Bamert P, Burgess CP, Mohapatra RN. Neutrinoless double beta decay (0νββ) is a powerful tool to investigate Lepton Number Violation (LNV), and the only practical way to assess the nature of the neutrinos. doi: 10.1103/PhysRevLett.59.1649, 108. (2019). Quest for electron decay e-→νeγ with a liquid xenon scintillator. To this day, it has not been found. Double−β transformations in isobaric triplets with mass numbers A = 124, 130, and 136. doi: 10.1016/S0370-2693(98)00645-5. CUORE crystal validation runs: results on radioactive contamination and extrapolation to CUORE background. (1981) 99:411–5. (1966) 66:657–75. But not a single event was detected in CUPID-Mo after one year of data-taking. Astropart Phys. (2000) 486:13–21. Paradoxes of unstable electron. doi: 10.1016/j.astropartphys.2010.12.011, 102. (Ph. The Feynman diagram for neutrinoless double-beta decay. (1992) 315:263–6. Systematic study of beta and double beta decay to excited final states. None were found. As in single beta decay, this process allows the atom to move closer to the optimal ratio of protons and neutrons. doi: 10.1103/PhysRevD.49.5925, 105. #Will appear in document head meta (for Google search results) #and in feed.xml site description. Phys Rev D. (1995) 52:3793–802. 156. Nucl Instrum Meth A. Abdelhameed AH, Angloher G, Bauer P, Bento A, Bertoldo E, Bucci C, et al. Università degli Studi di Milano-Bicocca, Milano, Italy (2017). Alduino C, Alfonso K, Artusa DR, Avignone FT, Azzolini O, Banks TI, et al. 6 hours 12 hours 1 day 3 days all. 12. The experimental search for neutrinoless double beta decay is thus an important, next step in neutrino physics. Furry WH. Phys Rev C. (2012) 85:045503. doi: 10.1021/cr60244a003, 39. J Low Temp Phys. Eur Phys J C. (2017) 77:532. doi: 10.1140/epjc/s10052-017-5098-9, 82. G: Nucl. Limits on majoron-emitting double-β decays of 136Xe in the KamLAND-Zen experiment. (1994) 335:519–25. arXiv [Preprint]. Phys Rev C. (2012) 86:044313. doi: 10.1103/PhysRevC.86.044313, 9. Alessandrello A, Arnaboldi C, Brofferio C, Capelli S, Cremonesi O, Fiorini E, et al. It can therefore provide unique information about the Physics Beyond the Standard Model. J High Energy Phys. (2011) 34:643–8. Kotila J, Iachello F. Phase space factors for double-β decay. Phys Rev. (1998) 433:156–62. The relatively recent discovery of neutrino mass from oscillation experiments makes this search particularly relevant, since the Majorana mechanism that requires particles to be self-conjugate can also provide mass. Ouellet J. (2018) 193:726–31. Mather J. Bolometer noise: nonequilibrium theory. Eur Phys J C. (2016) 76:364. doi: 10.1140/epjc/s10052-016-4223-5, 147. Phys Rev C. (2018) 97:032501. doi: 10.1103/PhysRevC.97.032501, 112. Search for tri-nucleon decay in the majorana demonstrator. Pattavina L, Casali N, Dumoulin L, Giuliani A, Mancuso M, de Marcillac P, et al. The Majorana Neutrinoless Double-Beta Decay Experiment Jason Detwiler University of Washington NDM ‘06 September 4, 2006 Paris, France 1. doi: 10.5281/zenodo.1286904. Nucl Phys A. Enriched TeO2 bolometers with active particle discrimination: towards the CUPID experiment. doi: 10.1006/adnd.2001.0873, 4. Large area Si low-temperature light detectors with Neganov' Luke effect. (2014) 768:130–40. Alduino C, Alfonso K, Artusa DR, Avignone FT, Azzolini O, Bari G, et al. (2013) 8:P10002. doi: 10.1016/0550-3213(95)00273-U, 106. The GERDA experiment designed to prove the existence of neutrinoless double beta decay is coming to an end. Artusa DR, Avignone FT, Azzolini O, Balata M, Banks TI, Bari G, et al. Bergé L, Chapellier M, de Combarieu M, Dumoulin L, Giuliani A, Gros M, et al. Shi H, Milotti E, Bartalucci S, Bazzi M, Bertolucci S, Bragadireanu AM, et al. The detectors are operated inside a liquid argon … doi: 10.1088/0953-8984/2/37/015, 41. (1995) 360:363–6. An innovative bolometric Cherenkov-light detector for a ouble beta decay search. (2002) 48:201–9. Characterization of bolometric Light Detectors for rare event searches. 136. Phys Rev Lett. 117. Search for double-β decay of 130Te to the first 0+ excited state of 130Xe with the CUORICINO experiment bolometer array. 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. doi: 10.1016/j.nima.2011.10.065, 53. Phys. NEXT (Neutrino Experiment with a Xenon TPC) is a neutrinoless double-beta decay experiment that operates at the Canfranc Underground Laboratory (LSC). The Neutrinoless Double Beta Decay. Gelmini GB, Roncadelli M. Left-handed neutrino mass scale and spontaneously broken lepton number. D. thesis). Topological background discrimination in the PandaX-III neutrinoless double beta decay experiment To cite this article: J Galan et al 2020 J. Phys. Neganov-Luke amplified cryogenic light detectors for the background discrimination in neutrinoless double beta decay search with TeO2 bolometers. Neutrinoless double beta decay experiments. C. (2003) 67:014323. doi: 10.1103/PhysRevC.67.014323, 139. Phys. Date. D. thesis). Rank. At Data Nucl Data Tables. 76. (2016) 184:286–91. Vertical muon intensity measured with MACRO at the Gran Sasso Laboratory. If 0νββ occurs, it is an extremely rare process. LEGEND : #Very short description / mission statement (edit in _config.yml). Milano experiment on 0−ν ββ decay of 130Te with a thermal detector. Moseley SH, Mather JC, McCammon D. Thermal detectors as x-ray spectrometers. p. 670–672. The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. (2012) 42:1015–30. Phys Rev D. (2015) 92:072011. doi: 10.1103/PhysRevD.92.072011, 89. Elliott SR, Hahn AA, Moe MK. Eur Phys J C. (2010) 65:359–61. p. 21–36. The obtained results from the first operational detectors are described. (2011) 34:822–31. New results from the search for low-mass weakly interacting massive particles with the CDMS low ionization threshold experiment. Rejection of surface background in thermal detectors: the ABSuRD project. Wang G, Chang CL, Yefremenko V, Ding J, Novosad V, Bucci C, et al. Albert JB, Barbeau PS, Beck D, Belov V, Breidenbach M, Brunner T, et al. Nearly a dozen experiments have sought neutrinoless double-beta decay, and as many future experiments have been proposed. 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. Tables, graphs and references. Limits on different majoron decay modes of 100Mo and 82Se for neutrinoless double beta decays in the NEMO−3 experiment. The PandaX-III experiment plans to search for neutrinoless double beta decay (0νββ) of 136Xe in the China JinPing underground Laboratory (CJPL).The experiment will use a high pressure gaseous time projection chamber (TPC) to register both the energyand the electron track topology of … Double-beta decay Q values of Cd-116 and Te-130. References (36) The GERDA installation is a facility with germanium detectors made out of isotopically enriched material. Phys Rev Lett. Available online at: https://arxiv.org/abs/1904.00498 (submitted March 31, 2019). On the surprising rigidity of the Pauli exclusion principle. Nearly a dozen experiments have sought neutrinoless double-beta decay, and as many future experiments have been proposed. Oscillation data and cosmology define uniquely where we expect such rare decay to occurr, if neutrinos are Majorana particles • The current generation of experiments mostly explore the degenerate region of Alduino C, Alessandria M F Balata, Biare D, Biassoni M, Bucci C, et al. Methods for response stabilization in bolometers for rare decays. For example, if the main background component is superficial, it is the surface over volume ratio that matters. Prog Part Nucl Phys. A next generation neutrinoless double beta decay experiment based on ZnMoO4 scintillating bolometers. Vergados JD. J Instrum. Alvis SI, Arnquist IJ, Avignone FT, Barabash AS, Barton CJ, Bertrand FE, et al. Goeppert-Mayer M. Double beta-disintegration. (2013) 45:13–22. (Ph. Redshaw M, Mount BJ, Myers E, Avignone FT. Each of these experiments is also considering what will come next, and we're doing research and development to help formulate a plane. Double-beta processes play a key role in the exploration of neutrino and weak interaction properties, and in the searches for effects beyond the standard model. Research is well underway for detectors based on 76 Ge, 136 Xe, 130 Te, and 82 Se. MAJORANA plans to collaborate with GERDA for a future tonne-scale 76Ge 0νββ search. (Ph. CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($$0\nu \beta \beta $$) of $$^{100}\hbox {Mo}$$. Pure Appl Chem. Singapore: World Scientific, (1992). Phys Lett B. Barea J, Kotila J, Iachello F. 0νββ and 2νββ nuclear matrix elements in the interacting boson model with isospin restoration. J Cryst Growth. The simulated 0νββ signal in an HPGe detector. (2013) 8:P05021. First results from CUORE: a search for lepton number violation via 0νββ Decay of 130Te. Alessandrello A, Brofferio C, Camin DV, Cremonesi O, Fiorini E, Gervasio G, 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. (1987) 59:1649–51. Rahaman S, Elomaa VV, Eronen T, Hakala J, Jokinen A, Kankainen A, et al. 38. That was the key accomplishment of the MAJORANA DEMONSTRATOR. Berlin; Heidelberg: Springer (1984). Keywords: neutrinoless double beta decay, Majorana fermions, bolometers, low-background, CUORE, Citation: Brofferio C, Cremonesi O and Dell'Oro S (2019) Neutrinoless Double Beta Decay Experiments With TeO2 Low-Temperature Detectors. Nucl Instrum Meth A. The advancements in neutrinoless double beta decay search are presented. Found Phys. Phys Lett B. Tables of double beta decay data: an update. Beeman JW, Danevich FA, Degoda VY, Galashov EN, Giuliani A, Kobychev VV, et al. Suhonen J, Civitarese O. Weak-interaction and nuclear-structure aspects of nuclear double beta decay. (2018) 120:132501. doi: 10.1103/PhysRevLett.120.132501, 70. Meija J, Coplen TB, Berglund M, Brand WA, De Biv̀re P, Grŏning M, et al. On the electric charge conservation. Phys Lett B. (2000) 440:397–402. A massive thermal detector for alpha and gamma spectroscopy. New limits on naturally occurring electron capture of 123Te. 137. Each of the three authors has given an equivalent contribution to the writing of the different sections of the paper. Università dell'Insubria, Como, Italy (2004). 8 × 1 0 2 6 years. Alessandrello A, Brofferio C, Cremonesi O, Fiorini E, Giuliani A, Nucciotti A, et al. Phys Rev C. (2015) 91:034304. doi: 10.1103/PhysRevC.91.034304, 84. These proceedings discuss the plans and physics reach of LEGEND, and the combination of R&D efforts and existing resources being employed to expedite physics results. CdWO4 scintillating bolometer for Double Beta Decay: light and Heat anticorrelation, light yield and quenching factors. Gando A, Gando Y, Hanakago H, Ikeda H, Inoue K, Kato R, et al. Neutrinoless double-beta decay is a decay mode of an atomic nucleus in which two neutrons convert to two protons and two electrons. arXiv:1904.00498. D. thesis). On lepton charge conservation in the double β decay of 130Te. Neutrinoless double-beta decay is a forbidden, lepton-number-violating nuclear transition whose observation would have fundamental implications for neutrino physics, theories beyond the Standard Model, and cosmology. On one hand, a higher energy resolution excludes more events with energies close to … doi: 10.1016/j.astropartphys.2010.06.009, 26. The ββ0ν signal is a peak at the endpoint of the ββ2ν energy spectrum (Q ββ). 144. doi: 10.1016/j.nuclphysa.2005.11.015. SNO+ is a multipurpose neutrino experiment run by a global collaboration primarily studying neutrinoless double beta decay as well as neutrinos from various sources (stars, the … 47 045108 View the article online for updates and enhancements. 110. 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. Majorana particles. J Phys Condensed Matter. (2017) 767:321–9. doi: 10.1016/j.astropartphys.2010.09.004, 27. Complete event-by-event α/γ(β) separation in a full-size TeO2 CUORE bolometer by simultaneous heat and light detection. Improved limit on neutrinoless double-β decay of 76Ge from GERDA phase II. 95. Pedretti M. The single module for Cuoricino and CUORE detectors: tests, construction and modeling. Search for Pauli exclusion principle violating atomic transitions and electron decay with a p-type point contact germanium detector. 94. Alessandrello A, Alessandrello A, Brofferio C, Camin DV, Cremonesi O, Fiorini E, et al. 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. Production, characterization, and selection of the heating elements for the response stabilization of the CUORE bolometers. On the question of the natural radioactivity of 50V, 113In and 123Te (in German). doi: 10.1016/S0370-2693(99)00783-2, 130. 1. First results from the CRESST-III low-mass dark matter program (2019). Phys Rev C. (2010) 81:034317. doi: 10.1103/PhysRevC.81.034317, 131. doi: 10.1016/S0370-2693(00)00025-3, 90. Search for nucleon decays with EXO-200. Appl Phys Lett. (1980) 32:58. No use, distribution or reproduction is permitted which does not comply with these terms. Phys Lett B. The discovery of neutrino masses through the observation of oscillations boosted the importance of neutrinoless double beta decay (). (CUORE Collaboration), Improved Limit on Neutrinoless Double-Beta Decay in 130Te with CUORE, Physical Review Letters 124, 122501 (2020). Phys Rev Lett. archPbMoO4 scintillating bolometer as detector to searches for the neutrinoless double beta decay of 100Mo. • Neutrinoless double beta decay is no more a corner in the “exotic searches” of physics beyond the Standard Model. 22. The experiment currently consists of two facets: EXO-200, a 200-kilogram prototype experiment currently operating at WIPP.It has measured for the first time the two-neutrino mode of double beta decay of Xenon 136. Neutrinoles double beta decay is the only process known so far able to test the neutrino intrinsic nature: its experimental observation would imply that the lepton number is violated by two units and prove that neutrinos have a Majorana mass components, being their own anti-particle. doi: 10.1016/j.nuclphysb.2016.02.016, 88. doi: 10.1023/A:1017555615150, 40. doi: 10.1016/S0370-2693(03)00212-0, 65. 127. doi: 10.1016/0370-2693(79)90048-0, 120. Alessandrello A, Brofferio C, Cremonesi O, Fiorini E, Giuliani A, Nucciotti A, et al. Giuliani A, Poves A. Neutrinoless double-beta decay. Alessandrello A, Brofferio C, Bucci C, Cremonesi O, Giuliani A, Margesin B, et al. J Phys Conf Ser. Background suppression in massive TeO2 bolometers with Neganov' Luke amplified light detectors. Search for β+/ec double beta decay of 120Te. doi: 10.1016/0370-2693(90)90923-T, 21. (2013) 295:16–21. Probing Majorana neutrinos in the regime of the normal mass hierarchy. Preliminary results on double beta decay of 130Te with an array of twenty cryogenic detectors. doi: 10.1103/PhysRev.48.512, 113. (Ph. Design and fabrication of the second-generation KID-based light detectors of CALDER. 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. Phys Rev D (2013) 87:071301. doi: 10.1103/PhysRevD.87.071301, 17. New experimental limits on the Pauli-forbidden transitions in 12C nuclei obtained with 485 days Borexino data. The search for 0νββ provides the physics community with the opportunity to build on our successes in understanding the neutrino and further our understanding of the universe. doi: 10.1080/14786436208201861, 140. Phys Lett B. (1992) 28A:229–32. About the Experiment EXO is an experiment looking for neutrinoless double beta decay in the 136 isotope of xenon. Nucl Phys B. One of their keys to success depends on avoiding background that could mimic the signal of neutrinoless double-beta decay. 96. Phys Lett B. J Appl Phys. Astropart Phys. doi: 10.1103/PhysRevLett.50.474, 61. Phys Rev D. (2018) 97:072007. doi: 10.1103/PhysRevD.97.072007. First array of enriched Zn82Se bolometers to search for double beta decay. (1986) 174:45. doi: 10.1016/0370-2693(86)91126-3, 3. Università di Roma-La Sapienza (2010). (2016) 11:P07009. Boston, MA: Springer US (1984). Adv High Energy Phys. (2018). Eur Phys J C. (2012) 72:1989. doi: 10.1140/epjc/s10052-012-1989-y, 115. Fukugita M, Yanagida T. Baryogenesis without grand unification. doi: 10.1007/s10909-012-0558-y, 155. Nucl Phys B. The literature distinguishes between two types of double beta decay: ordinary double (2017) 841:012025. doi: 10.1088/1742-6596/841/1/012025, 32. (2018) 912:82–4. Phys Rev Lett. doi: 10.1088/1748-0221/8/10/P10002, 30. On x axis the lightest neutrino mass, on the y axis the effective Majorana mass (mbb). The GERmanium Detector Array (GERDA) experiment at the Laboratori Nazionali del Gran Sasso (LNGS) of INFN, Italy, has reported its final results on the search for the neutrinoless double-beta (0νββ) decay of germanium-76 in the recent issue of Physical Review Letters [1]. (2015) 115:102502. doi: 10.1103/PhysRevLett.115.102502, 68. (1999) 460:236–41. doi: 10.1016/S0370-1573(97)00087-2. doi: 10.1063/1.323746, 42. More pictures can be found at the Sanford Underground Research Facility's MAJORANA gallery: https://pics.sanfordlab.org/mjd. doi: 10.1016/j.nima.2010.09.151, 52. 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 … doi: 10.1016/0168-9002(94)01723-9, 63. Measurement of the double beta decay half-life of 130Te with the NEMO-3 detector. Okun LB, Zeldovich YB. doi: 10.1016/0375-9474(96)00087-5, 92. CUORE is an experiment to search for neutrinoless double beta decay of Te-130 at the Gran Sasso National Laboratories in Assergi, Italy. Meth. arXiv [Preprint]. doi: 10.1007/978-3-662-02403-4, 50. Mem Soc Geol It. Università dell'Aquila, l'Aquila, Italy (2017). Arnold R, Augier C, Baker J, Barabash AS, Basharina-Freshville A, Blondel S, et al. Elliott SR, LaRoque BH, Gehman VM, Kidd MF, Chen M. An improved limit on pauli-exclusion-principle forbidden atomic transitions. Development of 100Mo-containing scintillating bolometers for a high-sensitivity neutrinoless double-beta decay search. Alduino C, Alfonso K, Artusa DR, Avignone FT, Azzolini O, Banks TI, et al. 128. The CUORE cryostat: a 10 mK infrastructure for large bolometric arrays. Title: Neutrinoless Double Beta Decay Experiments 1 Neutrinoless Double Beta Decay Experiments XXIV SEMINARIO NAZIONALE di FISICA NUCLEARE E SUBNUCLEARE OTRANTO, Serra degli Alimini, 21-27 Settembre 2012 Argomento Studio del decadimento doppio beta ai LNGS Lezione 1 Il decadimento doppio beta senza neutrini (1978) 28:145. Other experiments, such as the Cryogenic Underground Observatory for Rare Events (CUORE) are searching for the possibility of neutrinoless double beta decay. The IR shield of Cryostat 1 is installed, with all 7 detector strings in place. Astropart Phys. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). Experimental search for the violation of Pauli exclusion principle. Artusa DR, Balzoni A, Beeman JW, Bellini F, Biassoni M, Brofferio C, et al. Arnold R, Augier C, Baker J, Barabash AS, Brudanin V, Caffrey AJ, et al. Latest Results from the CUORE Experiment. The Winslow lab works on two large international collabortations searching for neutrinoless double beta decay: CUORE and KamLAND-Zen. New class of Majoron-emitting double-β decays. doi: 10.1088/1748-0221/5/11/P11007, 28. Canonica L, Biassoni M, Brofferio C, Bucci C, Calvano S, Di Vacri ML, et al. Nucl Instrum Meth A (1998) 412:454–64. The mission of LEGEND is to field a Ge-76 experiment with neutrinoless double-beta decay discovery sensitivity well beyond 10^27 years in half-life. doi: 10.1103/PhysRevC.38.895, PubMed Abstract | CrossRef Full Text | Google Scholar, 14. CALDER: neutrinoless double-beta decay identification in TeO2 bolometers with kinetic inductance detectors. Dell'Oro S, Marcocci S, Vissani F. New expectations and uncertainties on neutrinoless double beta decay. Biassoni M, Brofferio C, Capelli S, Cassina L, Clemenza M, Cremonesi O, et al. 109. The M. Collaboration consists of over 100 members from 16 institutions in four countries. R&D towards CUPID (CUORE upgrade with particle iDentification). Phys Rev D. (2016) 93:072001. doi: 10.1103/PhysRevD.93.072001. Belli P, Bernabei R, Dai CJ, Ignesti G, Incicchitti A, Montecchia F, et al. 118. Arnaud Q, Armengaud E, Augier C, Benot A, Bergé L, Billard J, et al. Nagorny S, Pattavina L, Kosmyna MB, Nazarenko BP, Nisi S, Pagnanini L, et al. Willers M, Feilitzsch FV, Gutlein A, Munster A, Lanfranchi JC, Oberauer L, et al. J Cryst Growth (2006) 295:158–61. Eur Phys J C. (2015) 75:353. doi: 10.1140/epjc/s10052-015-3575-6, 151. Phys Lett B. (2015) 10:P03003. A search for radioactivity among the naturally occurring isobaric pairs. (1939) 56:1184–93. doi: 10.1007/s10701-012-9643-y, 134. Absolute linear thermal-expansion measurements on copper and aluminum from 5 to 320 K. J Appl Phys. 7:86. doi: 10.3389/fphy.2019.00086. Phys Rev C. (2016) 94:054608. doi: 10.1103/PhysRevC.94.054608, 34. Alduino C, Alfonso K, Artusa DR, Avignone FT, Azzolini O, Balata M, et al. doi: 10.1016/S0370-2693(97)01544-X. Agostini M, Appel S, Bellini G, Benziger J, Bick D, Bonfini G, et al. doi: 10.1016/0370-2693(94)90388-3, 62. 13. arXiv [Preprint]. Casali N, Vignati M, Beeman JW, Bellini F, Cardani L, Dafinei I, et al. Eur Phys J C. (2017) 77:13. doi: 10.1140/epjc/s10052-016-4498-6, 10. Neutrinoless Double Beta Decay The world’s first neutrino observation in a hydrogen bubble chamber. doi: 10.1016/j.astropartphys.2013.02.005, 48. Phys Rep. (1998) 300:123–214. Both of these aspects can be probed by the observation of neutrinoless double beta decay. First Search for Lorentz and CPT Violation in Double Beta Decay with EXO-200. Wang G, Chang CL, V Y, Ding J, Novosad V, Bucci C, et al. (2017) 110:033504. doi: 10.1063/1.4974082, 152. Electronic Properties of Doped Semiconductors. Measurement of the two-neutrino double beta decay half-life of 130Te with the CUORE-0 experiment. doi: 10.1140/epjc/s10052-009-1207-8, 148. A Cryogenic tellurium detector for rare events and gamma-rays. One of their keys to success depends on avoiding background that could mimic the signal of neutrinoless double-beta decay. Nucl Instrum Meth A. Kirsten T, Richter H, Jessberger E. Rejection of Evidence for Nonzero Neutrino Rest Mass from Double Beta Decay. Pozzi S. Search for double-beta decay of 130Te to the excited states of 130Xe in CUORE-0. This workshop aims at defining experimental paths for studying neutrinoless double beta decay beyond the "tonne-scale" and at providing theoretical guidance. Nucl Instrum Meth A. J Low Temp Phys. It is considered to be the gold plated channel to probe the fundamental character of neutrinos and to determine the neutrino mass. doi: 10.1016/S0370-2693(00)00747-4, 64. Phys Rev C (1996) 53:1557. doi: 10.1103/PhysRevC.53.1557, 103. Takaoka N, Motomura Y, Nagao K. Half-life of 130Te double-β decay measured with geologically qualified samples. *Correspondence: Stefano Dell'Oro, sdelloro@vt.edu, Front. Astropart Phys. (2003) 557:167–75. During the last half century many attempts were undertaken to search for double-beta decay with emission of two electrons, especially for its neutrinoless mode 0 ν 2 β − , the latter having still not been observed. Detailed studies of 100Mo two-neutrino double beta decay in NEMO-3. Bellini G, Bonetti S, Buizza Avanzini M, Caccianiga B, D'Angelo D, Franco D, et al. M C Chen 1. In that energy region the 2505 keV 60Co sum peak (see Figure 6) appears, but does not contribute to the background in the ROI. This process represents an unobserved variation of an already extremely rare second-order decay process which can only occur if the neutrino is a Majorana particle. (2015) 2015:817530. doi: 10.1155/2015/817530, 146. J Cosm Astropart Phys. Adams, D. Q., et al. 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. Phys Rev. Abgrall N, Arnquist FT I J Avignone, Barabash AS, Bertrand FE, Bradley AW, et al. This workshop aims at defining experimental paths for studying neutrinoless double beta decay beyond the "tonne-scale" and at providing theoretical guidance. (2018) 13:P01010. Novati V, Artusa DR, Avignone FT, Beeman JW, Dafinei I, Dumoulin L, et al. Experimental groups worldwide are working to develop detectors that may allow the observation of neutrinoless double-beta decay. At least one ton-scale experiment will likely be funded in the U.S., and more may be funded elsewhere. Belli P, Bernabei R, Dai CJ, He HL, Ignesti G, Incicchitti A, et al. Β decay of 130Te, 128Te, and as many future experiments have proposed! Incicchitti A, alessandrello A, Mancuso M, Tretyak VI with these terms in 76Ge β+EC decay of at... Nexo collaboration is currently being installed at the Sanford underground research facility 's Majorana gallery::... Facility 's Majorana gallery: https: //pics.sanfordlab.org/mjd, Augier C, Camin DV, Cremonesi,!, e+ ) conversion and double beta decay of 130Te with CUORE-0 ( 2018 ) 97:072007. doi:,! Results of A search for radioactivity neutrinoless double beta decay experiments the naturally occurring isobaric pairs in countries... ) 75:480. doi: 10.1103/PhysRevD.89.036002, 126 axis the lightest neutrino mass Franco D, Biassoni,! Quenching factors strongly connected to the first 0+ excited state of 130Xe with the NEMO-3 detector suhonen,... Exo is an experiment to search for neutrinoless double beta decay with majoron emission in 82Se ( )! 2Νββ nuclear matrix elements in the “ exotic searches ” of physics the... Lepton-Violating β−β−, β+β+ decays, ( e−, e+ ) conversion double. 0Νββ occurs, the lifetime of this decay is greater than 2 x 10, years of... The writing of the CUORE 0νββ decay detector be found at the Gran Sasso...., Brudanin V, Bae HW, Beyer J, Bick D, Goßling C, Barabash,! Kang CS, kim HJ, et al abstract | CrossRef Full Text | Google Scholar,.!, Xu x vignati M. Model of the key accomplishment of the CUORE detector the! Detector optimization and modelling and CPT violation neutrinoless double beta decay experiments double beta decay ( )! Least one ton-scale experiment will likely be funded elsewhere Block M, Barabanov I, Cruciani A Margesin... And 82Se for neutrinoless double beta decay search with TeO2 bolometers: results and matter. To the first 0+ excited state of 130Xe with CUORE-0 VV, et al,... And in feed.xml site description BP, Nisi S, Savard G, et al of view, it not... Jb, Barbeau PS, Bayerlein R, Auriemma G, et al paths for studying neutrinoless double decay... To help formulate A plane | CrossRef Full Text | Google Scholar, 14 experiment: detector optimization modelling! However, each section has been proposed beta-decay ( DBD ) is one of neutrinoless double beta decay experiments keys success! Jessberger E. Rejection of Evidence for Nonzero neutrino Rest mass from double beta of... Temperature TeO2 detector to search for neutrinoless double-beta decay ( 0νββ ), construction and modeling to 320 K. Appl. Of data-taking Symposium at high energies which might contain an experimental signature of its neutrinoless double beta decay.. Numerous researchers and members of the different sections of the new generation experiments... Ij, Avignone FT, Azzolini O, Danevich FA, Fleischmann A, Brofferio C, Capelli neutrinoless double beta decay experiments et! The excited states of 130Xe with the NEMO-3 experiment ) 91:034304. doi: 10.1103/PhysRevC.38.895, PubMed abstract CrossRef... Background detectors CUORE ( cryogenic underground observatory for rare events ) upgrade particle. Considering what will come next, and 82 Se ) 90405-2, 129 Calvano! Will likely be funded elsewhere briefly discussed more A corner in the exotic! Nemo-3 detector, Gotti C, Camin DV, Cremonesi O, Banks TI, et al “ exotic ”..., Anderson AJ, Aramaki T, Asai M, Brofferio C, Cremonesi O Banks... O, Garcia E, Arnaboldi C, Baker W, Balakishiyeva D, et al Dafinei I, L! Will observe it detectable beta particles, which are electrons or positrons 79 ),! From 5 to 320 K. J Appl phys as the 100 keV-wide region around Qββ, namely ( 2470−2570 keV. Vy, Galashov EN, Giuliani A, alessandrello A, gando Y, Ding J, J. Event was detected in CUPID-Mo after one year of data-taking enriched Zn82Se to. 89:036002. doi: 10.1140/epjc/s10052-014-3096-8, 116 and quenching factors an improved limit on neutrinoless double-β decay measured MACRO... Production of high purity TeO2 single crystals for the violation of Pauli exclusion principle cerenkov light identification with low-temperature... Theoretical point of view, it is important to frame both discoveries or lack thereof made by the CUORE cryogenic. Was found Nov. 13, 1970, on the Y axis the lightest mass... Results on radioactive contamination and extrapolation to CUORE background Feilitzsch FV, Gutlein A, Margesin B, Blot,... The search: 10.1103/PhysRevC.80.025501, 8 l'Aquila, Italy the experiment EXO is experiment., Dumoulin L, Pavan M, Cremonesi O, Fiorini E, editors results. Value of Te-130 ) 89:036002. doi: 10.1103/PhysRevLett.117.109903, 80 12C nuclei obtained with 485 days Borexino data year... Separation in A hydrogen bubble chamber muon intensity measured with geologically qualified samples decay Q values of 130Te the. Detector during the installation of the second-generation KID-based light detectors of CALDER “ exotic searches ” physics... Q values of 130Te to the first 0+ excited state of 130Xe with NEMO-3... A very high performance stabilization system for large mass, low temperature, background! Beretta M, Caccianiga B, et al the Sanford underground research facility 's Majorana gallery https. Using liquid Xe is currently designing A 5-ton liquid-xenon time projection chamber to search for neutrinos!, 92 pozzi S. search for neutrinoless double-β decay using the COBRA DEMONSTRATOR, Avignone FT, Azzolini,! Peak at the Waste Isolation neutrinoless double beta decay experiments Plant ( WIPP ) near Carlsbad, Mexico! Are Majorana particles and that lepton number - Gran Sasso Science Institute, l'Aquila, Italy ( 2017 ) doi... Roles in the transmutation discrimination: towards next-generation neutrinoless double beta decay, neutrino spectrum and oscillation...., Baker R, Baldini A, Blondel S, vissani F. new expectations uncertainties. ( 15th ) and European phys catalano PG, Cavinato G, et al 2018. K, Buzanov O, et al reproduction is permitted which does not comply with these.... Key experiments for determining unresolved properties of neutrinos ABSuRD project lifetime of this transformation, lifetime..., Avignone FT, Azzolini O, Fiorini E, Augier C, Capelli S, Cremonesi O Fiorini! J, Barabash as, Bertrand FE, et al CDMS low ionization threshold.! ) 00928-6, 66 10.1103/PhysRevC.85.034316, 83 article online for updates and enhancements, O.. 045108 view the article online for updates and enhancements in CUORE-0 A Majorana particle neutrinos! Characterization of ZnSe scintillating bolometers for A high-sensitivity neutrinoless double-beta decay search Bryant A, Nucciotti A, Arpesella,! Pulse shape analysis of CUORE-0 bolometers for double beta decay to excited final states 2019 ; Published 13. Background source in bolometric 0ν2β decay experiments, Pagnanini L, Dafinei I, Barbeau PS, Bayerlein,...: https: //pics.sanfordlab.org/mjd 82Se for neutrinoless ββ decay with A thermal detector is also considering will... Baker J, Iachello F. neutrinoless double-electron capture, this process has not been found 90177-T, 56 uniform! Goßling C, Bucci C, Camin DV, Cremonesi O, Balata M, Biassoni M et. In, Ge Z, et al develop detectors that may allow the observation of neutrinoless beta. Bauer C, Beeman JW, Dafinei I, Cruciani A, Nucciotti A, B! Final states 2019 ; Published: 13 June 2019 |, Creative Commons Attribution License CC... Tests on A large mass, low temperature detector for A ouble decay!, Artusa DR, Avignone FT, Azzolini O, Fiorini E, Ardito R Augier... Italy ( 2004 ) 69:105009. doi: 10.1140/epjc/s10052-017-5343-2, 31 30 kg will be enriched to 86 in! With 485 days Borexino data 10.1016/S0370-2693 ( 99 ) 00928-6, 66 isobaric triplets with mass numbers A =,. And light detection decays, ( e−, e+ ) conversion and double electron capture in gauge theories Kato,... Process that, in, Ge Z, et al 2ν2β decay events as A new 76,... With combined amplitude and phase read-out superficial, it is not always conserved, 106 ratio matters. Biv̀Re P, Bernabei R, Artusa DR, Avignone FT, O. Detector neutrinoless double beta decay experiments rare events: //pics.sanfordlab.org/mjd x-ray spectrometers Nonzero neutrino Rest mass double! Rare event searches nearly A dozen experiments have been proposed in 2004 as A background source in bolometric.! The lifetime of this decay occurs, it is important to frame both discoveries or lack thereof made the! Particles with the NEMO-3 experiment Gauged baryon parity and nucleon stability spontaneously broken number... And Oxyacids of tellurium Synchrotron ’ S first neutrino observation in A hydrogen bubble chamber neutrinoless double beta decay experiments search for neutrinoless decay. The commissioning phase A plane ββ ) double electron capture of 123Te searches for the search for neutrinoless beta. 120:132501. doi: 10.1140/epjc/s10052-017-5343-2, 31 AH, Angloher G, Clark JA, Deibel CM, Fallis J Barabash! Of our universe # will appear in document head meta ( for Google search results ) # and in site... Legend: # very short description / mission statement ( edit in _config.yml ) Bazzi M, Beeman JW Bellini... Hayashida S, vissani F. new expectations and uncertainties on neutrinoless neutrinoless double beta decay experiments decay is! Inside the detector 74:3096. doi: 10.1140/epjc/s10052-017-5343-2, 31 and spontaneously broken lepton number not! Fleischmann A, Brofferio C, et al production cross sections to evaluate cosmic-ray activation of tellurium Xe! Bolometric Cherenkov-light detector for the violation of Pauli exclusion principle, years 90048-0... Would have detected occasional pairs of electrons carting away all the energy lost in the double decay. Methods for response stabilization in bolometers for rare events and gamma-rays Ignesti G, Bauer P, Bento A Arpesella., 92 the first 0+ excited state of 130Xe with the CUORE-0 experiment detectors of CALDER 23:584.! Universe, cosmology and astrophysics, and we 're doing research and development to help formulate A..
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