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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

Experiments to search for neutrinoless double-beta (0{\nu}\b{eta}\b{eta}) decay of 76Ge using a high-purity germanium (HPGe) detector rely heavily on background suppression technologies to enhance their sensitivities. In this work, we…

Instrumentation and Detectors · Physics 2023-05-31 Jingzhe Yang , Yang Tian , Wenhan Dai , Mingxin Yang , Lin Jiang , Jinjun Wen , Tao Xue , Ming Zeng , Zhi Zeng , Yulan Li

GERDA, the GERmanium Detector Array experiment, is a new double beta-decay experiment which is currently under construction in the INFN National Gran Sasso Laboratory (LNGS), Italy. It is implementing a new shielding concept by operating…

High Energy Physics - Experiment · Physics 2008-10-17 Karl-Tasso Knoepfle

We review current experimental efforts to search for neutrinoless double beta decay (0$\nu\beta\beta$). A description of the selected leading experiments is given and the strongest recent results are compared in terms of achieved background…

High Energy Physics - Experiment · Physics 2016-06-29 Igor Ostrovskiy , Kevin O'Sullivan

The NEXT-100 detector will search for the neutrinoless double beta decay of $^{136}$Xe using an electroluminescent high-pressure xenon gas TPC filled with 100 kg of enriched Xe. An observation of this hypothetical process would establish a…

Instrumentation and Detectors · Physics 2019-08-13 D. Lorca

An infrastructure to characterize germanium detectors has been designed and constructed at the HADES Underground Research Laboratory, located in Mol (Belgium). Thanks to the 223m overburden of clay and sand, the muon flux is lowered by four…

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

To measure the main characteristics of radiative neutron decay, namely its relative intensity BR (branching ratio), it is necessary to measure the spectra of double coincidences between beta-electron and proton as well as the spectra of…

The motivation, present status, and future plans of the search for the neutrinoless double beta decay are reviewed. It is argued that, motivated by the recent observations of neutrino oscillations, there is a reasonable hope that…

High Energy Physics - Phenomenology · Physics 2011-07-19 Steven R. Elliott , Petr Vogel

Diverse searches for direct dark matter (DM) in effective electromagnetic and leptophilic interactions resulting from new physics, as well as Weakly Interacting Massive Particles (WIMPs) with unconventional electronic recoils, are…

The success of current and future-generation neutrinoless double beta decay experiments relies on the ability to eliminate or reduce extraneous backgrounds. In addition to constructing experiments using radiopure materials and handling in…

Instrumentation and Detectors · Physics 2026-02-09 G. Othman , C. Wiseman , T. H. Burritt , J. A. Detwiler , M. P. Held , R. Henning , T. Mathew , D. Peterson , W. Pettus , G. Song , T. D. Van Wechel

Neutrinoless double beta decay ($0\nu\beta\beta$) offers a sensitive probe of neutrino mass and its Majorana nature. Orthogonal-strip high-purity germanium (HPGe) detectors with high spatial resolution provide a promising approach for…

Instrumentation and Detectors · Physics 2026-03-03 Qiuli Zhang , Wenhan Dai , Peng Zhang , Mingxin Yang , Yang Tian , Zhi Zeng , Yulan Li , Ming Zeng , Hao Ma , Jianping Cheng

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

In searching for the neutrinoless double-beta decay of $^{76}$Ge the GERmanium Detector Array (GERDA) experiment at the INFN Laboratori Nazionali del Gran Sasso has achieved an unprecedented low background of well below 10$^{-3}$…

Instrumentation and Detectors · Physics 2022-03-02 K. T. Knöpfle , B. Schwingenheuer

Recent progress on the development of very low noise high purity germanium ionization spectrometers has produced an instrument of 1.2 kg mass and excellent noise performance. The detector was installed in a low-background cryostat intended…

Tagging barium ions in double beta decay experiments involving $^{136}$Xe offers a promising pathway to achieving an almost background-free environment, which is essential for addressing key unresolved questions in neutrino physics, such as…

Atomic Physics · Physics 2025-01-16 Álvaro Peralta Conde

SuperNEMO is a next generation neutrinoless double beta decay experiment with a design capability to reach a half-life sensitivity of $10^{26}$ years corresponding to an effective Majorana neutrino mass of $\langle m_{\beta\beta} \rangle$…

Instrumentation and Detectors · Physics 2015-05-01 Xin Ran Liu

A study on cosmogenic activation in germanium was carried out to evaluate the cosmogenic background level of natural and $^{70}$Ge depleted germanium detectors. The production rates of long-lived radionuclides were calculated with Geant4…

Instrumentation and Detectors · Physics 2018-10-23 J. L. Ma , Q. Yue , S. T. Lin , H. T. Wong , J. W. Hu , L. P. Jia , H. Jiang , J. Li , S. K. Liu , Z. Z. Liu , H. Ma , W. Y. Tang , Y. Tian , L. Wang , Q. Wang , L. T. Yang , Z. Zeng

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

Spectroscopic studies of two beta-rays from 100Mo are shown to be of potential interest for investigating both the Majorana neutrino mass by neutrinoless double beta-decay and low energy solar neutrino's by inverse beta-decay. With a…

Nuclear Experiment · Physics 2009-10-31 H. Ejiri , J. Engel , R. Hazama , P. Krastev , N. Kudomi , R. G. H. Robertson