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The search for neutrinoless double beta decay is a rich source for new physics. The observation of this decay will lead to understanding of the absolute mass scale of neutrinos, the Majorana nature of the neutrino (whether the neutrino is…

Nuclear Experiment · Physics 2013-05-16 Lisa J. Kaufman

We quantify the extent to which future experiments will test the existence of neutrinoless double-beta decay mediated by light neutrinos with inverted-ordered masses. While it remains difficult to compare measurements performed with…

High Energy Physics - Phenomenology · Physics 2021-10-12 Matteo Agostini , Giovanni Benato , Jason A. Detwiler , Javier Menéndez , Francesco Vissani

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

The first phase of the Advanced Mo-based Rare Process Experiment (AMoRE-I), an experimental search for neutrinoless double beta decay (0$\nu\beta\beta$) of $^{100}$Mo in calcium molybdate (CMO) crystal using cryogenic techniques, is in…

Instrumentation and Detectors · Physics 2017-04-12 A. Luqman , D. H. Ha , J. J. Lee , E. J. Jeon , H. S. Jo , H. J. Kim , Y. D. Kim , Y. H. Kim , V. V. Kobychev , H. S. Lee , H. K. Park , K. Siyeon , J. H. So , V. I. Tretyak , Y. S. Yoon

BINGO is a project aiming to set the grounds for large-scale bolometric neutrinoless double-beta-decay experiments capable of investigating the effective Majorana neutrino mass at a few meV level. It focuses on developing innovative…

Dual-phase xenon detectors, as currently used in direct detection dark matter experiments, have observed elevated rates of background electron events in the low energy region. While this background negatively impacts detector performance in…

Bolometers are low temperature particle detectors with high energy resolution and detection efficiency. Some types of bolometric detectors are also able to perform an efficient particle identification. A wide variety of radiopure dielectric…

Instrumentation and Detectors · Physics 2017-11-06 Denys Poda , Andrea Giuliani

The Enriched Xenon Observatory (EXO) will search for double beta decays of 136Xe. We report the results of a systematic study of trace concentrations of radioactive impurities in a wide range of raw materials and finished parts considered…

Using data from the NEMO-3 experiment, we have measured the two-neutrino double beta decay ($2\nu\beta\beta$) half-life of $^{82}$Se as $T_{1/2}^{2\nu} = \left[ 9.39 \pm 0.17\,\left(\mbox{stat}\right) \pm…

The surface $^{210}$Pb is one of the main background sources for dark-matter-search experiments using NaI(Tl) crystals, and its spectral features associated with the beta-decay events for energies less than 60 keV depends on the depth…

Instrumentation and Detectors · Physics 2020-10-14 G. H. Yu , C. Ha , E. J. Jeon , K. W. Kim , N. Y. Kim , Y. D. Kim , H. S. Lee , H. K. Park , C. Rott

The existing calculations of the nuclear matrix elements of the neutrinoless double beta-decay differ by about a factor three. This uncertainty prevents quantative interpretation of the results of experiments searching for this process. We…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. M. Bilenky , J. A. Grifols

We present an evaluation of the background induced by $^{241}$Am-$^{13}$C neutron calibration sources in the Daya Bay reactor neutrino experiment. As a significant background for electron-antineutrino detection at 0.26$\pm$0.12 per detector…

Instrumentation and Detectors · Physics 2016-07-21 W. Q. Gu , G. F. Cao , X. H. Chen , X. P. Ji , G. S. Li , J. J. Ling , J. Liu , X. Qian , W. Wang

Background coming from the $^{42}$Ar decay chain is considered to be one of the most relevant for the GERDA experiment, which aims to search of the neutrinoless double beta decay of $^{76}$Ge. The sensitivity strongly relies on the absence…

The purpose of the NEMO3 experiment is to detect neutrinoless double beta decay in order to determine the nature of neutrino and its absolute mass. We analysed the 389 effective days of data from the $\sim 7$ kg of $^{100}$Mo and $\sim 1$…

High Energy Physics - Experiment · Physics 2016-08-31 J. S Ricol

The KArlsruhe TRItium Neutrino (KATRIN) experiment is a next generation, model independent, large scale tritium beta-decay experiment to determine the effective electron anti-neutrino mass by investigating the kinematics of tritium…

Instrumentation and Detectors · Physics 2011-10-04 F. M. Fränkle , L. Bornschein , G. Drexlin , F. Glück , S. Görhardt , W. Käfer , S. Mertens , N. Wandkowsky , J. Wolf

The possibility to probe new physics scenarios of light Majorana neutrino exchange and right-handed currents at the planned next generation neutrinoless double beta decay experiment SuperNEMO is discussed. Its ability to study different…

In this paper we evaluate sources of background for the $\gamma p \to \omega p$, with the $\omega$ detected through its $\pi^0 \gamma$ decay channel, to compare with the experiment carried out at ELSA. We find background from $\gamma p \to…

Nuclear Theory · Physics 2010-12-09 M. Kaskulov , E. Hernandez , E. Oset

Internal contaminations of $^{238}$U, $^{235}$U and $^{232}$Th in the bulk of high purity germanium detectors are potential backgrounds for experiments searching for neutrinoless double beta decay of $^{76}$Ge. The data from GERDA Phase~I…

Instrumentation and Detectors · Physics 2017-03-21 GERDA collaboration , M. Agostini , M. Allardt , A. M. Bakalyarov , M. Balata , I. Barabanov , L. Baudis , C. Bauer , N. Becerici-Schmidt , E. Bellotti , S. Belogurov , S. T. Belyaev , G. Benato , A. Bettini , L. Bezrukov , T. Bode , D. Borowicz , V. Brudanin , R. Brugnera , A. Caldwell , C. Cattadori , A. Chernogorov , V. D'Andrea , E. V. Demidova , A. di Vacri , A. Domula , E. Doroshkevich , V. Egorov , R. Falkenstein , O. Fedorova , K. Freund , N. Frodyma , A. Gangapshev , A. Garfagnini , P. Grabmayr , V. Gurentsov , K. Gusev , J. Hakemüller , A. Hegai , M. Heisel , S. Hemmer , W. Hofmann , M. Hult , L. V. Inzhechik , J. Janicsko Csathy , J. Jochum , M. Junker , V. Kazalov , T. Kihm , I. V. Kirpichnikov , A. Kirsch , A. Kish , A. Klimenko , R. Kneißl , K. T. Knöpfle , O. Kochetov , V. N. Kornoukhov , V. V. Kuzminov , M. Laubenstein , A. Lazzaro , V. I. Lebedev , B. Lehnert , H. Y. Liao , M. Lindner , I. Lippi , A. Lubashevskiy , B. Lubsandorzhiev , G. Lutter , C. Macolino , B. Majorovits , W. Maneschg , E. Medinaceli , R. Mingazheva , M. Misiaszek , P. Moseev , I. Nemchenok , D. Palioselitis , K. Panas , L. Pandola , K. Pelczar , A. Pullia , S. Riboldi , N. Rumyantseva , C. Sada , F. Salamida , M. Salathe , C. Schmitt , B. Schneider , S. Schönert , J. Schreiner , A. -K. Schütz , O. Schulz , B. Schwingenheuer , O. Selivanenko , E. Shevchik , M. Shirchenko , H. Simgen , A. Smolnikov , L. Stanco , M. Stepaniuk , L. Vanhoefer , A. A. Vasenko , A. Veresnikova , K. von Sturm , V. Wagner , M. Walter , A. Wegmann , T. Wester , C. Wiesinger , M. Wojcik , E. Yanovich , I. Zhitnikov , S. V. Zhukov , D. Zinatulina , K. Zuber , G. Zuzel
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