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The ability of background discrimination using pulse shape discrimination (PSD) in broad-energy germanium (BEGe) detectors makes them as competitive candidates for neutrinoless double beta decay (0{\nu}\b{eta}\b{eta}) experiments. The…

Instrumentation and Detectors · Physics 2016-06-28 Zhi Zeng , Yu-Hao Mi , Ming Zeng , Hao Ma , Qian Yue , Jian-Ping Cheng , Jun-Li Li , Rui Qiu , Hui Zhang

The MAJORANA Collaboration is building the MAJORANA DEMONSTRATOR, a 60 kg array of high purity germanium detectors housed in an ultra-low background shield at the Sanford Underground Laboratory in Lead, SD. The MAJORANA DEMONSTRATOR will…

We decompose the neutrinoless double-beta decay matrix elements into sums of products over the intermediate nucleus with two less nucleons. We find that the sum is dominated by the J^pi=0^+ ground state of this intermediate nucleus for both…

Nuclear Theory · Physics 2015-06-23 B. A. Brown , M. Horoi , R. A. Sen'kov

The various mechanisms for neutrinoless double beta decay in gauge theories are reviewed and the present experimental data is used to set limits on physics scenarios beyond the standard model. The positive indications for nonzero neutrino…

High Energy Physics - Phenomenology · Physics 2007-05-23 Rabindra N. Mohapatra

We propose the construction of LEGEND-1000, the ton-scale Large Enriched Germanium Experiment for Neutrinoless $\beta \beta$ Decay. This international experiment is designed to answer one of the highest priority questions in fundamental…

Instrumentation and Detectors · Physics 2024-09-10 LEGEND Collaboration , N. Abgrall , I. Abt , M. Agostini , A. Alexander , C. Andreoiu , G. R. Araujo , F. T. Avignone , W. Bae , A. Bakalyarov , M. Balata , M. Bantel , I. Barabanov , A. S. Barabash , P. S. Barbeau , C. J. Barton , P. J. Barton , L. Baudis , C. Bauer , E. Bernieri , L. Bezrukov , K. H. Bhimani , V. Biancacci , E. Blalock , A. Bolozdynya , S. Borden , B. Bos , E. Bossio , A. Boston , V. Bothe , R. Bouabid , S. Boyd , R. Brugnera , N. Burlac , M. Busch , A. Caldwell , T. S. Caldwell , R. Carney , C. Cattadori , Y. -D. Chan , A. Chernogorov , C. D. Christofferson , P. -H. Chu , M. Clark , T. Cohen , D. Combs , T. Comellato , R. J. Cooper , I. A. Costa , V. D'Andrea , J. A. Detwiler , A. Di Giacinto , N. Di Marco , J. Dobson , A. Drobizhev , M. R. Durand , F. Edzards , Yu. Efremenko , S. R. Elliott , A. Engelhardt , L. Fajt , N. Faud , M. T. Febbraro , F. Ferella , D. E. Fields , F. Fischer , M. Fomina , H. Fox , J. Franchi , R. Gala , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , A. Geraci , C. Gilbert , M. Gold , C. Gooch , K. P. Gradwohl , M. P. Green , G. F. Grinyer , A. Grobov , J. Gruszko , I. Guinn , V. E. Guiseppe , V. Gurentsov , Y. Gurov , K. Gusev , B. Hacket , F. Hagemann , J. Hakenmüeller , M. Haranczyk , L. Hauertmann , C. R. Haufe , C. Hayward , B. Heffron , F. Henkes , R. Henning , D. Hervas Aguilar , J. Hinton , R. Hodak , H. Hoffmann , W. Hofmann , A. Hostiuc , J. Huang , M. Hult , M. Ibrahim Mirza , J. Jochum , R. Jones , D. Judson , M. Junker , J. Kaizer , V. Kazalov , Y. Kermaïdic , H. Khushbakht , M. Kidd , T. Kihm , K. Kilgus , I. Kim , A. Klimenko , K. T. Knöpfle , O. Kochetov , S. I. Konovalov , I. Kontul , K. Kool , L. L. Kormos , V. N. Kornoukhov , M. Korosec , P. Krause , V. V. Kuzminov , J. M. López-Castaño , K. Lang , M. Laubenstein , E. León , B. Lehnert , A. Leonhardt , A. Li , M. Lindner , I. Lippi , X. Liu , J. Liu , D. Loomba , A. Lubashevskiy , B. Lubsandorzhiev , N. Lusardi , Y. Müller , M. Macko , C. Macolino , B. Majorovits , F. Mamedov , W. Maneschg , L. Manzanillas , G. Marshall , R. D. Martin , E. L. Martin , R. Massarczyk , D. Mei , S. J. Meijer , S. Mertens , M. Misiaszek , E. Mondragon , M. Morella , B. Morgan , T. Mroz , D. Muenstermann , C. J. Nave , I. Nemchenok , M. Neuberger , T. K. Oli , G. Orebi Gann , G. Othman , V. Palušova , R. Panth , L. Papp , L. S. Paudel , K. Pelczar , J. Perez Perez , L. Pertoldi , W. Pettus , P. Piseri , A. W. P. Poon , P. Povinec , A. Pullia , D. C. Radford , Y. A. Ramachers , C. Ransom , L. Rauscher , M. Redchuk , A. L. Reine , S. Riboldi , K. Rielage , S. Rozov , E. Rukhadze , N. Rumyantseva , J. Runge , N. W. Ruof , R. Saakyan , S. Sailer , G. Salamanna , F. Salamida , D. J. Salvat , V. Sandukovsky , S. Schönert , A. Schültz , M. Schütt , D. C. Schaper , J. Schreiner , O. Schulz , M. Schuster , M. Schwarz , B. Schwingenheuer , O. Selivanenko , M. Shafiee , E. Shevchik , M. Shirchenko , Y. Shitov , H. Simgen , F. Simkovic , M. Skorokhvatov , M. Slavickova , K. Smolek , A. Smolnikov , J. A. Solomon , G. Song , K. Starosta , I. Stekl , M. Stommel , D. Stukov , R. R. Sumathi , D. A. Sweigart , K. Szczepaniec , L. Taffarello , D. Tagnani , R. Tayloe , D. Tedeschi , M. Turqueti , R. L. Varner , S. Vasilyev , A. Veresnikova , K. Vetter , C. Vignoli , C. Vogl , K. von Sturm , D. Waters , J. C. Waters , W. Wei , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , V. H. -S. Wu , W. Xu , E. Yakushev , T. Ye , C. -H. Yu , V. Yumatov , N. Zaretski , J. Zeman , I. Zhitnikov , D. Zinatulina , A. -K. Zschocke , A. J. Zsigmond , K. Zuber , G. Zuzel

High purity germanium (HPGe) crystals will be used for the MAJORANA DEMONSTRATOR, where they serve as both the source and the detector for neutrinoless double beta decay. It is crucial for the experiment to understand the performance of the…

We report a novel correlated background in the antineutrino detection using the inverse beta decay reaction. Spontaneous fissions and $(\alpha,n)$ reactions in peripheral materials of the antineutrino detector, such as borosilicate glass of…

Instrumentation and Detectors · Physics 2021-12-01 Zhiyuan Chen , Xin Zhang , Zeyuan Yu , Jun Cao , Changgen Yang

A new design of a cryogenic germanium detector for dark matter search is presented, taking advantage of the coplanar grid technique of event localisation for improved background discrimination. Experiments performed with prototype devices…

GALATEA is a test facility designed to investigate bulk and surface effects in high purity germanium detectors. A vacuum tank houses an infrared screened volume with a cooled detector inside. A system of three stages allows an almost…

Instrumentation and Detectors · Physics 2015-12-09 I. Abt , A. Caldwell , B. Doenmez , L. Garbini , S. Irlbeck , B. Majorovits , M. Palermo , O. Schulz , H. Seitz , F. Stelzer

The existing calculations of the nuclear matrix elements of the neutrinoless double beta-decay differ by about a factor three. This uncertainty prevents quantative interpretation of the results of experiments searching for this process. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Bilenky , J. A. Grifols

An extremely low-background environment is a crucial requirement for any neutrinoless double beta decay experiment. Neutrons are very difficult to stop, because they can pass through the shields and activate nuclei in the detector, even…

Instrumentation and Detectors · Physics 2023-07-25 Qianming Wang , Zeyu Huang , Pengchong Hu , Emilio Ciuffoli

The Advanced Molybdenum-based Rare process Experiment in its second phase (AMoRE-II) will search for neutrinoless double-beta (0{\nu}\b{eta}\b{eta}) decay of 100Mo in 200 kg of molybdate crystals. To achieve the zero-background level in the…

Instrumentation and Detectors · Physics 2021-02-03 S. Y. Park , K. I. Hahn , W. G. Kang , V. Kazalov , G. W. Kim , Y. D. Kim , E. K. Lee , M. H. Lee , D. S. Leonard

The MAJORANA DEMONSTRATOR recently concluded its search for neutrinoless double-beta decay. The experiment operated an array of up to 40.4 kg of germanium detectors, 27 kg of which were isotopically enriched in 76Ge and housed inside a…

Nuclear Experiment · Physics 2024-01-11 David J. Tedeschi

Neutrinoless double-beta decay of nuclei represents one of the most promising methods for uncovering physics beyond the Standard Model. In this context, $^{76}$Ge stands out as a particularly attractive candidate, as it can serve as an…

Low counting experiments (search for double $\beta$ decay and dark matter particles, measurements of neutrino fluxes from different sources, search for hypothetical nuclear and subnuclear processes, low background $\alpha$, $\beta$,…

Instrumentation and Detectors · Physics 2020-01-20 F. A. Danevich , V. I. Tretyak

We investigated charge transport in an n-type germanium detector at 5.2 K to explore new technology for enhancing low-mass dark matter detection sensitivity. Calculations of dipole and cluster dipole state binding energies and electric…

Instrumentation and Detectors · Physics 2023-02-17 Sanjay Bhattarai , Dongming Mei , Rajendra Panth , Mathbar Raut , Kyler Kooi , Hao Mei , Guojian Wang

The Karlsruhe Tritium Neutrino (KATRIN) experiment investigating tritium beta-decay close to the endpoint with unprecedented precision has stringent requirements on the background level of less than 10^(-2) counts per second. Electron…

Instrumentation and Detectors · Physics 2015-06-15 N. Wandkowsky , G. Drexlin , F. M. Fränkle , F. Glück , S. Groh , S. Mertens

The next generation of double-beta decay experiments have an excellent chance of providing data on the neutrino mass pattern. This presentation is a summary of what is currently known about the mass pattern and expectations from experiment.…

Nuclear Experiment · Physics 2015-06-26 Steven R. Elliott