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Related papers: EXO: the Enriched Xenon Observatory for Double Bet…

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A search for double-beta decays of 136Xe to excited states of 136Ba has been performed with the first phase data set of the KamLAND-Zen experiment. The 0+1, 2+1 and 2+2 transitions of 0{\nu}\{beta}\{beta} decay were evaluated in an exposure…

We used a high-resolution magnetic spectrograph to study neutron pair-correlated $0^+$ states in $^{136}$Ba, produced via the $^{138}{\rm Ba}(p,t)$ reaction. In conjunction with state-of-the-art shell model calculations, these data…

We present data characterizing the performance of the first segmented, N-type Ge detector, isotopically enriched to 85% $^{76}$Ge. This detector, based on the Ortec PT6x2 design and referred to as SEGA (Segmented, Enriched Germanium…

The NEMO 3 detector, which has been operating in the Frejus underground laboratory since February 2003, is devoted to the search for neutrinoless double beta decay (bb0nu). Half-lives of the two neutrino double beta decays (bb2nu) have been…

High Energy Physics - Experiment · Physics 2019-08-18 R. Arnold

The nature of the neutrino is one of the major open questions in experimental nuclear and particle physics. The most sensitive known method to establish the Majorana nature of the neutrino is detection of the ultra-rare process of…

Instrumentation and Detectors · Physics 2019-10-16 P. Thapa , I. Arnquist , N. Byrnes , A. A. Denisenko , F. W. Foss , B. J. P. Jones , A. D. McDonald , D. R. Nygren , K. Woodruff

The NEMO 3 experiment is devoted to the search for neutrinoless double beta decay, as well as for accurate measurement of two-neutrino double beta decay. The detector has been taking data in the LSM laboratory since 2003 and the latest NEMO…

High Energy Physics - Experiment · Physics 2009-09-11 Ladislav Vala

We report results from a systematic measurement campaign conducted to identify low radioactivity materials for the construction of the EXO-200 double beta decay experiment. Partial results from this campaign have already been reported in a…

The objective of the Majorana Experiment is to study neutrinoless double beta decay (0nbb) with an effective Majorana-neutrino mass sensitivity below 50 meV in order to characterize the Majorana nature of the neutrino, the Majorana mass…

Nuclear Experiment · Physics 2012-08-27 The Majorana collaboration

In view of recent great progress achieved in the experimental study of the neutrinoless double beta decay (0nbb-decay) of 134Xe we discuss theoretical aspects of this process. The light and heavy Majorana neutrino exchange as well as the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Fedor Simkovic , Pavol Domin , Amand Faessler

The PandaX-III experiment searches the neutrinoless double beta decay of $^{136}$Xe with a high-pressure xenon gaseous time projection chamber~(TPC). Thermal-bonding Micromegas modules are used for charge collection. Benefitting from the…

Instrumentation and Detectors · Physics 2023-11-23 Wenming Zhang , Heng Lin , Yuanchun Liu , Ke Han , Kaixiang Ni , Shaobo Wang , Wenchang Zhai

The present status of double beta decay experiments (including the search for $2\beta^{+}$, EC$\beta^{+}$ and ECEC processes) are reviewed. The results of the most sensitive experiments are discussed. Average and recommended half-life…

High Energy Physics - Experiment · Physics 2010-02-17 A. S. Barabash

The NEMO-3 experiment is searching for neutrinoless double beta decay for 2 main isotopes (100Mo and 82Se) and is studying the two-neutrino double beta decay of seven isotopes. The experiment has been taking data since 2003 and, up to the…

High Energy Physics - Experiment · Physics 2019-08-14 Mathieu BONGRAND

nEXO is a proposed next-generation experiment searching for the neutrinoless double beta decay of $^{136}$Xe using a tonne-scale liquid xenon (LXe) time projection chamber (TPC). To image the ionization signals from events in the liquid…

Instrumentation and Detectors · Physics 2025-12-15 Z. Li , M. Yu , E. Angelico , A. Atencio , A. Gupta , P. Knauss , A. Pena-Perez , B. G. Lenardo , P. Acharya , A. Amy , A. Anker , I. J. Arnquist , J. Bane , V. Belov , T. Bhatta , A. Bolotnikov , J. Breslin , P. A. Breur , J. P. Brodsky , E. Brown , T. Brunner , B. Burnell , E. Caden , G. F. Cao , L. Q. Cao , D. Cesmecioglu , D. Chernyak , M. Chiu , R. Collister , M. Marquis , T. Daniels , L. Darroch , R. DeVoe , M. L. di Vacri , X. Defay , Y. Y. Ding , D. Doering , M. J. Dolinski , A. Dragone , B. Eckert , A. Emara , N. Fatemighomi , W. Fairbank , B. T. Foust , D. Gallacher , N. Gallice , A. Gaur , W. Gillis , F. Girard , A. Gorham , K. Gracequist , G. Gratta , C. A. Hardy , J. Hasi , S. Hedges , M. Heffner , E. Hein , H. Hernandez Herrera , J. D. Holt , A. Iverson , X. S. Jiang , A. Karelin , D. Keblbeck , C. Kenney , I. Kotov , A. Kuchenkov , K. S. Kumar , S. Lavoie , A. Larson , M. B. Latif , K. G. Leach , D. S. Leonard , G. Lessard , K. K. H. Leung , G. Li , X. Li , C. Licciardi , R. Lindsay , R. MacLellan , S. Majidi , C. Malbrunot , B. Markovic , J. Masbou , M. Medina-Peregrina , S. Mngonyama , B. Mong , D. C. Moore , K. Ni , I. Nitu , A. Nolan , S. C. Nowicki , J. C. Nzobadila Ondze , A. Odian , J. L. Orrell , G. S. Ortega , L. Pagani , H. Peltz Smalley , A. Piepke , A. Pocar , S. Prentice , V. Radeka , E. Raguzin , R. Rai , H. Rasiwala , D. Ray , B. Reese , S. Rescia , F. Retiere , G. Richardson , V. Riot , R. Ross , L. Rota , P. C. Rowson , R. Saldanha , S. Sangiorgio , S. Sekula , T. Shetty , L. Si , F. Spadoni , V. Stekhanov , X. L. Sun , S. Thibado , T. Totev , S. Triambak , R. H. M. Tsang , O. A. Tyuka , T. Vallivilayil John , E. van Bruggen , M. Vidal , S. Viel , M. Walent , H. Wang , Q. D. Wang , M. Watts , W. Wei , M. Wehrfritz , L. J. Wen , S. Wilde , X. M. Wu , H. Xu , H. B. Yang , L. Yang , O. Zeldovich , J. Zhao

Xenon dual-phase time projection chambers designed to search for Weakly Interacting Massive Particles have so far shown a relative energy resolution which degrades with energy above $\sim$200 keV due to the saturation effects. This has…

Instrumentation and Detectors · Physics 2020-09-10 E. Aprile , J. Aalbers , F. Agostini , M. Alfonsi , L. Althueser , F. D. Amaro , V. C. Antochi , E. Angelino , J. Angevaare , F. Arneodo , D. Barge , L. Baudis , B. Bauermeister , L. Bellagamba , M. L. Benabderrahmane , T. Berger , P. A. Breur , A. Brown , E. Brown , S. Bruenner , G. Bruno , R. Budnik , C. Capelli , J. M. R. Cardoso , D. Cichon , B. Cimmino , M. Clark , D. Coderre , A. P. Colijn , J. Conrad , J. P. Cussonneau , M. P. Decowski , A. Depoian P. Di Gangi A. Di Giovanni R. Di Stefano , S. Diglio , A. Elykov , G. Eurin , A. D. Ferella , W. Fulgione , P. Gaemers , R. Gaior , A. Gallo Rosso , M. Galloway , F. Gao , M. Garbini , L. Grandi , C. Hasterok , C. Hils , K. Hiraide , L. Hoetzsch , E. Hogenbirk , J. Howlett , M. Iacovacci , Y. Itow , F. Joerg , N. Kato , S. Kazama , M. Kobayashi , G. Koltman , A. Kopec , H. Landsman , R. F. Lang , L. Levinson , Q. Lin , S. Lindemann , M. Lindner , F. Lombardi , J. A. M. Lopes , E. López Fune , C. Macolino , J. Mahlstedt , L. Manenti , A. Manfredini , F. Marignetti , T. Marrodán Undagoitia , K. Martens , J. Masbou , D. Masson , S. Mastroianni , M. Messina , K. Miuchi , A. Molinario , K. Morå , S. Moriyama , Y. Mosbacher , M. Murra , J. Naganoma , K. Ni , U. Oberlack , K. Odgers , J. Palacio , B. Pelssers , R. Peres , J. Pienaar , V. Pizzella , G. Plante J. Qin , H. Qiu , D. Ramírez García , S. Reichard , A. Rocchetti , N. Rupp , J. M. F. dos Santos , G. Sartorelli , N. Šarčević , M. Scheibelhut , S. Schindler , J. Schreiner , D. Schulte , M. Schumann , L. Scotto Lavina , M. Selvi , F. Semeria , P. Shagin , E. Shockley , M. Silva , H. Simgen , A. Takeda , C. Therreau , D. Thers , F. Toschi , G. Trinchero , C. Tunnell , M. Vargas , G. Volta , O. Wack , H. Wang , Y. Wei , C. Weinheimer , M. Weiss Xu , D. Wenz , C. Wittweg , J. Wulf , Z. Xu , M. Yamashita , J. Ye , G. Zavattini , Y. Zhang , T. Zhu , J. P. Zopounidis

The NEMO-3 detector, which has been operating in the Frejus Underground Laboratory since February 2003, is devoted to searching for neutrinoless double beta decay (\beta\beta 0 \nu). The expected performance of the detector has been…

High Energy Physics - Experiment · Physics 2010-12-09 Xavier Sarazin

$^{136}$Xe is a 0{\nu}{\beta}{\beta} decay candidate isotope, and is used in multiple experiments searching for this hypothetical decay mode. These experiments require precise information about neutron capture for their background…

NEXT-100 is a high-pressure xenon time projection chamber with electroluminescent amplification, designed to operate with up to approximately 70.5 kg at 13.5 bar. It is the most recent detector developed by the NEXT collaboration to search…

Instrumentation and Detectors · Physics 2026-01-13 NEXT Collaboration , M. Pérez Maneiro , M. Martínez-Vara , S. Torelli , G. Martínez-Lema , P. Novella , J. A. Hernando Morata , J. J. Gómez-Cadenas , C. Adams , H. Almazán , V. Álvarez , A. I. Aranburu , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , Y. Ayyad , C. D. R. Azevedo , K. Bailey , F. Ballester , J. E. Barcelon , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , A. Brodoline , N. Byrnes , A. Castillo , E. Church , L. Cid , M. Cid , X. Cid , C. A. N. Conde , C. Cortes-Parra , F. P. Cossío , R. Coupe , E. Dey , P. Dietz , C. Echeverria , M. Elorza , R. Esteve , R. Felkai , L. M. P. Fernandes , P. Ferrario , F. W. Foss , Z. Freixa , J. García-Barrena , J. W. R. Grocott , R. Guenette , J. Hauptman , C. A. O. Henriques , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , A. F. B. Isabel , B. J. P. Jones , F. Kellerer , L. Larizgoitia , A. Larumbe , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. Marauri , A. P. Marques , J. Martín-Albo , A. Martínez , R. L. Miller , K. Mistry , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , D. R. Nygren , E. Oblak , J. Palacio , B. Palmeiro , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Querol , J. Renner , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , E. Ruiz-Chóliz , P. Saharia , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , A. L. M. Silva , P. A. O. C. Silva , A. Simón , S. R. Soleti , M. Sorel , J. Soto-Oton , J. M. R. Teixeira , S. Teruel-Pardo , J. F. Toledo , C. Tonnelé , J. Torrent , A. Trettin , P. R. G. Valle , M. Vanga , P. Vázquez Cabaleiro , J. F. C. A. Veloso , J. D. Villamil , J. Waiton , A. Yubero-Navarro

NEXT-100 is an electroluminescent high pressure Time Projection Chamber currently under construction. It will search for the neutrino-less double beta decay in 136Xe at the Canfranc Underground Laboratory. NEXT-100 aims to achieve nearly…

Instrumentation and Detectors · Physics 2019-08-16 C. A. B. Oliveira