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Neutrinoless double beta decay belongs to the most sensitive tools for the search of new physics beyond the standard model. The recent half life limit of the Heidelberg-Moscow experiment implies restrictive bounds on the absolute mass scale…

High Energy Physics - Phenomenology · Physics 2016-11-03 H. V. Klapdor-Kleingrothaus , H. Päs

Heavy neutrino potential for neutrinoless double beta decay is studied with focusing on its statistical property. The existence condition for heavy neutrinos is also presented. In particular sterile neutrinos are possible candidate for…

High Energy Physics - Phenomenology · Physics 2018-04-13 Yoritaka Iwata

The mechanism of beta decay in nature is not understood yet. Mirrored energy spectra of electron and antineutrino can clarify the situation. A special experiment is needed to measure antineutrino spectrum from known beta-decaying isotope to…

High Energy Physics - Phenomenology · Physics 2021-02-26 S. V. Silaeva , V. V. Sinev

Nuclear double beta decay provides an extraordinarily broad potential to search for beyond Standard Model physics, probing already now the TeV scale, on which new physics should manifest itself. These possibilities are reviewed here. First,…

High Energy Physics - Experiment · Physics 2007-05-23 H. V. Klapdor-Kleingrothaus

Neutrinoless double beta decay is the most powerful tool to probe not only for Majorana neutrino masses but for lepton number violating physics in general. We discuss relations between lepton number violation, double beta decay and neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-11 Frank F. Deppisch , Martin Hirsch , Heinrich Päs

We investigate the possibility of producing neutrinoless double beta decay without having an electron neutrino with a mass in the vicinity of 1 eV. We do so by having a much lighter electron neutrino mix with a much heavier (m > 1 GeV)…

High Energy Physics - Phenomenology · Physics 2009-10-28 P. Bamert , C. P. Burgess , R. N. Mohapatra

The 110Pd double-beta decay Q-value was measured with the Penning-trap mass spectrometer ISOLTRAP to be Q = 2017.85(64) keV. This value shifted by 14 keV compared to the literature value and is 17 times more precise, resulting in new…

Several liters of an organic liquid scintillator (LS) loaded with Nd have been made. We report on performances of this scintillator in terms of optical properties, radiopurity and light yield for a Nd concentration of 6.5 g/l. A possible…

Instrumentation and Detectors · Physics 2009-09-14 I. Barabanov , L. Bezrukov , C. Cattadori , N. Danilov , A. Di Vacri , A. Ianni , S. Nisi , F. Ortica , A. Romani , C. Salvo , O. Smirnov , E. Yanovich

The half-life of the 2 neutrino double-beta-decay of 160Gd, a process which was previously reported as theoretically forbidden, is estimated by including the pairing interaction, which mixes different occupations and opens channels for the…

Nuclear Theory · Physics 2009-11-07 Jorge G. Hirsch , Octavio Castanos , Peter O. Hess , Osvaldo Civitarese

Recent results of the Heidelberg-Moscow double beta decay experiment are presented. After 8.6 kg$\cdot$a of measuring time no signal is seen for the neutrinoless decay mode. A half-life limit of $T_{1/2}^{0\nu\beta\beta} > 5.1\cdot…

High Energy Physics - Experiment · Physics 2016-08-31 Heidelberg-Moscow-Collaboration

A radiopure cadmium tungstate crystal scintillator, enriched in $^{106}$Cd to 66%, with mass of 216 g ($^{106}$CdWO$_4$), was used to search for double beta decay processes in $^{106}$Cd in coincidence with four ultra-low background high…

We perform a comprehensive study of the $3+3$ Type-I seesaw model for a broad range of right-handed mass scales (from keV to 10 TeV). We take into account and, in some cases, update the constraints from a large number of high- and…

High Energy Physics - Phenomenology · Physics 2025-05-16 Vincenzo Cirigliano , Wouter Dekens , Sebastián Urrutia Quiroga

Possibilities to search for double beta decay of alpha/beta unstable nuclei, many of which have higher energy release than "conventional" (beta stable) double beta decay candidates, are discussed. First experimental half-life limits on…

Nuclear Experiment · Physics 2009-11-10 V. I. Tretyak , F. A. Danevich , S. S. Nagorny , Yu. G. Zdesenko

One possible probe to physics beyond the standard model is to look for scalar bilinears, which couple to two fermions of the standard model. We point out that the scalar bilinears allow new diagrams contributing to the neutrinoless double…

High Energy Physics - Phenomenology · Physics 2009-11-07 H. V. Klapdor-Kleingrothaus , U. Sarkar

Liquid-scintillator-based detectors are a robust technology that scales well to large volumes. For this reason, they are attractive for experiments searching for neutrinoless double-beta decay. A combination of improved photo-detection…

Instrumentation and Detectors · Physics 2013-07-12 Lindley Winslow

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

In rather general terms the long term perspective of double beta decay is discussed. All important experimental parameters are investigated as well as the status of nuclear matrix element issues. The link with other neutrino physics results…

Nuclear Experiment · Physics 2010-11-09 K. Zuber

We searched for the neutrino-less double beta decay(0nbb) of 48Ca by using CaF2(Eu) scintillators. Analysis of their pulse shapes was effective to reduce backgrounds. No events are observed in the Q-value region for the data of 3394 kg…

This White Paper, prepared for the Fundamental Symmetries, Neutrons, and Neutrinos Town Meeting related to the 2023 Nuclear Physics Long Range Plan, makes the case for double beta decay as a critical component of the future nuclear physics…

Nuclear Experiment · Physics 2022-12-22 C. Adams , K. Alfonso , C. Andreoiu , E. Angelico , I. J. Arnquist , J. A. A. Asaadi , F. T. Avignone , S. N. Axani , A. S. Barabash , P. S. Barbeau , L. Baudis , F. Bellini , M. Beretta , T. Bhatta , V. Biancacci , M. Biassoni , E. Bossio , P. A. Breur , J. P. Brodsky , C. Brofferio , E. Brown , R. Brugnera , T. Brunner , N. Burlac , E. Caden , S. Calgaro , G. F. Cao , L. Cao , C. Capelli , L. Cardani , R. Castillo Fernandez , C. M. Cattadori , B. Chana , D. Chernyak , C. D. Christofferson , P. -H. Chu , E. Church , V. Cirigliano , R. Collister , T. Comellato , J. Dalmasson , V. D'Andrea , T. Daniels , L. Darroch , M. P. Decowski , M. Demarteau , S. De Meireles Peixoto , J. A. Detwiler , R. G. DeVoe , S. Di Domizio , N. Di Marco , M. L. di Vacri , M. J. Dolinski , Yu. Efremenko , M. Elbeltagi , S. R. Elliott , J. Engel , L. Fabris , W. M. Fairbank , J. Farine , M. Febbraro , E. Figueroa-Feliciano , D. E. Fields , J. A. Formaggio , B. T. Foust , B. Franke , Y. Fu , B. K. Fujikawa , D. Gallacher , G. Gallina , A. Garfagnini , C. Gingras , L. Gironi , A. Giuliani , M. Gold , R. Gornea , C. Grant , G. Gratta , M. P. Green , G. F. Grinyer , J. Gruszko , Y. Guan , I. S. Guinn , V. E. Guiseppe , T. D. Gutierrez , E. V. Hansen , C. A. Hardy , J. Hauptman , M. Heffner , K. M. Heeger , R. Henning , H. Hergert , D. Hervas Aguilar , R. Hodak , J. D. Holt , E. W. Hoppe , M. Horoi , H. Z. Huang , K. Inoue , A. Jamil , J. Jochum , B. J. P. Jones , J. Kaizer , G. Karapetrov , S. Al Kharusi , M. F. Kidd , Y. Kishimoto , J. R. Klein , Yu. G. Kolomensky , I. Kontul , V. N. Kornoukhov , P. Krause , R. Krucken , K. S. Kumar , K. Lang , K. G. Leach , B. G. Lenardo , A. Leonhardt , A. Li , G. Li , Z. Li , C. Licciardi , R. Lindsay , I. Lippi , J. Liu , M. Macko , R. MacLellan , C. Macolino , S. Majidi , F. Mamedov , J. Masbou , R. Massarczyk , A. T. Mastbaum , D. Mayer , A. Mazumdar , D. M. Mei , Y. Mei , S. J. Meijer , E. Mereghetti , S. Mertens , K. Mistry , T. Mitsui , D. C. Moore , M. Morella , J. T. Nattress , M. Neuberger , X. E. Ngwadla , C. Nones , V. Novosad , D. R. Nygren , J. C. Nzobadila Ondze , T. O'Donnell , G. D. Orebi Gann , J. L. Orrell , G. S. Ortega , J. L. Ouellet , C. Overman , L. Pagani , V. Palusova , A. Para , M. Pavan , A. Perna , L. Pertoldi , W. Pettus , A. Piepke , P. Piseri , A. Pocar , P. Povinec , F. Psihas , A. Pullia , D. C. Radford , G. J Ramonnye , H. Rasiwala , M. Redchuk , S. Riboldi , G. Richardson , K. Rielage , L. Rogers , P. C. Rowson , E. Rukhadze , R. Saakyan , C. Sada , G. Salamanna , F. Salamida , R. Saldanha , D. J. Salvat , S. Sangiorgio , D. C. Schaper , S. Schoenert , M. Schwarz , S. E. Schwartz , Y. Shitov , F. Simkovic , V. Singh , M. Slavickova , A. C. Sousa , F. L. Spadoni , D. H. Speller , I. Stekl , R. R. Sumathi , P. T. Surukuchi , R. Tayloe , W. Tornow , J. A. Torres , T. I. Totev , S. Triambak , O. A. Tyuka , S. I. Vasilyev , M. Velazquez , S. Viel , C. Vogl , K. von Strum , Q. Wang , D. Waters , S. L. Watkins , M. Watts , W. -Z. Wei , B. Welliver , Liangjian Wen , U. Wichoski , S. Wilde , J. F. Wilkerson , L. Winslow , C. Wiseman , X. Wu , W. Xu , H. Yang , L. Yang , C. H. Yu , J. Zeman , J. Zennamo , G. Zuzel