gangapshev , A. Garfagnini , C. Gooch , P. Grabmayr , V. Gurentsov , K. Gusev , J. Hakenmüller , A. Hegai , M. Heisel , S. Hemmer , R. Hiller , W. Hofmann , M. Hult , L. V. Inzhechik , J. Janicskó Csáthy , J. Jochum , M. Junker , V. Kazalov , Y. Kermaidic , 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 , M. Lindner , I. Lippi , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , B. Majorovits , W. Maneschg , M. Miloradovic , R. Mingazheva , M. Misiaszek , P. Moseev , I. Nemchenok , K. Panas , L. Pandola , A. Pullia , C. Ransom , S. Riboldi , N. Rumyantseva , C. Sada , F. Salamida , C. Schmitt , B. Schneider , J. Schreiner , O. Schulz , B. Schwingenheuer , S. Schönert , A-K. Schütz , O. Selivanenko , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , L. Vanhoefer , A. A. Vasenko , A. Veresnikova , K. von Sturm , V. Wagner , A. Wegmann , T. Wester , C. Wiesinger , M. Wojcik , E. Yanovich , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , A. J. Zsigmond , K. Zuber , G. Zuzel

Neutrinoless double-beta decay searches play a major role in determining the nature of neutrinos, the existence of a lepton violating process, and the effective Majorana neutrino mass. The Majorana Collaboration proposes to assemble an…

Nuclear Experiment · Physics 2019-08-13 V. E. Guiseppe

High Purity Germanium Detectors have excellent energy resolution; the best among the technologies used in double beta decay. Since neutrino-less double beta decay hinges on the search for a rare peak upon a background continuum, this…

Nuclear Experiment · Physics 2019-04-19 Frank T. Avignone , Steven R. Elliott

After nearly 80 years since the first guess on its existence, neutrino still escapes our insight: the mass and the true nature (Majorana or Dirac) of this particle is still unknown. In the past ten years, neutrino oscillation experiments…

Instrumentation and Detectors · Physics 2013-12-17 O. Cremonesi , M. Pavan

Recent results of the Heidelberg-Moscow double beta decay experiment are presented. After 8.6 kg$\cdot$a of measuring time no signal is seen for the neutrinoless decay mode. A half-life limit of $T_{1/2}^{0\nu\beta\beta} > 5.1\cdot…

High Energy Physics - Experiment · Physics 2016-08-31 Heidelberg-Moscow-Collaboration

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

The GERmanium Detector Array GERDA experiment, located at the Laboratori Nazionali del Gran Sasso (LNGS) of INFN, searches for $0\nu\beta\beta$ of $^{76}$Ge. Germanium diodes enriched to $\sim 86~\%$ in the double beta emitter $^{76}$Ge…

Instrumentation and Detectors · Physics 2019-08-13 Valerio D'Andrea

The search for neutrinoless double-beta decay is the most sensitive technique to establish the Majorana nature of neutrinos. Two operating experiments that look for such decays in $^{76}$Ge -- GERDA and the MAJORANA DEMONSTRATOR -- have…

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

Indirect support for the evidence of neutrinoless double beta decay reported recently, is obtained by analysis of other Ge double beta experiments, which yield independent information on the background in the region of Q_(beta-beta). Some…

High Energy Physics - Phenomenology · Physics 2015-06-25 H. V. Klapdor-Kleingrothaus , A. Dietz , I. V. Krivosheina , Ch. Doerr , C. Tomei

The most stringent constraint on the so-called effective electron neutrino mass from the present neutrinoless double beta decay experiments is |M_{ee}| < 0.2 eV, while the planned next generation experiment GENIUS is anticipated to reach a…

High Energy Physics - Phenomenology · Physics 2009-10-31 Anna Kalliomaki , Jukka Maalampi