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Neutrinoless double-beta decay ($0\nu\beta\beta$) is a rare nuclear process that, if observed, will provide insight into the nature of neutrinos and help explain the matter-antimatter asymmetry in the universe. The Large Enriched Germanium…

Data Analysis, Statistics and Probability · Physics 2025-04-22 E. León , A. Li , M. A. Bahena Schott , B. Bos , M. Busch , J. R. Chapman , G. L. Duran , J. Gruszko , R. Henning , E. L. Martin , J. F. Wilkerson

Neutrinoless double-beta decay($0\nu\beta\beta$) decay is a hypothetical process that violates lepton number, and whose observation would unambiguously indicate that neutrinos are Majorana fermions. In the standard inverted-ordering…

Nuclear Experiment · Physics 2019-12-10 I. S. Guinn , J. M. López-Castaño

LEGEND (Large Enriched Germanium Experiment for Neutrinoless Double-Beta Decay) is a ton-scale experimental program to search for neutrinoless double beta ($0 \nu \beta \beta$) decay using high-purity germanium detectors enriched in the…

Instrumentation and Detectors · Physics 2019-11-15 Michael Willers

Particle tracks and differential energy loss measured in high pressure gaseous detectors can be exploited for event identification in neutrinoless double beta decay~($0\nu \beta \beta$) searches. We develop a new method based on Kalman…

Instrumentation and Detectors · Physics 2021-07-07 Tao Li , Shaobo Wang , Yu Chen , Ke Han , Heng Lin , Kaixiang Ni , Wei Wang , Yiliu Xu , Anni Zou

This paper describes the energy scale procedures and germanium detectors performance in the LEGEND-200 experiment, a critical component for the first unblinding in the search for neutrinoless double beta decay. We detail the digital signal…

Instrumentation and Detectors · Physics 2026-05-25 The LEGEND Collaboration , H. Acharya , M. Agostini , A. Alexander , C. Alvarez-Garcia , V. Aures , F. T. Avignone , M. Babicz , W. Bae , M. Balata , A. S. Barabash , P. S. Barbeau , C. J. Barton , L. Baudis , C. Bauer , S. Bellman , E. Bernieri , J. P. Ulloa Beteta , L. Bezrukov , K. H. Bhimani , V. Biancacci , A. Biondi , R. Biondi , E. Blalock , P. Bongratz , S. J. Borden , G. Borghi , F. Borra , B. Bos , A. Boston , G. Botogoske , R. Bouabid , R. Brugnera , T. Bürger , N. Burlac , M. Busch , S. Calgaro , N. Canci , L. Canonica , S. Capra , M. Carminati , R. M. D. Carney , L. Carroll , C. Cattadori , R. Cesarano , Y. -D. Chan , J. R. Chapman , A. Chernogorov , P. -J. Chiu , O. Chkvorets , C. D. Christofferson , A. I. Colon-Rivera , F. Confortini , D. D'Agostino , V. D'Andrea , G. De Gregorio , R. Deckert , J. A. Detwiler , N. Di Marco , F. Di Capua , C. Di Fraia , A. Di Giacinto , D. Di Leo , T. Dixon , K. -M. Dong , A. Drobizhev , G. Duran , Yu. Efremenko , S. R. Elliott , T. Elmikawy , C. H. J. Emmanuel , E. Engelhardt , E. Esch , L. Favilla , M. Febbraro , F. Ferella , R. Feriozzi , D. E. Fields , C. Fiorini , M. Fomina , N. Fuad , R. Gala , A. Galindo-Uribarri , A. Gangapshev , A. Garfagnini , S. Gazzana , A. Geraci , L. Gessler , C. Ghiano , A. Gieb , S. Giri , A. Gogosha , M. Gold , M. P. Green , G. Grünauer , J. Gruszko , I. Guinn , V. E. Guiseppe , Y. Gurov , K. Gusev , B. Hackett , F. Hagemann , M. Haranczyk , F. Henkes , R. Henning , J. Herrera , D. Hervas Aguilar , J. Hinton , R. Hodák , H. F. R. Hoffmann , M. Huber , M. Hult , A. Iorio , U. T. Islek , A. Jany , J. Jochum , D. S. Judson , M. Junker , J. Kaizer , V. Kazalov , M. F. Kidd , T. Kihm , K. Kilgus , A. Klimenko , K. T. Knöpfle , I. Kochanek , O. Kochetov , I. Kontul , V. N. Kornoukhov , A. B. Kowaleswska , P. Krause , H. Krishnamoorthy , V. V. Kuzminov , K. Lang , M. Laubenstein , N. N. P. N. Lay , A. Leder , B. Lehnert , A. Leonhardt , N. Levashko , A. Li , L. Y. Li , Y. -R. Lin , I. Lippi , A. Love , A. Lubashevskiy , B. Lubsandorzhiev , N. Lusardi , B. Majorovits , F. Mamedov , G. G. Marshall , E. L. Martin , R. D. Martin , R. Massarczyk , A. Mazumdar , G. McDowell , D. -M. Mei , M. Menzel , S. Mertens , E. Miller , I. Mirza , M. Misiaszek , M. Morella , B. Morgan , D. Muenstermann , C. J. Nave , M. Neuberger , N. O'Briant , F. Paissan , L. Papp , K. Pelczar , L. Pertoldi , W. Pettus , F. Piastra , M. Pichotta , P. Piseri , A. W. P. Poon , P. P. Povinec , A. Pullia , W. S. Quinn , D. C. Radford , Y. A. Ramachers , A. L. Reine , S. Riboldi , E. Richards , K. Rielage , C. Romo-Luque , B. Rossi , N. Rossi , S. Rozov , N. Rumyantseva , R. Saakyan , S. Sailer , G. Salamanna , F. Salamida , G. Saleh , E. Sanchez Garcia , C. Savarese , D. C. Schaper , J. Schlegel , S. J. Schleich , L. Schlüter , S. Schönert , O. Schulz , A. -K. Schütz , M. Schwarz , M. Schweizer , B. Schwingenheuer , C. Seibt , G. Senatore , A. Serafini , K. Shakhov , E. Shevchik , H. Shi , M. Shirchenko , Y. Shitov , N. Sierig , H. Simgen , F. Šimkovic , S. Simonaitis-Boyd , M. Singh , M. Skorokhvatov , M. Slavíčková , J. A. Solomon , G. Song , A. C. Sousa , A. R. Sreekala , L. Steinhart , I. Štekl , T. Sterr , M. Stommel , R. Stroili , S. A. Sullivan , R. R. Sumathi , K. Szczepaniec , L. Taffarello , D. Tagnani , V. Tretyak , M. Turqueti , E. E. van Nieuwenhuizen , L. J. Varriano , S. Vasilyev , V. Vatsa , C. Vignoli , C. Vogl , I. Wang , A. Warren , J. N. Warren , D. Waters , S. L. Watkins , C. Wiesinger , J. F. Wilkerson , M. Willers , M. Wojcik , D. Xu , E. Yakushev , T. Ye , C. -H. Yu , V. Yumatov , D. Zinatulina , K. Zuber , G. Zuzel

The neutrinoless double beta (0nubb) decay experiment GERDA at the LNGS of INFN has started physics data taking in November 2011. This paper presents an analysis aimed at understanding and modeling the observed background energy spectrum,…

Data Analysis, Statistics and Probability · Physics 2019-08-13 N. Becerici-Schmidt

Measurements with a bare p-type high purity germanium diode (HPGe) submerged in a 19 kg liquid argon (LAr) scintillation detector at MPIK Heidelberg are reported. The liquid argon--germanium system (LArGe) is operated as a 4$\pi$…

Instrumentation and Detectors · Physics 2008-11-26 M. Di Marco , P. Peiffer , S. Schönert

Neutrinoless double beta decay would be a key to understanding the nature of neutrino masses. The next generation of High Purity Germanium experiments will have to be operated with a background rate of better than 10^-5 counts/(kg y keV) in…

Instrumentation and Detectors · Physics 2011-05-19 B. Majorovits , I. Abt , M. Laubenstein , O. Volynets

In the present work, we describe the results obtained with a large ($\approx 133$ cm$^3$) TeO$_2$ bolometer, with a view to a search for neutrinoless double-beta decay ($0\nu\beta\beta$) of $^{130}$Te. We demonstrate an efficient $\alpha$…

A series of test experiments on three different Si-based neutron detectors, namely a 1-d 128 channel, 0.5 mm space resolution Si microstrip sensor coupled to natural Gd converter, a medium size ? 1 cm2 PIN diode coupled to nGd2O3 or…

Instrumentation and Detectors · Physics 2018-05-04 G. Mauri , M. Mariotti , F. Casinini , F. Sacchetti , C. Petrillo

Low background experiments need a suppression of cosmogenically induced events. The GERDA experiment located at LNGS is searching for the neutrinless double beta decay of $^{76}$Ge. It is equipped with an active muon veto the main part of…

A software package for modeling segmented High-Purity Segmented Germanium detectors, AGATAGeFEM, is presented. The choices made for geometry implementation and the calculations of the electric and weighting fields are discussed. Models used…

Instrumentation and Detectors · Physics 2021-07-07 J. Ljungvall

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

A new type of radiation detector, a p-type modified electrode germanium diode, is presented. The prototype displays, for the first time, a combination of features (mass, energy threshold and background expectation) required for a…

Nuclear Experiment · Physics 2011-05-12 P. S. Barbeau , J. I. Collar , O. Tench

High-purity germanium (HPGe) detectors used for low-background gamma ray spectrometry are usually operated under either a fairly low overburden of the order of one meter of water equivalent (mw.e.) or a high overburden of the order of…

The GERDA and Majorana experiments will search for neutrinoless double-beta decay of germanium-76 using isotopically enriched high-purity germanium detectors. Although the experiments differ in conceptual design, they share many aspects in…

Data Analysis, Statistics and Probability · Physics 2012-08-01 M. Agostini , J. A. Detwiler , P. Finnerty , K. Kröninger , D. Lenz , J. Liu , M. G. Marino , R. Martin , K. D. Nguyen , L. Pandola , A. G. Schubert , O. Volynets , P. Zavarise

The MAJORANA DEMONSTRATOR is searching for neutrinoless double-beta decay in $^{76}$Ge with two modular arrays of natural and $^{76}$Ge-enriched germanium detectors. It is located at the 4850 level of Sanford Underground Research Facility…

High Energy Physics - Experiment · Physics 2020-01-08 J. M. López-Castaño

The EDELWEISS-II collaboration has completed a direct search for WIMP dark matter using cryogenic Ge detectors (400 g each) and 384 kg$\times$days of effective exposure. A cross-section of $4.4 \times 10^{-8}$ pb is excluded at 90% C.L. for…

A successfull application of Geiger-mode multipixel avalanche diodes (GMAPDs) for pulse-shape discrimination in alpha-beta spectrometry using organic liquid scintillator is described in this paper. Efficient discrimination of alpha and beta…

Instrumentation and Detectors · Physics 2015-05-28 I. Kreslo , I. Badhrees , S. Delaquis , A. Ereditato , S. Janos , M. Messina , U. Moser , B. Rossi , M. Zeller