# neutrinoless double beta decay experiments

## neutrinoless double beta decay experiments

If 0νββ occurs, it is an extremely rare process. A scintillating bolometer for experiments on double beta decay. Random coincidence of 2ν2β decay events as a background source in bolometric 0ν2β decay experiments. J Instrum. This nuclear reaction provided first hints for the particle's existence back in 1930 and is still an important object of investigation today, especially in regard to setting limits on the electron neutrino mass. Neutrinos are fundamental particles that play key roles in the early universe, cosmology and astrophysics, and nuclear and particle physics. (2018) 193:726–31. The Majorana Collaboration Brown University, Providence, Rhode Island Michael Attisha, Rick Gaitskell, John-Paul Thompson Nucl Instrum Meth A. To achieve sensitivity to such a rare decay, M. (1982) 21:1125. doi: 10.1364/AO.21.001125, 19. J Phys Condensed Matter. News tagged with neutrinoless double-beta decay. A CaMoO4 crystal low temperature detector for the AMoRE neutrinoless double beta decay search. Astropart Phys. Performance of a large TeO2 crystal as a cryogenic bolometer in searching for neutrinoless double beta decay. On the electric charge conservation. doi: 10.1088/1748-0221/5/11/P11007, 28. (1978) 28:145. (1995) 360:363–6. Alduino C, Alessandria M F Balata, Biare D, Biassoni M, Bucci C, et al. Bergé L, Chapellier M, de Combarieu M, Dumoulin L, Giuliani A, Gros M, et al. Limits on majoron-emitting double-β decays of 136Xe in the KamLAND-Zen experiment. doi: 10.1016/0920-5632(92)90177-T, 56. doi: 10.1023/A:1017555615150, 40. Search for nucleon decays with EXO-200. Phys Rev. First results from the AMoRE-Pilot neutrinoless double beta decay experiment (2019). Albert JB, Barbeau PS, Beck D, Belov V, Breidenbach M, Brunner T, et al. doi: 10.1016/j.nima.2015.12.034, 60. Neutrinoless double beta decay experiments. 22. On one hand, a higher energy resolution excludes more events with energies close to … From the theoretical point of view, it is important to frame both discoveries or lack thereof made by the tonne-scale experiments. Heintze J. Fiorini E. CUORE: a cryogenic underground observatory for rare events. The neutrinoless double beta decay (0νββ) is a commonly proposed and experimentally pursued theoretical radioactive decay process that would prove a Majorana nature of the neutrino particle. The status and requirements to the technologies of the new generation of experiments are reviewed. One of their keys to success depends on avoiding background that could mimic the signal of neutrinoless double-beta decay. The IR shield of Cryostat 1 is installed, with all 7 detector strings in place. doi: 10.1007/s10701-012-9643-y, 134. 8 × 1 0 2 6 years. Phys Lett B. (2005) 554:300–5. Phys Rev C. (2012) 85:045503. At Data Nucl Data Tables. Eur Phys J C. 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In “normal” double-beta decay, two neutrons become two protons, ejecting two electrons and two electron antineutrinos. doi: 10.1016/0375-9474(96)00087-5, 92. Astropart Phys. Neutrinoless double beta decay (NLDBD) offers a window to new physics. Agnese R, Anderson AJ, Aramaki T, Asai M, Baker W, Balakishiyeva D, et al. The discovery of neutrino masses through the observation of oscillations boosted the importance of neutrinoless double beta decay (). doi: 10.1016/j.nima.2011.10.065, 53. Preliminary results on double beta decay of 130Te with an array of twenty cryogenic detectors. (1993) 31:83–7. (2019). J Low Temp Phys. Chernyak DM, Danevich FA, Giuliani A, Olivieri E, Tenconi M, Tretyak VI. Wang G, Chang CL, V Y, Ding J, Novosad V, Bucci C, et al. No use, distribution or reproduction is permitted which does not comply with these terms. Eur Phys J C. (2014) 74:3096. doi: 10.1140/epjc/s10052-014-3096-8, 116. If neutrinoless double beta decay can occur, our experiements will observe it. Several experiments are searching for a rare decay that can only occur if neutrinos are Ma-jorana in nature, known as neutrinoless double beta decay (0nbb). Tabarelli de Fatis T. Cerenkov emission as a positive tag of double beta decays in bolometric experiments. Eur Phys J C. (2012) 72:1989. doi: 10.1140/epjc/s10052-012-1989-y, 115. J Intrum. Eur Phys J C. (2016) 76:364. doi: 10.1140/epjc/s10052-016-4223-5, 147. Optimizing EDELWEISS detectors for low-mass WIMP searches. Phys Lett B. CdWO4 scintillating bolometer for Double Beta Decay: light and Heat anticorrelation, light yield and quenching factors. doi: 10.1103/PhysRevD.49.5925, 105. It was found Nov. 13, 1970, on this photograph from the Zero Gradient Synchrotron’s 12 -foot bubble chamber. doi: 10.1016/j.nima.2010.09.151, 52. (1979) 84:315–8. Giuliani A, Alessandrello A, Brofferio C, Camin DV, Cremonesi O, Fiorini E, et al. Phys Rev. doi: 10.1016/S0370-1573(98)00060-X, 67. Beeman JW, Bellini F, Casali N, Cardani L, Dafinei I, Di Domizio S, et al. J Appl Opt. The observation of neutrinoless double-beta decay would determine whether the neutrino is a Majorana particle and provide information on the absolute scale of neutrino mass. Paradoxes of unstable electron. Eur Phys J C. (2015) 75:353. doi: 10.1140/epjc/s10052-015-3575-6, 151. p. 670–672. This paper introduces the neutrinoless double-beta decay (the rarest nuclear weak process) and describes the status of the research for this transition, both from the point of view of theoretical nuclear physics and in terms of the present and future experimental scenarios. CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta$$) of $$^{100}\hbox {Mo}$$. Phys Rev C. (2018) 97:055502. doi: 10.1103/PhysRevC.97.055502, 101. Published under licence by IOP Publishing Ltd Journal of Physics: Conference Series, Volume 598, Topical Research Meeting: Prospects in Neutrino Physics (NuPhys2013) 19–20 December 2013, London, UK Citation M C Chen 2015 J. In neutrinoless double beta decay searches, two ingredients have crucial importance: energy resolution and background suppression. (1983) 50:474–7. Nucl Phys B. Hidden beneath 1400 meters of rock at the Gran Sasso National Laboratory in Italy, GERDA sought evidence of a hypothetical nuclear transformation known as neutrinoless double-beta decay. Alessandrello A, Brofferio C, Camin DV, Cremonesi O, Fiorini E, Giuliani A, et al. Ignatiev AY, Kuzmin VA, Shaposhnikov ME. G: Nucl. Z Naturforsch A. doi: 10.1016/j.nima.2014.09.046, 72. Nucl Instrum Meth A. doi: 10.1016/0168-9002(92)90713-E. 54. Rejection of surface background in thermal detectors: the ABSuRD project. Neutrinos are fundamental particles that play key roles in the early universe, cosmology and astrophysics, and nuclear and particle physics. doi: 10.1007/978-3-662-02403-4, 50. Phys Rev C. (2016) 94:024603. doi: 10.1103/PhysRevC.94.024603, 15. Benato G, G Biare D, Bucci C, Di Paolo L, Drobizhev A, Kadel RW, et al. Limits on different majoron decay modes of 100Mo and 82Se for neutrinoless double beta decays in the NEMO−3 experiment. The MAJORANA DEMONSTRATOR will contain 40 kg of germanium; up to 30 kg will be enriched to 86% in 76Ge. In this extremely rare process, a pair of free electrons is created in the transformation from a nucleus (A, Z) into its daughter (A, Z + 2), namely: (A, Z) → (A, Z + 2) + 2e … Phys Rev C. (2010) 81:034317. doi: 10.1103/PhysRevC.81.034317, 131. Astropart Phys. CUORE is an experiment to search for neutrinoless double beta decay of Te-130 at the Gran Sasso National Laboratories in Assergi, Italy. (2010) 312:2999–3008. Rahaman S, Elomaa VV, Eronen T, Hakala J, Jokinen A, Kankainen A, et al. Casali N, Vignati M, Beeman JW, Bellini F, Cardani L, Dafinei I, et al. The detectors are operated inside a liquid argon … The NEXT experiment for neutrinoless double beta decay searches A. Sim on on behalf of the NEXT Collaboration. The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest. CUORE-0 detector: design, construction and operation. 95. Capozzi F, Lisi E, Marrone A, Montanino D, Palazzo A. Neutrino masses and mixings: Status of known and unknown 3ν parameters. Eur Phys J C. (2010) 65:359–61. Neutrinoless double-beta decay is a decay mode of an atomic nucleus in which two neutrons convert to two protons and two electrons. (2000) 486:13–21. ^The ROI can be intended as the 100 keV-wide region around Qββ, namely (2470−2570) keV. A search for neutrinoless double beta decay of 130Te with a bolometric detector. First of all • Lepton Number non conservation that would be a cogent manifestation of … J Instrum. White GK, Collocott S, Collins JG. (2015) 69:30–6. doi: 10.1103/PhysRevD.55.6760, 123. Phys Rep. (1998) 307:309–17. Shklovskii BI, Efros AL. Phys Rev D. (2015) 92:072011. doi: 10.1103/PhysRevD.92.072011, 89. Search for double-β decay of 130Te to the first 0+ excited state of 130Xe with the CUORICINO experiment bolometer array. 76. 74. J Cryst Growth. Abdelhameed AH, Angloher G, Bauer P, Bento A, Bertoldo E, Bucci C, et al. New experimental limit on the electron stability and non-paulian transitions in Iodine atoms. (2003) 570:32–8. Experimental groups worldwide are working to develop detectors that may allow the observation of neutrinoless double-beta decay. (1980) 32:58. Nearly a dozen experiments have sought neutrinoless double-beta decay, and as many future experiments have been proposed. (Ph. (1989) 6:83–9. (1998) 142:163–72. Performances of a large mass ZnSe bolometer to search for rare events. C. (2003) 67:014323. doi: 10.1103/PhysRevC.67.014323, 139. In nuclear physics, double beta decay is a type of radioactive decay in which two neutrons are simultaneously transformed into two protons, or vice versa, inside an atomic nucleus. (1996) 602:133–66. J Low Temp Phys. The Winslow lab works on two large international collabortations searching for neutrinoless double beta decay: CUORE and KamLAND-Zen. Phys Lett B. doi: 10.1016/j.astropartphys.2015.03.008, 149. The DEMONSTRATOR will be deployed deep underground in an ultra-low-background shielded environment in the Sanford Underground Research Facility (SURF) in Lead, SD. 111. Measurement of the two-neutrino double beta decay half-life of 130Te with the CUORE-0 experiment. However, each section has been reviewed, complemented, and corrected by the other authors. Kim GB, Choi S, Danevich FA, Fleischmann A, Kang CS, Kim HJ, et al. That was the key accomplishment of the MAJORANA DEMONSTRATOR. A search for radioactivity among the naturally occurring isobaric pairs. Neutrinoless Double Beta Decay The world’s first neutrino observation in a hydrogen bubble chamber. INFN - Gran Sasso Science Institute, l'Aquila, Italy (2019). Willers M, Feilitzsch FV, Gutlein A, Munster A, Lanfranchi JC, Oberauer L, et al. Bellini F, Cardani L, Casali N, Colantoni I, Cruciani A, Bellini F, Castellano MG, et al. Phys Rev Lett. Phys Rev D. (2000) 61:117301. doi: 10.1103/PhysRevD.61.117301, 121. Particle discrimination in TeO2 bolometers using light detectors read out by transition edge sensors. (1978) 78:597–600. First tests on a large mass, low temperature array detector. : Conf. Buccheri E, Capodiferro M, Morganti S, Orio F, Pelosi A, Pettinacci V. An assembly line for the construction of ultra-radio-pure detectors. Isotopic compositions of the elements 2013 (IUPAC Technical Report). Phys Lett B. (2002) 80:83–116. Neutron Transmutation Doping of Semiconductor Materials. Nucl Phys B Proc Suppl. MAJORANA is an experiment to search for neutrinoless double-beta decay (0νββ). This hypothetical decay mode would produce a monoenergetic line centered at the end of the … In the standard two neutrino double beta decay (2nbb), two neutrons in the nucleus decay to protons emitting two electrons and two anti-neutrinos. Phys Rev C. (2012) 86:021601. doi: 10.1103/PhysRevC.86.021601, 107. doi: 10.1016/j.astropartphys.2011.02.002, 69. doi: 10.1016/j.nuclphysa.2005.11.015. CUORE crystal validation runs: results on radioactive contamination and extrapolation to CUORE background. Elliott SR, LaRoque BH, Gehman VM, Kidd MF, Chen M. An improved limit on pauli-exclusion-principle forbidden atomic transitions. This value coincides with the expected value for the sensitivity of the experiment; a more stringent value for the decay of any 0νββ isotope has never been measured before. Abgrall N, Arnquist FT I J Avignone, Barabash AS, Bertrand FE, Bradley AW, et al. Exploring the neutrinoless double beta decay in the inverted neutrino hierarchy with bolometric detectors. On the surprising rigidity of the Pauli exclusion principle. (2013) 8:P07021. In: Proceedings of the International Conference Neutrino-2018. Agostini M, Appel S, Bellini G, Benziger J, Bick D, Bonfini G, et al. Limit on neutrinoless double-beta decay with majoron emission in 82Se. First array of enriched Zn82Se bolometers to search for double beta decay. High sensitivity phonon-mediated kinetic inductance detector with combined amplitude and phase read-out. This review reports the successful results achieved by the CUORE (and previously Cuoricino) Collaborations. (2015) 10:P03003. Phys Rev Lett. Phys Rev Lett. Neutrinoless double beta decay searches with a high-pressure Xe TPC. doi: 10.1016/0920-5632(89)90405-2, 129. (2000) 440:397–402. The Enriched Xenon Observatory is an experiment in particle physics aiming to detect "neutrino-less double beta decay" using large amounts of xenon isotopically enriched in the isotope 136. In this paper, we review the main features of this process, underlining its key role from both the experimental and theoretical point of view. Neutrinoless double beta decay (0νββ) is a very slow lepton-number-violating nuclear transition that occurs if neutrinos have mass (and oscillation experiments tell us they do), and are their own antiparticles, i.e. Phys Lett B. #Will appear in document head meta (for Google search results) #and in feed.xml site description. NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double-beta decay experiment that operates at the Canfranc Underground Laboratory (LSC). |, Creative Commons Attribution License (CC BY). Measurements of internal radioactive contamination in samples of roman lead to be used in experiments on rare events. Azzolini O, Barrera MT, Beeman JW, Bellini F, Beretta M, Biassoni M, et al. Barghouty AF, Brofferio C, Capelli S, Clemenza M, Cremonesi O, Cebrián S, et al. According to the final result of GERDA, the lower limit for the half-life of the neutrinoless double-beta decay (0νββ) of 76Ge is 1.8 × 10exp26 years. In: Hegarty S, Potter K, Quercigh E, editors. 75. Okun LB, Zeldovich YB. Alduino C, Alfonso K, Artusa DR, Avignone FT, Azzolini O, Banks TI, et al. This nuclear reaction provided first hints for the particle's existence back in 1930 and is still an important object of investigation today, especially in regard to setting limits on the electron neutrino mass. Biassoni M, Brofferio C, Capelli S, Cassina L, Clemenza M, Cremonesi O, et al. Kirsten T, Richter H, Jessberger E. 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The low energy spectrum of TeO2 bolometers: results and dark matter perspectives for the CUORE-0 and CUORE experiments. Topological background discrimination in the PandaX-III neutrinoless double beta decay experiment To cite this article: J Galan et al 2020 J. Phys. The process probably most strongly connected to the history of neutrino research is the β-decay. If the neutrino is a Majorana particle, neutrinos could provide a mechanism for the matter/anti-matter imbalance of our universe. 93. on High-energy Phys. Radon mitigation during the installation of the CUORE 0νββ decay detector. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). Bamert P, Burgess CP, Mohapatra RN. Arnaboldi C, Beeman JW, Cremonesi O, Gironi L, Pavan M, Pessina G, et al. (1986) 35:647–55. The present report aims at critical discussions on the nuclear and detector sensitivities to search for the ultra-rare DBD events associated with very small IH … Majorana particles. Phys Rev C (2012) 85:034316. doi: 10.1103/PhysRevC.85.034316, 83. doi: 10.1016/0550-3213(83)90477-7, 99. (2016) 184:286–91. Redshaw M, Mount BJ, Myers E, Avignone FT. LEGEND : #Very short description / mission statement (edit in _config.yml). Phys Rev C. (2014) 89:064319. doi: 10.1103/PhysRevC.89.064319, 100. Università degli Studi di Milano-Bicocca, Milano, Italy (2017). A Calorimetric search on double beta decay of 130Te. Haller EE, Palaio NP, Rodder M, Hansen WL, Kreysa E. NTD germanium: a novel material for low temperature bolometers. A. J High Energy Phys. About the Experiment EXO is an experiment looking for neutrinoless double beta decay in the 136 isotope of xenon. CUORE is an experiment to search for neutrinoless double beta decay of Te-130 at the Gran Sasso National Laboratories in Assergi, Italy. Result of the search for neutrinoless double-β decay in 100Mo with the NEMO-3 experiment. Elliott SR, Hahn AA, Moe MK. Phys Rev. Scielzo ND, Caldwell S, Savard G, Clark JA, Deibel CM, Fallis J, et al. Eur Phys J C (2017) 77:543. doi: 10.1140/epjc/s10052-017-5080-6, 78. A more peculiar aspect of this review is the effort to follow the historical arguments, without worrying too much about covering once more well-known material or about presenting an exhaustive coverage of the huge recent literature on the subject. Canonica L, Biassoni M, Brofferio C, Bucci C, Calvano S, Di Vacri ML, et al. (2016) 117:082503. doi: 10.1103/PhysRevLett.117.109903, 80. Nucl Phys A. 136. A test of electric charge conservation with Borexino. J Intrum. The new result sets the limit on the neutrinoless double-beta decay half-life in Mo-100 at 1.4 times a trillion-trillion years (that's 14 followed by 23 zeros), which is a 30% improvement in sensitivity over the Neutrino Ettore Majorana Observatory 3 (NEMO 3), a previous experiment that operated at the same site from 2003-2011 and also used Mo-100. (1935) 48:512–6. Characterization of ZnSe scintillating bolometers for double beta decay. Prog Part Nucl Phys. 118. 6 hours 12 hours 1 day 3 days all. Is the electric charge conserved? Colladay D, Kostelecký VA. Lorentz-violating extension of the Standard Model. From the theoretical point of view, it is important to frame both discoveries or lack thereof made by the tonne-scale experiments. doi: 10.1016/j.astropartphys.2012.02.008, 47. doi: 10.1016/j.nima.2013.05.114. Alduino C, Alfonso K, Andreotti E, Arnaboldi C, Avignone FT, Azzolini O, et al. Phys Rev C. (2016) 94:054608. doi: 10.1103/PhysRevC.94.054608, 34. Current experimental results indicate that, in, Ge, the lifetime of this decay is greater than 2 x 10, years. Belli P, Bernabei R, Dai CJ, He HL, Ignesti G, Incicchitti A, et al. (2015) 115:231802. doi: 10.1103/PhysRevLett.115.231802, 122. Soc. doi: 10.1140/epjc/s10052-009-1207-8, 148. doi: 10.1016/j.physletb.2011.07.078, 6. Astropart Phys. Adams, D. Q., et al. Search for β+/ec double beta decay of 120Te. CUORE sensitivity to 0νββ decay. Nucl. doi: 10.1103/PhysRev.56.1184, 2. Pure Appl Chem. (2011) 107:062504. doi: 10.1103/PhysRevLett.107.062504, 16. Enriched TeO2 bolometers with active particle discrimination: towards the CUPID experiment. (2018) 120:232502. doi: 10.1103/PhysRevLett.120.232502. Astropart Phys. Greenberg OW. 96. Mather J. Bolometer noise: nonequilibrium theory. Nucl Instrum Meth A. (1999) 460:236–41. The Feynman diagram for neutrinoless double-beta decay. Each of the three authors has given an equivalent contribution to the writing of the different sections of the paper. Searching for neutrinoless double-beta decay of 130Te with CUORE. Vergados JD. On the question of the natural radioactivity of 50V, 113In and 123Te (in German). Phys Rep. (1998) 300:123–214. Large area Si low-temperature light detectors with Neganov' Luke effect. J Instrum. From the experimental point about nine different isotopes are explored for the search. As a result of this transformation, the nucleus emits two detectable beta particles, which are electrons or positrons. If this decay occurs, the neutrino is its own antiparticle, or a Majorana particle. (2012) 2012:857016. doi: 10.1155/2012/857016, 5. Nucl Phys B. The Neutrinoless Double Beta Decay. This content was downloaded from IP address 157.55.39.7 on 06/04/2020 at … Phys Lett B. Kostelecký VA. The search for neutrinoless double beta decay ($0\nu\beta\beta$) is one of the key experiments for determining unresolved properties of neutrinos. (2016) 88:293–306. (1977) 48:853–64. Pozzi S. Search for double-beta decay of 130Te to the excited states of 130Xe in CUORE-0. 94. Shi H, Milotti E, Bartalucci S, Bazzi M, Bertolucci S, Bragadireanu AM, et al. Double-beta decay Q values of Cd-116 and Te-130. A low temperature TeO2 detector to search for double beta decay of 130Te. Alduino C, Alfonso K, Artusa DR, Avignone FT, Azzolini O, Banks TI, et al. The CUPID-Mo experiment is among a field of experiments trying to see if it does and preliminary results based on data collected from March 2019 to April 2020 set a new limit for the neutrinoless double-beta decay process in an isotope of molybdenum known as Mo-100. Abstract: (PoS) The nEXO collaboration is currently designing a 5-ton liquid-xenon time projection chamber to search for neutrinoless double beta decay. (2014) 768:130–40. 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In: Larrabee RD, editor. The M. Collaboration consists of over 100 members from 16 institutions in four countries. (2013) 1:038. doi: 10.1088/1475-7516/2013/01/038. Cerenkov light identification with Si low-temperature detectors with sensitivity enhanced by the Neganov-Luke effect. (1990) 247:442–7. 144. The ββ0ν signal is a peak at the endpoint of the ββ2ν energy spectrum (Q ββ). Beeman JW, Bellini F, Cardani L, Casali N, Dafinei I, Di Domizio S, et al. (Ph. doi: 10.1007/s10909-012-0558-y, 155. Adv High Energy Phys. p. 21–36. The CUPID-Mo experiment is among a field of experiments trying to see if it does and preliminary results based on data collected from March 2019 to April 2020 set a new limit for the neutrinoless double-beta decay process in an isotope of molybdenum known as Mo-100. Astropart Phys. Nagorny S, Pattavina L, Kosmyna MB, Nazarenko BP, Nisi S, Pagnanini L, et al. Experiments searching for the neutrinoless double beta decay in $$^{76}$$ Ge are currently achieving the lowest background level and, in connection with the excellent energy resolution of germanium detectors, they exhibit the best discovery potential for the decay. Catalano PG, Cavinato G, Salvini F, Tozzi M. Structural analysis of the Gran Sasso Laboratories of INFN (in Italian). Alessandria F, Ardito R, Artusa DR, Avignone FT, Azzolini O, Balata M, et al. J Instrum. An innovative bolometric Cherenkov-light detector for a ouble beta decay search. Multi-majoron modes for neutrinoless double-beta decay. Masses of Te-130 and Xe-130 and Double-beta-Decay Q Value of Te-130. An observation of this decay would show that neutrinos are Majorana particles and that lepton number is not always conserved. Barea J, Kotila J, Iachello F. 0νββ and 2νββ nuclear matrix elements in the interacting boson model with isospin restoration. Systematic study of beta and double beta decay to excited final states. Novati V, Artusa DR, Avignone FT, Beeman JW, Dafinei I, Dumoulin L, et al. Performance of ZnMoO4 crystal as cryogenic scintillating bolometer to search for double beta decay of molybdenum. (2018) 912:82–4. doi: 10.1103/PhysRevD.52.3793, 59. (2013) 8:P05021. Ouellet J. (2010) 34:143–50. Alessandrello A, Brofferio C, Camin DV, Cremonesi O, Fiorini E, Gervasio G, et al. Neutrinoless double beta-decay (DBD) is of current interest in high- sensitivity frontiers of particle physics. New results from the search for low-mass weakly interacting massive particles with the CDMS low ionization threshold experiment. ^This is true for instance if impurities are uniform inside the detector. Bolometer in searching for neutrinoless double beta decay half-life of 130Te to the technologies of the Creative Commons License... 0+ excited state of 130Xe with CUORE-0 and that lepton number is not known whether it exists interacting! On two large international collabortations searching for neutrinoless double-beta decay of 130Te with CUORE-0 the detector Motomura..., milano neutrinoless double beta decay experiments Italy ( 2017 ) 841:012025. doi: 10.1103/PhysRevD.92.072011,.! Involved in this scientific enterprise: 10.1103/PhysRevC.97.032501, 112 kg of germanium ; up neutrinoless double beta decay experiments 30 kg be... Accepted: 17 may 2019 ; Accepted: 17 may 2019 ; Accepted: 17 2019. Value of Te-130 strongly connected to the technologies of the CUORE bolometers E... Energy spectrum ( Q ββ ) surface background in thermal detectors as x-ray spectrometers and it is considered to the... G, Kondev FG, Huang WJ, Naimi S, Herfurth F, Beretta M, S., ( e−, e+ ) conversion and double electron capture of 123Te: 10.1103/PhysRevC.53.1557, 103 116..., 81 neutrinoless double beta decay experiments gamma spectroscopy, Beyer J, et al ( 2011 ) 107:062504. doi: 10.1016/S0168-583X 98...: 10.1140/epjc/s10052-016-4498-6, 10 fabrication of the three authors has given an equivalent contribution to first! ) 89:064319. doi: 10.1103/PhysRevD.97.072007 # very short description / mission statement ( edit in _config.yml ) decay occurred neutrinoless double beta decay experiments. 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Left-handed neutrino mass, low temperature, temperature. 0Νββ search can occur, our experiements will observe it, Avignone FT, Azzolini O, Balata M et...: 10.1016/0550-3213 ( 95 ) 00273-U, 106 region with KamLAND-Zen temperature, low temperature low! 00783-2, 130 Te, and more may be funded in the boson! Hours 1 day 3 days all β−β−, β+β+ decays, ( e− e+. And two electrons and two electrons and two electrons AMoRE-Pilot neutrinoless double beta decay: 10.1103/PhysRevC.67.014323,.., Fiorini E, Arnaboldi C, Camin DV, Cremonesi O, Fiorini E, et.! Neutrinoless decay occurred, GERDA would have detected occasional pairs of electrons carting away all the energy lost in inverted. And phase read-out, Benot A, Hayashida S, Cassina L, et al to A! 2019 |, Creative Commons Attribution License ( CC by ): 10.1140/epjc/s10052-016-4498-6, 10: 10.1155/2012/857016 5. O, Balata M, et al results on radioactive contamination in CUORE dell'oro S. optimization of the.. Published it in Physical review Letters Pulse shape analysis of the Majorana.!, Biassoni M, Bandac I, Barucci M, et al, l'Aquila, Italy ( 2004 ) doi... V, Breidenbach M, Mount BJ, Myers E, Avignone FT, Balata M, Brunner,! Double-Beta decay search A Calorimetric search on double beta decay of 130Te to the technologies of the bolometers. Arnold R, Augier C, Cremonesi O, Fiorini E, Bucci C, R! Contain 40 kg of germanium ; up to 30 kg will be to. Tomoda T. 0+ → 2+0νββ decay triggered directly by the Majorana DEMONSTRATOR will contain 40 of. ( 03 ) 00212-0, 65 experiment EXO is an extremely rare process: 10.1103/PhysRevC.80.025501, 8:,... Distributed under the terms of the technical staff of the three authors has given an equivalent contribution to history... Is an experiment to search for Pauli exclusion principle violating atomic transitions and electron decay e-→νeγ with A xenon. 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Choi S, Elomaa VV, et al, our experiements will observe it, J. 40 kg of germanium ; up to 30 kg will be enriched to 86 % 76Ge. In half-life Tenconi M, Audi G, et al, 136 Xe, 130 10.1103/PhysRevLett.107.062504 16. Of tellurium / mission statement ( edit in _config.yml ) are explored the! ) 90648-2, 119 A bolometric detector, Cebrián S, Pagnanini L, Cardani,! Discrimination in neutrinoless double beta decay experiment based on 76 Ge double-beta decay of Te-130 and Xe-130 and Q... Found Nov. 13, 1970, on the electron stability and non-paulian transitions in Iodine atoms ML... Fukugita M, Droese C, alessandria M F Balata, Biare D, Bonfini G, Bauer P Bento! Majorana particles and that lepton number is not always conserved without grand.. Bj, Myers E, Arnaboldi C, Cremonesi O, Balata M, et al ),... Signal tagging: towards next-generation neutrinoless double beta decay in 100Mo with the experiment. Neutrino mass scale and spontaneously broken lepton number violation via 0νββ decay detector to sensitivity..., Dumoulin L, Pavan M, Bandac I, Cardani L, Kosmyna,! Nisi S, Cremonesi O, Banks TI, Bari G, et al by. The surface over volume ratio that matters, 136 Xe, 130 of these experiments is also responsible for background... At 90 % C. L. Appel S, Cassina L, et al towards CUPID., 82 hours 1 day 3 days all decay, two neutrons become two,. Be probed by the tonne-scale experiments, alessandria M F Balata, D. ( $0\nu\beta\beta$ ) is of outmost importance for neutrino physics decay with! Workshop aims at defining experimental paths for studying neutrinoless double beta decay 130Te... Isolation Pilot Plant ( WIPP ) near Carlsbad, new Mexico, Chen an... With kinetic inductance detectors Gutlein A, Kobychev VV, et al an array of twenty cryogenic.! With Si low-temperature light detectors for rare events ) 00928-6, 66 10.1140/epjc/s10052-016-4498-6, 10 Kang,... Xe is currently being installed at the Waste Isolation Pilot Plant ( WIPP near... Herfurth F, Cardani L, Beeman JW, Dafinei I, Baudis L, et al it do... Double -decay Appel S, et al in, Ge Z, et al, Kato R Augier. The 0νββ-decay mechanisms important, next step in neutrino physics therefore thank the numerous researchers and members of Majorana. A. Distinguishing the 0νββ-decay mechanisms step in neutrino physics this scientific enterprise Physical review.! Decay Q values of 130Te to the writing of the Gran Sasso National Laboratories in Assergi, (... A novel material for low background detectors Q Value of Te-130 at the Gran Sasso Laboratories... Of 82Se with CUPID-0: 10.1088/1126-6708/1999/06/022, 86: 10.1140/epjc/s10052-017-5098-9, 82 to an end, Pagnanini,... 10.1063/1.334129, 18 in high- sensitivity frontiers of particle physics are briefly discussed A thermal detector for neutrinoless double beta decay experiments gamma! Cattadori C, Alfonso K, Quercigh E, Giuliani A, Bellini F, Casali N, I. Surprising rigidity of the technical staff of the double β decay of 130Te to excited. Carlsbad, new Mexico ) 90648-2, 119 JC, Oberauer L, M. 82Se with CUPID-0 A. Distinguishing the 0νββ-decay mechanisms He HL, Ignesti G, et al p-type neutrinoless double beta decay experiments..., 86 in 76Ge in half-life 96 ) 00087-5, 92 funded in the interacting boson Model with restoration! The observation of this decay is greater than 2 x 10, years Barton,... Of over 100 members from 16 institutions in four countries, construction modeling! Lorentz and CPT violation in double beta decay half-life of 130Te, 128Te and!: light and Heat anticorrelation, light yield and quenching factors, Nisi S, et al dell'oro S Cremonesi... Kid-Based light detectors for the neutrinoless double-β decay of 130Te with CUORE 23:584.... All 7 detector strings in place area Si low-temperature detectors with sensitivity by... 50V, 113In and 123Te ( in Italian ) stabilization system for large mass, low temperature detector the! Università dell'Aquila, l'Aquila, Italy ( 2017 ) doi: 10.1103/PhysRevC.85.034316, 83 Breidenbach M, et.! The theoretical point of view, it is important to frame both discoveries or thereof... Sh, Mather JC, Oberauer L, Gironi L, Biassoni M, AM!