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Neutrinoless Double Beta Decay / Adams, C. (Argonne) ; Alfonso, K. (Virginia Tech.) ; Andreoiu, C. (Simon Fraser U., Burnaby (main)) ; Angelico, E. (SLAC) ; Arnquist, I.J. (PNL, Richland) ; Asaadi, J.A.A. (Texas U., Arlington) ; Avignone, F.T. (South Carolina U.) ; Axani, S.N. (Delaware U.) ; Barabash, A.S. (Moscow, ITEP) ; Barbeau, P.S. (Duke U. ; TUNL, Durham) et al.
This White Paper, prepared for the Fundamental Symmetries, Neutrons, and Neutrinos Town Meeting related to the 2023 Nuclear Physics Long Range Plan, makes the case for double beta decay as a critical component of the future nuclear physics program. [...]
arXiv:2212.11099 ; FERMILAB-CONF-22-962-ND. - 20.
Fermilab Library Server - Fulltext - Fulltext

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Sensitivity projections for a dual-phase argon TPC optimized for light dark matter searches through the ionization channel / Global Argon Dark Matter Collaboration
Dark matter lighter than 10 GeV/c$^2$ encompasses a promising range of candidates. A conceptual design for a new detector, DarkSide-LowMass, is presented, based on the DarkSide-50 detector and progress toward DarkSide-20k, optimized for a low-threshold electron-counting measurement. [...]
arXiv:2209.01177.- 2023-06-01 - 19 p. - Published in : Phys. Rev. D 107 (2023) 112006 Fulltext: 2209.01177 - PDF; 91ce6168799b33f720d8ae133fe8e56d - PDF; External link: Fermilab Library Server

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Separating $^{39}$Ar from $^{40}$Ar by cryogenic distillation with Aria for dark matter searches / DarkSide Collaboration
The Aria project consists of a plant, hosting a 350 m cryogenic isotopic distillation column, the tallest ever built, which is currently in the installation phase in a mine shaft at Carbosulcis S.p.A., Nuraxi-Figus (SU), Italy. Aria is one of the pillars of the argon dark-matter search experimental program, lead by the Global Argon Dark Matter Collaboration. [...]
arXiv:2101.08686.- 2021-04-26 - 18 p. - Published in : Eur. Phys. J. C 81 (2021) 359 Article from SCOAP3: PDF; Fulltext: PDF; Fulltext from Publisher: PDF;

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Sensitivity of future liquid argon dark matter search experiments to core-collapse supernova neutrinos / DarkSide 20k Collaboration
Future liquid-argon DarkSide-20k and ARGO detectors, designed for direct dark matter search, will be sensitive also to core-collapse supernova neutrinos, via coherent elastic neutrino-nucleus scattering. This interaction channel is flavor-insensitive with a high-cross section, enabling for a high-statistics neutrino detection with target masses of $\sim$50~t and $\sim$360~t for DarkSide-20k and ARGO, respectively. [...]
arXiv:2011.07819.- 2021-03-15 - 22 p. - Published in : JCAP 2103 (2021) 043 Fulltext: 2011.07819 - PDF; fermilab-pub-20-601-nd-ppd - PDF; External link: Fermilab Library Server (fulltext available)

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SiPM-matrix readout of two-phase argon detectors using electroluminescence in the visible and near infrared range / DarkSide Collaboration
Proportional electroluminescence (EL) in noble gases is used in two-phase detectors for dark matter searches to record (in the gas phase) the ionization signal induced by particle scattering in the liquid phase. The "standard" EL mechanism is considered to be due to noble gas excimer emission in the vacuum ultraviolet (VUV). [...]
arXiv:2004.02024; FERMILAB-PUB-20-155-PPD.- 2021-02-15 - 26 p. - Published in : Eur. Phys. J. C 81 (2021) 153 Article from SCOAP3: PDF; Fulltext: 2004.02024 - PDF; fermilab-pub-20-155-ppd - PDF; External link: Fermilab Library Server (fulltext available)

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Design and construction of a new detector to measure ultra-low radioactive-isotope contamination of argon / DarkSide Collaboration
Large liquid argon detectors offer one of the best avenues for the detection of galactic weakly interacting massive particles (WIMPs) via their scattering on atomic nuclei. The liquid argon target allows exquisite discrimination between nuclear and electron recoil signals via pulse-shape discrimination of the scintillation signals. [...]
arXiv:2001.08106.- 2020-02-26 - 19 p. - Published in : JINST 15 (2020) P02024 Fulltext: fermilab-pub-20-023-ppd - PDF; 2001.08106 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server (fulltext available)

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Flux Modulations seen by the Muon Veto of the GERDA Experiment / GERDA Collaboration
The GERDA experiment at LNGS of INFN is equipped with an active muon veto. The main part of the system is a water Cherenkov veto with 66~PMTs in the water tank surrounding the GERDA cryostat. [...]
arXiv:1601.06007.- 2016-11 - 7 p. - Published in : Astropart. Phys. 84 (2016) 29-35 Preprint: PDF; External link: Preprint

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Measurement of CNGS muon neutrino speed with Borexino / Borexino Collaboration
We have measured the speed of muon neutrinos with the Borexino detector using short-bunch CNGS beams. The final result for the difference in time-of-flight between a =17 GeV muon neutrino and a particle moving at the speed of light in vacuum is {\delta}t = 0.8 \pm 0.7stat \pm 2.9sys ns, well consistent with zero..
arXiv:1207.6860.- 2012-10-02 - 6 p. - Published in : Phys. Lett. B 716 (2012) 401-405 Fulltext: PDF; External link: Preprint

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Search for Electron Decay Mode e^-\to\gamma +\nu_e with Prototype of Borexino Detector / Back, H O ; Balata, M ; De Bari, A ; Beau, T ; De Bellefon, A ; Bellini, G ; Benziger, J B ; Bonetti, S ; Buck, C ; Caccianiga, B et al.
The prototype of the Borexino detector Counting Test Facility, located in the Gran Sasso laboratory, has been used to obtain a bound on the stability of the electron. [...]
E1-2002-30 ; JINR-E1-2002-30. - 2002. - 19 p.
Fulltext from JINR Dubna

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10.

Study of the Neutrino Electromagnetic Properties with Prototype of Borexino Detector / Back, H O ; Balata, M ; De Bari, A ; Beau, T ; De Bellefon, A ; Bellini, G ; Benziger, J B ; Bonetti, S ; Buck, C ; Caccianiga, B et al.
Results of background measurements with the prototype of the Borexino detector have been used to obtain upper bound on neutrino magnetic moment \mu_{\nu} and lifetime of radiative neutrino decay \nu_H\to\nu_L +\gamma. The new upper limit for \mu_{\nu} of pp and ^{7}Be neutrino is 5.5\cdot 10^{-10}\mu_B and lifetime \tau_{c.m.}(\nu_H\to\nu_L +\gamma)/m_\nu\ge 1.5\cdot 10^3 s\cdot eV^{-1}. [...]
E1-2002-29; JINR-E1-2002-29.- Dubna : Joint Inst. Nucl. Res., 2003 - 15 p. - Published in : Phys. Lett. B 563 (2003) 35-47 External link: Fulltext from JINR Dubna

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