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A high pressure xenon gas time projection chamber with electroluminescent amplification (EL HPGXe TPC) searching for the neutrinoless double beta ($0\nu\beta\beta$) decay offers: excellent energy resolution ($0.5-0.7\%$ FWHM at the…

Instrumentation and Detectors · Physics 2017-10-11 N. Lopez-March

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

Background: Time-reversal-invariance violation, or equivalently CP violation, may explain the observed cosmological baryon asymmetry as well as signal physics beyond the Standard Model. In the decay of polarized neutrons, the triple…

Neutrinoless double-$\beta$ decay ($0\nu\beta\beta$ decay) is a hypothetical process that can occur if the neutrino is its own antiparticle. The COBRA collaboration operates a demonstrator to search for these decays at the Laboratori…

A search for double beta decays of $^{110}$Pd and $^{102}$Pd into excited states of the daughter nuclides has been performed using three ultra-low background gamma-spectrometry measurements in the Felsenkeller laboratory, Germany, the HADES…

Nuclear Experiment · Physics 2016-11-23 B. Lehnert , E. Andreotti , D. Degering , M. Hult , M. Laubenstein , T. Wester , K. Zuber

Scintillator detectors can be used in experiments searching for neutrinoless double beta decay. A wide variety of double beta decay candidate isotopes can be made into scintillators or can be loaded into scintillators. Experimental programs…

Instrumentation and Detectors · Physics 2008-12-18 Mark C. Chen

We present a technique for estimating the number of future neutrinoless double-beta decay results using several distinct nuclei to optimize the physics reach of upcoming experiments. We use presently available matrix element calculations…

High Energy Physics - Phenomenology · Physics 2008-11-26 V. M. Gehman , S. R. Elliott

The double beta decay study of 160-Gd has been performed in the Solotvina Underground Laboratory with the help of Gd_2SiO_5(Ce) crystal scintillator (volume 95 cc). The background of the detector in the vicinity of the 2 beta energy of…

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

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

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 study of the neutrinoless double beta ($0 \beta\beta$) decay mode can provide us with important information on the neutrino properties, particularly on the electron neutrino absolute mass. In this work we revise the present constraints…

Nuclear Theory · Physics 2016-11-25 Sabin Stoica , Andrei Neacsu

Nuclear double beta decay provides an extraordinarily broad potential to search for beyond Standard Model physics, probing already now the TeV scale, on which new physics should manifest itself. These possibilities are reviewed here. First,…

High Energy Physics - Experiment · Physics 2007-05-23 H. V. Klapdor-Kleingrothaus

The GERDA experiment located at the LNGS searches for neutrinoless double beta (0\nu\beta\beta) decay of ^{76}Ge using germanium diodes as source and detector. In Phase I of the experiment eight semi-coaxial and five BEGe type detectors…

Instrumentation and Detectors · Physics 2013-12-09 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. Budjáš , 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. Janicskó Csáthy , J. Jochum , M. Junker , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Klimenko , 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 , X. Liu , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , A. A. Machado , B. Majorovits , W. Maneschg , M. Misiaszek , I. Nemchenok , S. Nisi , C. O'Shaughnessy , L. Pandola , K. Pelczar , G. Pessina , A. Pullia , S. Riboldi , N. Rumyantseva , C. Sada , M. Salathe , C. Schmitt , J. Schreiner , O. Schulz , B. Schwingenheuer , S. Schönert , 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

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

We discuss a consistency test which makes it possible to discriminate unknown nuclear background lines from neutrinoless double beta decay with only one isotope. By considering both the transition to the ground state and to the first…

High Energy Physics - Phenomenology · Physics 2011-11-18 Michael Duerr , Manfred Lindner , Kai Zuber

Solar neutrinos interact within double-beta decay (\BB) detectors and contribute to backgrounds for \BB\ experiments. Background contributions due to charge-current solar neutrino interactions with \BB\ nuclei of $^{76}$Ge, $^{82}$Se,…

Nuclear Experiment · Physics 2017-10-25 S. R. Elliott , H. Ejiri

We consider the interpretation of the MiniBooNE low-energy anomaly and the Gallium radioactive source experiments anomaly in terms of short-baseline electron neutrino disappearance in the framework of 3+1 four-neutrino mixing schemes. The…

High Energy Physics - Phenomenology · Physics 2010-10-12 Carlo Giunti , Marco Laveder

Neutrinoless double beta decay (\( 0 \nu \beta \beta \)) is a hypothetical nuclear decay mode with important implications. In particular, observation of this decay would demonstrate that the neutrino is a Majorana particle and that lepton…

High Energy Physics - Lattice · Physics 2020-04-17 W. Detmold , D. J. Murphy

It is important to identify and reduce the gamma radiation which can be a significant source of background for any double beta decay experiment. The TIN.TIN detector array, which is under development for the search of Neutrinoless Double…

Instrumentation and Detectors · Physics 2015-08-03 V. Singh , N. Dokania , S. Mathimalar , V. Nanal , R. G. Pillay

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
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