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We have investigated the role of proton-neutron pairing in the context of the Quasiparticle Random Phase approximation formalism. This way the neutrinoless double beta decay matrix elements of the experimentally interesting A= 48, 76, 82,…

Nuclear Theory · Physics 2008-11-26 G. Pantis , F. Simkovic , J. D. Vergados , Amand Faessler

A brief overview is given of theoretical analyses with neutrinoless double beta decay experiments. Theoretical bounds on the ``observable'', <m>_betabeta, are presented. By using experimental bounds on <m>_betabeta, allowed regions are…

High Energy Physics - Phenomenology · Physics 2017-08-23 Hiroaki Sugiyama

We present a concise formula to relate the effective mass term of the neutrinoless double beta decay to a single neutrino mass, two Majorana CP-violating phases and four observables of neutrino oscillations for a generic neutrino mass…

High Energy Physics - Phenomenology · Physics 2009-11-07 Zhi-zhong Xing

We present an extensive study of nuclear matrix elements (NME) for the neutrinoless double beta decay of the nuclei $^{48}$Ca, $^{76}$Ge, $^{82}$Se, $^{96}$Zr, $^{100}$Mo, $^{116}$Cd, $^{124}$Sn, $^{128}$Te, $^{130}$Te, $^{136}$Xe, and…

Nuclear Theory · Physics 2010-12-28 Tomás R. Rodríguez , G. Martinez-Pinedo

Neutrinoless $\beta\beta$ decay nuclear matrix elements calculated with the shell model and energy-density functional theory typically disagree by more than a factor of two in the standard scenario of light-neutrino exchange. In contrast,…

Nuclear Theory · Physics 2018-04-18 Javier Menéndez

The HEIDELBERG-MOSCOW experiment, which is the most sensitive double beta decay experiment since ten years has been regularly continued until end of November 2003. An analysis of the data has been performed already until May 20, 2003. The…

High Energy Physics - Phenomenology · Physics 2009-09-29 H. V. Klapdor-Kleingrothaus , I. V. Krivosheina , A. Dietz , C. Tomei , O. Chkvoretz , H. Strecker

We investigate how recent updates to neutrino oscillation parameters and the sum of neutrino masses influence the sensitivity of neutrinoless double-beta (0$\nu\beta\beta$) decay experiments. Incorporating the latest cosmological…

High Energy Physics - Phenomenology · Physics 2024-06-28 Dongming Mei , Kunming Dong , Austin Warren , Sanjay Bhattarai

Here, we study the neutrinoless double-$\beta$ ($0\nu\beta\beta$) decay between the ground state and the first $2^+$ state of $^{76}\mbox{Ge} \rightarrow {}^{76}\mbox{Se}$, $^{82}\mbox{Se} \rightarrow{}^{82}\mbox{Kr}$, $^{130}\mbox{Te}…

Nuclear Theory · Physics 2023-01-06 J. Ferretti , R. Magana Vsevolodovna , J. Kotila , E. Santopinto

The LEGEND collaboration is searching for neutrinoless double beta ($0\nu\beta\beta$) decay by operating high-purity germanium detectors enriched in $^{76}$Ge in a low-background liquid argon environment. Building on key technological…

High Energy Physics - Experiment · Physics 2025-10-01 H. Acharya , N. Ackermann , M. Agostini , A. Alexander , C. Andreoiu , G. R. Araujo , F. T. Avignone , M. Babicz , W. Bae , A. Bakalyarov , M. Balata , A. S. Barabash , P. S. Barbeau , C. J. Barton , L. Baudis , C. Bauer , E. Bernieri , L. Bezrukov , K. H. Bhimani , V. Biancacci , E. Blalock , S. J. Borden , G. Borghi , F. Borra , B. Bos , A. Boston , V. Bothe , R. Bouabid , R. Brugnera , N. Burlac , M. Busch , S. Calgaro , L. Canonica , S. Capra , M. Carminati , R. M. D. Carney , C. Cattadori , R. Cesarano , Y. -D. Chan , J. R. Chapman , A. Chernogorov , P. -J. Chiu , C. D. Christofferson , M. L. Clark , A. I. Colon-Rivera , T. Comellato , V. D'Andrea , R. Deckert , J. A. Detwiler , A. Di Giacinto , N. Di Marco , T. Dixon , K. -M. Dong , A. Drobizhev , G. Duran , Yu. Efremenko , S. R. Elliott , C. H. J. Emmanuel , E. Engelhardt , E. Esch , M. T. Febbraro , F. Ferella , 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 , M. Gold , C. Gooch , G. Grünauer , M. P. Green , J. Gruszko , I. Guinn , V. E. Guiseppe , V. Gurentsov , 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. A. Howe , M. Huber , M. Hult , A. Ianni , K. Jędrzejczak , J. Jochum , R. W. L. Jones , 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 , L. L. Kormos , V. N. Kornoukhov , P. Krause , H. Krishnamoorthy , V. V. Kuzminov , K. Lang , M. Laubenstein , N. N. P. N. Lay , E. León , A. Leder , B. Lehnert , A. Leonhardt , N. Levashko , L. Y. Li , A. Li , Y. -R. Lin , M. Lindner , I. Lippi , A. Love , A. Lubashevskiy , B. Lubsandorzhiev , N. Lusardi , C. Macolino , B. Majorovits , F. Mamedov , L. Manzanillas , G. G. Marshall , R. D. Martin , E. L. Martin , R. Massarczyk , A. Mazumdar , G. McDowell , D. -M. Mei , S. P. Meireles , M. Menzel , S. Mertens , E. Miller , I. Mirza , M. Misiaszek , M. Morella , B. Morgan , T. Mroz , D. Muenstermann , C. J. Nave , I. Nemchenok , M. Neuberger , N. O'Briant , F. Paissan , L. Papp , L. S. Paudel , K. Pelczar , L. Pertoldi , W. Pettus , F. Piastra , M. Pichotta , P. Piseri , A. W. P. Poon , P. P. Povinec , M. Pruckner , A. Pullia , W. S. Quinn , D. C. Radford , Y. A. Ramachers , A. Razeto , M. Redchuk , A. L. Reine , S. Riboldi , K. Rielage , C. Romo-Luque , N. Rossi , S. Rozov , T. J. Ruland , N. Rumyantseva , J. Runge , R. Saakyan , S. Sailer , G. Salamanna , F. Salamida , G. Saleh , V. Sandukovsky , C. Savarese , S. Schönert , A. -K. Schütz , D. C. Schaper , L. Schlüter , S. J. Schleich , O. Schulz , M. Schwarz , B. Schwingenheuer , C. Seibt , O. Selivanenko , G. Senatore , A. Serafini , K. Shakhov , E. Shevchik , M. Shirchenko , Y. Shitov , H. Simgen , F. Šimkovic , S. Simonaitis-Boyd , M. Skorokhvatov , M. Slavíčková , A. Smolnikov , J. A. Solomon , G. Song , A. C. Sousa , A. R. Sreekala , L. Steinhart , I. Štekl , T. Sterr , M. Stommel , S. A. Sullivan , R. R. Sumathi , K. Szczepaniec , L. Taffarello , D. Tagnani , D. J. Tedeschi , T. N. Thorpe , V. Tretyak , M. Turqueti , E. E. Van Nieuwenhuizen , L. J. Varriano , S. Vasilyev , A. Veresnikova , C. Vignoli , C. Vogl , K. von Sturm , A. Warren , D. Waters , S. L. Watkins , C. Wiesinger , J. F. Wilkerson , M. Willers , C. Wiseman , M. Wojcik , D. Xu , W. Xu , E. Yakushev , T. Ye , C. -H. Yu , V. Yumatov , D. Zinatulina , K. Zuber , G. Zuzel

The vacuum stability condition of the Standard Model Higgs potential with mass in the range of 124-127 GeV puts an upper bound on the Dirac mass of the neutrinos. We study this constraint with the right-handed neutrino masses upto TeV…

High Energy Physics - Phenomenology · Physics 2015-06-05 Joydeep Chakrabortty , Moumita Das , Subhendra Mohanty

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

We discuss to what extent future precision measurements of neutrino mixing observables will influence the information we can draw from a measurement of (or an improved limit on) neutrinoless double beta decay. Whereas the Delta m^2…

High Energy Physics - Phenomenology · Physics 2009-11-11 S. Choubey , W. Rodejohann

We reconsider the possibility that the masses of the three light neutrinos of the Standard Model might be almost degenerate and close to the present upper limits from Tritium beta decay and cosmology. In such a scenario, the cancellations…

High Energy Physics - Phenomenology · Physics 2009-09-11 John Ellis , Smaragda Lola

Search for \beta \beta -decay of Xe-136 with two high pressure proportional counters is carried out in Baksan Neutrino Observatory. The experiment is based on comparision of spectra measured with natural and enriched xenon. The measured…

The International Germanium Experiment (IGEX) has analyzed 117 mole yr of 76Ge data from its isotopically enriched (86% 76Ge) germanium detectors. Applying pulse-shape discrimination (PSD) to the more recent data, the lower bound on the…

NEMO 3 is a currently running experiment to search for the neutrinoless double beta decay and to study the two-neutrino double beta decay with 10kg of enriched isotopes. On the basis of the first two years of data taking, a limit on the…

Nuclear Experiment · Physics 2019-08-13 V. I. Tretyak

Neutrinoless double beta ($0\nu\beta\beta$) decay, an important low-energy process, serves not only as a potential test of the Majorana nature of neutrinos, but also as a sensitive probe for new physics beyond the Standard Model. In this…

High Energy Physics - Phenomenology · Physics 2025-10-10 Vivek Banerjee , Sasmita Mishra

Neutrinoless double beta decay is a very important process both from the particle and nuclear physics point of view. From the elementary particle point of view it pops up in almost every model. giving rise, among others, to the following…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. D. Vergados

All existing data on neutrino oscillations (including those from the LSND experiment) imply a four neutrino scheme with six different allowed mass patterns. Some of the latter are shown to be disfavored by using a conservative upper bound…

High Energy Physics - Phenomenology · Physics 2009-11-07 Sandip Pakvasa , Probir Roy
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