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Related papers: Double beta decay: present status

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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 paper reviews recent experiments on tritium beta spectroscopy searching for the absolute value of the electron neutrino mass $m(\nu_e)$. By use of dedicated electrostatic filters with high acceptance and resolution, the uncertainty on…

High Energy Physics - Experiment · Physics 2011-05-24 E. W. Otten , C. Weinheimer

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

A brief sketch is given of the present observational status and future prospects of the physics of neutrino mass, including a survey of the various theoretical schemes of neutrino mass generation. Emphasis is given to those which are…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jose W. F. Valle

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

Double beta decay of $^{100}$Mo to the excited states of daughter nuclei has been studied using a 600 cm$^3$ low-background HPGe detector and an external source consisting of 2588 g of 97.5% enriched metallic $^{100}$Mo, which was formerly…

Nuclear Experiment · Physics 2019-08-12 R. Arnold , C. Augier , A. S. Barabash

The probability distribution for the effective Majorana mass as a function of the lightest neutrino mass in the standard three neutrino scheme is computed via a random sampling from the distributions of the involved mixing angles and…

High Energy Physics - Phenomenology · Physics 2016-01-20 Giovanni Benato

We present a novel mode of neutrinoless double beta decay with emission of a light Majoron-like scalar particle phi. We assume it couples via an effective seven-dimensional operator with a (V+A) lepton current and (V+-A) quark currents…

High Energy Physics - Phenomenology · Physics 2019-05-16 Ricardo Cepedello , Frank F. Deppisch , Lorena González , Chandan Hati , Martin Hirsch

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

Since 2003 the NEMO~3 experiment has been searching for neutrinoless double beta decay using about 10 kg of enriched isotopes. A limit of T_(1/2)(0nu) > 5.8 10**23 years at 90 % CL has been obtained for 100-Mo from the first two years of…

High Energy Physics - Experiment · Physics 2008-11-26 Stefan Soldner-Rembold

Neutrinoless double beta decay $(\b\b)_{0\nu}$ occurs through the magnetic coupling of dimension five, $\lambda_W^{(\nu*)}/m_{\nu*}$, among the excited electron neutrino $\nu^*$, electron and $W$ boson if $\nu^*$ is a massive Majorana…

High Energy Physics - Phenomenology · Physics 2011-04-15 Eiichi Takasugi

The transition matrix elements for the $0^{+}\to 0^{+}$ double beta decays are calculated for $^{48}Ca$, $^{76}Ge $, $^{82}Se$, $^{100}Mo$, $^{128}Te$ and $^{130}Te$ nuclei, using a ${\delta}$-interaction. As a guide, to fix the…

Nuclear Theory · Physics 2016-08-14 F. Krmpotić , S. Shelly Sharma

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

The observation of neutrinoless double beta decay will have important consequences. First it will signal that lepton number is not conserved and the neutrinos are Majorana particles. Second, it represents our best hope for determining the…

High Energy Physics - Phenomenology · Physics 2016-12-12 J. D. Vergados , H. Ejiri , F Šimkovic

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

Nuclear double $\beta ^-$-decays with two neutrinos were observed for many years and a systematic law describing the relation between their half-lives and decay energies was also proposed recently [Phys. Rev. C89, 064603 (2014)]. However,…

Nuclear Theory · Physics 2015-01-08 Yuejiao Ren , Zhongzhou Ren

We present results from a search for neutrinoless double-$\beta$ ($0\nu\beta\beta$) decay using 36.6 g of the isotope $^{150}$Nd with data corresponding to a live time of 5.25 y recorded with the NEMO-3 detector. We construct a complete…

We report the results of a search for neutrinoless double-beta decay in a 9.8~kg$\cdot$yr exposure of $^{130}$Te using a bolometric detector array, CUORE-0. The characteristic detector energy resolution and background level in the region of…

Nuclear Experiment · Physics 2015-10-02 K. Alfonso , D. R. Artusa , F. T. Avignone , O. Azzolini , M. Balata , T. I. Banks , G. Bari , J. W. Beeman , F. Bellini , A. Bersani , M. Biassoni , C. Brofferio , C. Bucci , A. Caminata , L. Canonica , X. G. Cao , S. Capelli , L. Cappelli , L. Carbone , L. Cardani , N. Casali , L. Cassina , D. Chiesa , N. Chott , M. Clemenza , S. Copello , C. Cosmelli , O. Cremonesi , R. J. Creswick , J. S. Cushman , I. Dafinei , A. Dally , S. Dell'Oro , M. M. Deninno , S. DiDomizio , M. L. DiVacri , A. Drobizhev , L. Ejzak , D. Q. Fang , M. Faverzani , G. Fernandes , E. Ferri , F. Ferroni , E. Fiorini , S. J. Freedman , B. K. Fujikawa , A. Giachero , L. Gironi , A. Giuliani , P. Gorla , C. Gotti , T. D. Gutierrez , E. E. Haller , K. Han , E. Hansen , K. M. Heeger , R. Hennings-Yeomans , K. P. Hickerson , H. Z. Huang , R. Kadel , G. Keppel , Yu. G. Kolomensky , K. E. Lim , X. Liu , Y. G. Ma , M. Maino , M. Martinez , R. H. Maruyama , Y. Mei , N. Moggi , S. Morganti , S. Nisi , C. Nones , E. B. Norman , A. Nucciotti , T. O'Donnell , F. Orio , D. Orlandi , J. L. Ouellet , C. E. Pagliarone , M. Pallavicini , V. Palmieri , L. Pattavina , M. Pavan , M. Pedretti , G. Pessina , V. Pettinacci , G. Piperno , S. Pirro , S. Pozzi , E. Previtali , C. Rosenfeld , C. Rusconi , E. Sala , S. Sangiorgio , D. Santone , N. D. Scielzo , M. Sisti , A. R. Smith , L. Taffarello , M. Tenconi , F. Terranova , C. Tomei , S. Trentalange , G. Ventura , M. Vignati , S. L. Wagaarachchi , B. S. Wang , H. W. Wang , L. Wielgus , J. Wilson , L. A. Winslow , T. Wise , L. Zanotti , C. Zarra , G. Q. Zhang , B. X. Zhu , S. Zucchelli

We show that, in the framework of a general model with mixing of three Majorana neutrinos and a neutrino mass hierarchy, the results of the Bugey and Krasnoyarsk reactor neutrino oscillation experiments imply strong limitations for the…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Bilenky , C. Giunti , M. Monteno