Conveners
Double Beta decays and Neutrino Masses: (Room 1)
- Fabio Pupilli (PD)
- Filippo Varanini (INFN Padova)
Double Beta decays and Neutrino Masses: (Room 1)
- Fabio Pupilli (PD)
- Filippo Varanini (INFN Padova)
Double Beta decays and Neutrino Masses: (Room 1)
- Christian Farnese (PD)
- Chiara Sirignano (PD)
Double Beta decays and Neutrino Masses: (Room 1)
- Christian Farnese (PD)
- Fabio Pupilli (PD)
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Dr Guido Fantini (Università di Roma 1 La Sapienza, Sezione INFN di Roma)23/02/2021, 10:00Neutrino Masses and MixingsParallel Contributed Talk
The Cryogenic Underground Observatory for Rare Events (CUORE) is the first bolometric experiment searching for neutrinoless double-beta (0νββ) decay that has been able to reach the one-ton scale. The detector, located at the Laboratori Nazionali del Gran Sasso in Italy, consists of an array of 988 TeO2 crystals arranged in a compact cylindrical structure of 19 towers. Following the completion...
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Hideyoshi Ozaki (RCNS, Tohoku University)23/02/2021, 10:20Neutrino Masses and MixingsParallel Contributed Talk
KamLAND-Zen 800 is a neutrinoless double-beta decay search experiment with the Kamioka Liquid-scintillator Anti-electron Neutrino Detector (KamLAND). In 2019, we started KamLAND-Zen 800 experiment with 745 kg of xenon. We achieved the background reductions by reducing the radioactive materials in the newly fabricated 25-μm-thick nylon film container for the Xe-loaded LS and developing a new...
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Dr Lior Arazi (Ben-Gurion University)23/02/2021, 10:40Neutrino Masses and MixingsParallel Contributed Talk
NEXT is a staged experimental program aiming at the detection of neutrinoless double beta (ββ0ν) decay in 136Xe using successive generations of high-pressure gaseous xenon time projection chambers. The collaboration is presently concluding four years of operation of NEXT-White, a radiopure 50-cm diameter and length TPC operated with enriched xenon at 10 bar, at the Laboratorio Subterràneo de...
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Tommaso Comellato (Technical University of Munich)23/02/2021, 11:00Neutrino Masses and MixingsParallel Contributed Talk
Neutrinoless double beta decay (0νββ) is a hypothetical lepton number violating nuclear process which creates matter without a compensation of anti-matter. If observed, it would give an insight on why our universe is predominantly composed of matter. Furthermore, it would reveal the Majorana nature of neutrinos, namely that they are equal to their anti-matter counterpart, and possibly explain...
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Ms Elisabetta Bossio (Physik-Department, Technische Universität München)23/02/2021, 11:35Neutrino Masses and MixingsParallel Flash talk
Double beta decay is predicted in the Standard Model with the emission of two active neutrinos. Models in which light exotic fermions are emitted, replacing one or both the neutrinos in the final state, could be tested through the search for spectral distortions in the electron spectrum with respect to the Standard Model expectations. In this contribution the discovery potential of a selection...
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Prof. Zoraida Freixa (University of the Basque Country (UPV/EHU))23/02/2021, 11:40Neutrino Masses and MixingsParallel Flash talk
It has been recently shown that the identification of the single positively-charged ion Ba2+ produced in double beta decay events in Xe-136 may be possible in a high-pressure gas TPC using molecular indicators. The NEXT collaboration is pursuing an intense R&D program geared towards a future detector able to detect “tag” the Ba2+ produced in such events, a technique that could lead to an...
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Emanuela Celi (Istituto Nazionale di Fisica Nucleare)23/02/2021, 11:45Neutrino Masses and MixingsParallel Flash talk
The development of cryogenic calorimeters to search for neutrinoless double-beta decay (0$\nu$DBD) has given in the last years increasingly promising results. The possibility of achieving ton-scale exposures, maintaining an excellent energy-resolution, makes this kind of detector very suitable for a next-generation experiment.
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In order to achieve a nearly background-free condition,... -
Alice Campani (GE)23/02/2021, 11:50Neutrino Masses and MixingsParallel Flash talk
The search for $0 \nu EC \beta^+$ of $^{120}$Te with CUORE
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Alice Campani (on behalf of the CUORE collaboration)
Università degli studi di Genova – INFN
CUORE (Cryogenic Underground Observatory for Rare Events) is a ton-scale experiment located at the LNGS searching for neutrinoless double beta decay of $^{130}$Te. The detector consists of TeO$_2$ crystals operated as cryogenic calorimeters.... -
Alberto Ressa23/02/2021, 12:05Neutrino Masses and MixingsParallel Flash talk
The next generation experiment CUPID will search for neutrinoless double beta decay using scintillating Li$_2$MoO$_4$ bolometers to study the candidate isotope $^{100}$Mo. The scintillating properties of these crystals allow for the dual read-out of heat and light signals to suppress the background induced by alpha particles. This feature, together with the high Q-value of $^{100}$Mo, will...
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Mr Stefano Ghislandi (Gran Sasso Science Institute)23/02/2021, 12:10Neutrino Masses and MixingsParallel Flash talk
I present dedicated studies and measurements aiming to the reduction of the $\gamma$ background in the $0\nu\beta\beta$ ROI for TeO$_{2}$ calorimeters. This is mainly due to 2615 keV $\gamma$'s scattering Compton with materials next to the detectors. It can be lowered by replacing the usual copper holders with organic compounds structures. TeO$_{2}$ crystals, positioned in a PMMA holder, have...
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Juliana Stachurska (MIT)23/02/2021, 12:15Neutrino Masses and MixingsParallel Flash talk
Project 8 is a next-generation direct neutrino mass experiment using tritium beta decay. To reach the target sensitivity of 40meV, major technological development is necessary. Building up on the milestones achieved so far, I will present the next developmental phases of Project 8: In Phase III, atomic tritium will be trapped magnetically, and cyclotron radiation emission spectroscopy (CRES)...
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Stefano Dell'Oro (UniMib)23/02/2021, 12:20Neutrino Masses and MixingsParallel Flash talk
In this talk, I will briefly describe the technique we developed to study the pile-up rejection capability of cryogenic bolometers. The precise characterization of the detector time resolution is indeed of crucial importance for next-generation cryogenic-bolometer experiments searching for neutrinoless double-beta decay, such as CUPID, in order to discriminate against the pile-up of...
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Dr Tom Neep23/02/2021, 12:25Neutrino Masses and MixingsParallel Flash talk
The search for neutrinoless double beta decay could cast light on one critical piece missing in our knowledge i.e. the nature of the neutrino mass. Its observation is indeed the most sensitive experimental way to prove that neutrino is a Majorana particle. The observation of such a potentially rare process demands a detector with an excellent energy resolution, an extremely low radioactivity...
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Reyco Henning (UNC Chapel Hill)23/02/2021, 17:30Neutrino Masses and MixingsParallel Contributed Talk
The Large Enriched Germanium Experiment for Neutrinoless $\beta\beta$ Decay (LEGEND) program is a search for the neutrinoless double-beta decay of the $^{76}$Ge isotope. Its first phase, LEGEND-200, uses 200-kg of enriched high-purity germanium (HPGe) detectors in an active liquid argon shield and is currently under construction at the Laboratori Nazionali del Gran Sasso (LNGS) in Italy. It...
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Ian Guinn (University of North Carolina at Chapel Hill)23/02/2021, 17:50Neutrino Masses and MixingsParallel Contributed Talk
The Majorana Demonstrator is searching for neutrinoless double beta decay ($0\nu\beta\beta$) in $^{76}$Ge, a beyond the standard model second order nuclear process whose discovery would indicate that the neutrino is a Majorana fermion. The experiment consists of a modular array of 44 kg of p-type point contact (PPC) high-purity germanium detectors (HPGe), 30 kg of which are enriched to 88% in...
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Dr Brian Lenardo (Stanford University)23/02/2021, 18:10Parallel Contributed Talk
The search for neutrinoless double beta decay (NDBD) provides the most sensitive experimental test of lepton number conservation, as well as a powerful experimental probe of the nature and mass scale of the neutrino. In this talk, I will introduce the nEXO experiment: a proposed next-generation search for the neutrinoless double beta decay of $^{136}$Xe with a halflife sensitivity of...
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Walter Pettus (Indiana University)23/02/2021, 18:30Neutrino Masses and MixingsParallel Contributed Talk
Project 8 is a tritium endpoint neutrino mass experiment utilizing a phased program to achieve sensitivity to the range of neutrino masses allowed by the inverted mass ordering. The Cyclotron Radiation Emission Spectroscopy (CRES) technique is employed to measure the differential energy spectrum of relativistic decay electrons with high precision. In Phase II, the CRES technique was extended...
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Andrea Giuliani (CUPID collaboration)24/02/2021, 10:20Neutrino Masses and MixingsParallel Contributed Talk
CUPID is a next-generation tonne-scale bolometric neutrinoless double
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beta decay experiment to probe the Majorana nature of neutrinos and
discover Lepton Number Violation if the effective neutrino mass is
greater than 10 meV. CUPID will be built on experience, expertise and
lessons learned in CUORE, and will be installed in the current CUORE
infrastructure in the Gran Sasso underground... -
Pia Loaiza24/02/2021, 10:40Neutrino Masses and MixingsParallel Contributed Talk
The CUPID-Mo experiment is devoted to the search of neutrinoless double beta decay, 2β0ν. This small-scale array of scintillating bolometers has set in 2020 the best limit to the half-live of 2β0ν in 100Mo, with 2.17 kg x y of exposure. CUPID-Mo has demonstrated the maturity of the scintillating bolometric technique for CUPID (Cuore Upgrade with Particle Identification), the next generation...
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Mr Thierry Lasserre (CEA)24/02/2021, 11:00Neutrino Masses and MixingsParallel Contributed Talk
I will report on the light sterile neutrino search from the first four-week science run of the KATRIN experiment. Beta-decay electrons from a high-purity gaseous molecular tritium source are analyzed by a high-resolution MAC-E filter down to 40 eV below the endpoint at 18.57 keV. The analysis of the spectral shape of the spectrum near the endpoint leads to an improvement over the previous...
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