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Background of germanium and xenon detectors due to the elastic scattering of $^{8}B$ solar neutrinos on electrons have been calculated. The background is 4.6 \times $10^{-4}$ counts/(keV$\cdot t\cdot$y) that defines the sensitivity of…

High Energy Physics - Phenomenology · Physics 2007-05-23 Alexander A. Klimenko

Double-beta decays of $^{100}$Mo from the 6.0195-year exposure of a 6.914 kg high-purity sample were recorded by the NEMO-3 experiment that searched for neutrinoless double-beta decays. These ultra-rare transitions to $^{100}$Ru have a…

Many extensions of the Standard Model of particle physics suggest that neutrinos should be Majorana-type fermions, but this assumption is difficult to confirm. Observation of neutrinoless double-beta decay ($0\nu \beta \beta$), a…

Neutrinoless double beta decay is a hypothetical nuclear transition whose observation would demonstrate that neutrinos are their own antiparticles and that lepton number is not conserved, with far-reaching implications for the origin of…

Nuclear Experiment · Physics 2026-04-16 Andrea Giuliani

The MAJORANA Collaboration has completed construction and is now operating an array of high purity Ge detectors searching for neutrinoless double-beta decay ($0\nu\beta\beta$) in $^{76}$Ge. The array, known as the MAJORANA DEMONSTRATOR, is…

Neutrinoless double-beta decay ($0\nu\beta\beta$) is a rare hypothesised process that, if discovered, would establish that the neutrino is Majorana, that is, it is its own antiparticle. Interpretation of experimental results relies on…

High Energy Physics - Lattice · Physics 2025-04-29 Anthony V. Grebe

The full data set of the NEMO-3 experiment has been used to measure the half-life of the two-neutrino double beta decay of $^{100}$Mo to the ground state of $^{100}$Ru, $T_{1/2} = \left[ 6.81 \pm 0.01\,\left(\mbox{stat}\right)…

If neutrinoless double beta decay is discovered, the next natural step would be understanding the lepton number violating physics responsible for it. Several alternatives exist beyond the exchange of light neutrinos. Some of these…

High Energy Physics - Experiment · Physics 2025-06-13 NEXT Collaboration , M. Martínez-Vara , K. Mistry , F. Pompa , B. J. P. Jones , J. Martín-Albo , M. Sorel , C. Adams , H. Almazán , V. Álvarez , B. Aparicio , A. I. Aranburu , L. Arazi , I. J. Arnquist , F. Auria-Luna , S. Ayet , C. D. R. Azevedo , K. Bailey , F. Ballester , M. del Barrio-Torregrosa , A. Bayo , J. M. Benlloch-Rodríguez , F. I. G. M. Borges , A. Brodolin , N. Byrnes , S. Cárcel , A. Castillo , E. Church , L. Cid , C. A. N. Conde , T. Contreras , F. P. Cossío , R. Coupe , E. Dey , G. Díaz , C. Echevarria , M. Elorza , J. Escada , R. Esteve , R. Felkai , L. M. P. Fernandes , P. Ferrario , A. L. Ferreira , F. W. Foss , Z. Freixa , J. García-Barrena , J. J. Gómez-Cadenas , J. W. R. Grocott , R. Guenette , J. Hauptman , C. A. O. Henriques , J. A. Hernando Morata , P. Herrero-Gómez , V. Herrero , C. Hervés Carrete , Y. Ifergan , F. Kellerer , L. Larizgoitia , A. Larumbe , P. Lebrun , F. Lopez , N. López-March , R. Madigan , R. D. P. Mano , A. P. Marques , G. Martínez-Lema , R. L. Miller , J. Molina-Canteras , F. Monrabal , C. M. B. Monteiro , F. J. Mora , K. E. Navarro , P. Novella , A. Nuñez , D. R. Nygren , E. Oblak , J. Palacio , B. Palmeiro , A. Para , I. Parmaksiz , A. Pazos , J. Pelegrin , M. Pérez Maneiro , M. Querol , J. Renner , I. Rivilla , C. Rogero , L. Rogers , B. Romeo , C. Romo-Luque , V. San Nacienciano , F. P. Santos , J. M. F. dos Santos , M. Seemann , I. Shomroni , P. A. O. C. Silva , A. Simón , S. R. Soleti , J. Soto-Oton , J. M. R. Teixeira , S. Teruel-Pardo , J. F. Toledo , C. Tonnelé , S. Torelli , J. Torrent , A. Trettin , A. Usón , P. R. G. Valle , J. F. C. A. Veloso , J. Waiton , A. Yubero-Navarro

The MAJORANA collaboration is pursuing the development of the so-called MAJORANA DEMONSTRATOR. The DEMONSTRATOR is intended to perform research and development towards a tonne-scale germanium-based experiment to search for the neutrinoless…

Nuclear Experiment · Physics 2019-08-13 Reyco Henning

Assuming 3-$\nu$ mixing, massive Majorana neutrinos and neutrinoless double-beta (\betabeta-) decay generated only by the (V-A) charged current weak interaction via the exchange of the three Majorana neutrinos, we briefly review the…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Pascoli , S. T. Petcov , T. Schwetz

Neutrinoless double beta ($\znbb$) decay violates lepton number; its absence stringently constrains the parameters of theories beyond the standard model in which the neutrino has a Majorana mass. R-parity violating weak-scale supersymmetry…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Hirsch

We present a study of the sensitivity and discovery potential of CUORE, a bolometric double-beta decay experiment under construction at the Laboratori Nazionali del Gran Sasso in Italy. Two approaches to the computation of experimental…

Nuclear Experiment · Physics 2013-03-21 F. Alessandria , R. Ardito , D. R. Artusa , F. T. Avignone , O. Azzolini , M. Balata , T. I. Banks , G. Bari , J. Beeman , F. Bellini , A. Bersani , M. Biassoni , T. Bloxham , C. Brofferio , C. Bucci , X. Z. Cai , L. Canonica , X. Cao , S. Capelli , L. Carbone , L. Cardani , M. Carrettoni , N. Casali , D. Chiesa , N. Chott , M. Clemenza , C. Cosmelli , O. Cremonesi , R. J. Creswick , I. Dafinei , A. Dally , V. Datskov , A. De Biasi , M. M. Deninno , S. Di Domizio , M. L. di Vacri , L. Ejzak , R. Faccini , D. Q. Fang , H. A. Farach , M. Faverzani , G. Fernandes , E. Ferri , F. Ferroni , E. Fiorini , M. A. Franceschi , S. J. Freedman , B. K. Fujikawa , A. Giachero , L. Gironi , A. Giuliani , J. Goett , P. Gorla , C. Gotti , E. Guardincerri , T. D. Gutierrez , E. E. Haller , K. Han , K. M. Heeger , H. Z. Huang , R. Kadel , K. Kazkaz , G. Keppel , L. Kogler , Yu. G. Kolomensky , D. Lenz , Y. L. Li , C. Ligi , X. Liu , Y. G. Ma , C. Maiano , M. Maino , M. Martinez , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , T. Napolitano , S. Newman , S. Nisi , C. Nones , E. B. Norman , A. Nucciotti , T. O'Donnell , F. Orio , D. Orlandi , J. L. Ouellet , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , G. Pessina , G. Piperno , S. Pirro , E. Previtali , V. Rampazzo , F. Rimondi , C. Rosenfeld , C. Rusconi , E. Sala , S. Sangiorgio , N. D. Scielzo , M. Sisti , A. R. Smith , F. Stivanello , L. Taffarello , M. Tenconi , W. D. Tian , C. Tomei , S. Trentalange , G. Ventura , M. Vignati , B. S. Wang , H. W. Wang , T. Wise , A. Woodcraft , L. Zanotti , C. Zarra , B. X. Zhu , S. Zucchelli

The present experimental status in the search for neutrinoless double beta decay is reviewed, with emphasis on the first indication for neutrinoless double beta decay found in the Heidelberg-Moscow experiment, giving first evidence for…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. V. Klapdor-Kleingrothaus , A. Dietz , I. V. Krivosheina

Background: The MAJORANA DEMONSTRATOR , a modular array of isotopically enriched high-purity germanium (HPGe) detectors, was constructed to demonstrate backgrounds low enough to justify building a tonne-scale experiment to search for the…

Instrumentation and Detectors · Physics 2025-01-07 N. Abgrall , E. Aguayo , I. J. Arnquist , F. T. Avignone , A. S. Barabash , C. J. Barton , P. J. Barton , F. E. Bertrand , E. Blalock , B. Bos , M. Boswell , A. W. Bradley , V. Brudanin , T. H. Burritt , M. Busch , M. Buuck , D. Byram , A. S. Caldwell , T. S. Caldwell , Y. -D. Chan , C. D. Christofferson , P. -H. Chu , M. L. Clark , D. C. Combs , C. Cuesta , J. A. Detwiler , Yu. Efremenko , H. Ejiri , S. R. Elliott , J. E. Fast , P. Finnerty , F. M. Fraenkle , N. Fuad , E. Fuller , T. Gilliss , G. K. Giovanetti , J. Goett , M. P. Green , J. Gruszko , I. S. Guinn , V. E. Guiseppe , G. C. Harper , C. R. Haufe , R. Henning , D. Hervas Aguilar , E. W. Hoppe , A. Hostiuc , M. A. Howe , B. R. Jasinski , K. J. Keeter , M. F. Kidd , I. Kim , R. T. Kouzes , B. D. LaFerriere , T. E. Lannen , A. Li , J. C. Loach , A. M. Lopez , J. M. Lopez-Castano , J. MacMullin , S. MacMullin , E. L. Martin , R. D. Martin , R. Massarczyk , S. J. Meijer , J. H. Merriman , S. Mertens , H. S. Miley , J. Myslik , T. K. Oli , J. L. Orrell , C. O'Shaughnessy , G. Othman , N. R. Overman , D. Peterson , W. Pettus , A. W. P. Poon , D. C. Radford , J. Rager , A. L. Reine , K. Rielage , R. G. H. Robertson , L. Rodriguez , N. W. Ruof , H. Salazar , D. C. Schaper , S. J. Schleich , B. Shanks , M. Shirchenko , K. J. Snavely , N. Snyder , A. Soin , D. Steele , A. M. Suriano , G. Swift , D. Tedeschi J. E. Trimble , M. Turqueti , T. D. Van Wechel , R. L. Varner , S. Vasilyev , K. Vorren , S. L. Watkins , B. R. White , J. F. Wilkerson , C. Wiseman , W. Xu , H. Yaver , C. -H. Yu , V. I. Yumatov , I. Zhitnikov , B. X. Zhu

This paper is the first part of the manuscript written in April 2012 for my academic Accreditation to supervise research. It offers a review of the double beta experimental techniques. My purpose is to detail, for each technique, the…

Instrumentation and Detectors · Physics 2012-10-30 Xavier Sarazin

Several efforts are ongoing for the development of spherical gaseous time projection chamber detectors for the observation of rare phenomena such as weakly interacting massive particles or neutrino interactions. The proposed detector,…

The NEMO collaboration is looking to measure neutrinoless double beta decay down to a lower limit of 0.1 eV for the effective neutrino mass. The NEMO 3 detector is now operating in the Frejus Underground Laboratory. The expected performance…

High Energy Physics - Experiment · Physics 2007-05-23 F. Piquemal , NEMO collaboration