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class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2405.10766">arXiv:2405.10766</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2405.10766">pdf</a>, <a href="https://arxiv.org/format/2405.10766">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Searching for Beyond the Standard Model physics using the improved description of $^{100}$Mo $2谓尾尾$ decay spectral shape with CUPID-Mo </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Celi%2C+E">E. Celi</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chiesa%2C+D">D. Chiesa</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Fujikawa%2C+B+K">B. K. Fujikawa</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Gironi%2C+L">L. Gironi</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a> , et al. (58 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2405.10766v2-abstract-short" style="display: inline;"> The current experiments searching for neutrinoless double-$尾$ ($0谓尾尾$) decay also collect large statistics of Standard Model allowed two-neutrino double-$尾$ ($2谓尾尾$) decay events. These can be used to search for Beyond Standard Model (BSM) physics via $2谓尾尾$ decay spectral distortions. $^{100}$Mo has a natural advantage due to its relatively short half-life, allowing higher $2谓尾尾$ decay statistics&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2405.10766v2-abstract-full').style.display = 'inline'; document.getElementById('2405.10766v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2405.10766v2-abstract-full" style="display: none;"> The current experiments searching for neutrinoless double-$尾$ ($0谓尾尾$) decay also collect large statistics of Standard Model allowed two-neutrino double-$尾$ ($2谓尾尾$) decay events. These can be used to search for Beyond Standard Model (BSM) physics via $2谓尾尾$ decay spectral distortions. $^{100}$Mo has a natural advantage due to its relatively short half-life, allowing higher $2谓尾尾$ decay statistics at equal exposures compared to the other isotopes. We demonstrate the potential of the dual read-out bolometric technique exploiting a $^{100}$Mo exposure of 1.47 kg $\times$ y, acquired in the CUPID-Mo experiment at the Modane underground laboratory (France). We set limits on $0谓尾尾$ decays with the emission of one or more Majorons, on $2谓尾尾$ decay with Lorentz violation, and $2谓尾尾$ decay with a sterile neutrino emission. In this analysis, we investigate the systematic uncertainty induced by modeling the $2谓尾尾$ decay spectral shape parameterized through an improved model, an effect never considered before. This work motivates searches for BSM processes in the upcoming CUPID experiment, which will collect the largest amount of $2谓尾尾$ decay events among the next-generation experiments. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2405.10766v2-abstract-full').style.display = 'none'; document.getElementById('2405.10766v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 27 August, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 May, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2402.12262">arXiv:2402.12262</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2402.12262">pdf</a>, <a href="https://arxiv.org/format/2402.12262">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> BINGO innovative assembly for background reduction in bolometric $0谓尾尾$ experiments </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Bandac%2C+I+C">I. C. Bandac</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Berest%2C+V">V. Berest</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Calvo-Mozota%2C+J+M">J. M. Calvo-Mozota</a>, <a href="/search/?searchtype=author&amp;query=Carniti%2C+P">P. Carniti</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gomez%2C+H">H. Gomez</a>, <a href="/search/?searchtype=author&amp;query=Gotti%2C+C">C. Gotti</a>, <a href="/search/?searchtype=author&amp;query=Gras%2C+P">Ph. Gras</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Khalife%2C+H">H. Khalife</a>, <a href="/search/?searchtype=author&amp;query=Kobychev%2C+V+V">V. V. Kobychev</a> , et al. (23 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2402.12262v2-abstract-short" style="display: inline;"> 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 technologies (a detector assembly, cryogenic photodetectors and active veto) to achieve a very low background index, of the order of $10^{-5}$ counts/(keV kg yr) in th&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2402.12262v2-abstract-full').style.display = 'inline'; document.getElementById('2402.12262v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2402.12262v2-abstract-full" style="display: none;"> 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 technologies (a detector assembly, cryogenic photodetectors and active veto) to achieve a very low background index, of the order of $10^{-5}$ counts/(keV kg yr) in the region of interest. The BINGO demonstrator, called MINI-BINGO, is designed to investigate the promising double-beta-decay isotopes $^{100}$Mo and $^{130}$Te and it will be composed of Li$_2$MoO$_4$ and TeO$_2$ crystals coupled to bolometric light detectors and surrounded by a Bi$_4$Ge$_3$O$_{12}$-based veto. This will allow us to reject a significant background in bolometers caused by surface contamination from $伪$-active radionuclides by means of light yield selection and to mitigate other sources of background, such as surface contamination from $尾$-active radionuclides, external $纬$ radioactivity, and pile-up due to random coincidence of background events. This paper describes an R\&amp;D program towards the BINGO goals, particularly focusing on the development of an innovative assembly designed to reduce the passive materials within the line of sight of the detectors, which is expected to be a dominant source of background in next-generation bolometric experiments. We present the performance of two prototype modules -- housing four cubic (4.5-cm side) Li$_2$MoO$_4$ crystals in total -- operated in the Canfranc underground laboratory in Spain within a facility developed for the CROSS double-beta-decay experiment. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2402.12262v2-abstract-full').style.display = 'none'; document.getElementById('2402.12262v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 July, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 19 February, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Submitted to Nucl. Instr. Meth. A; 28 pages, 11 figures, 4 tables</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2311.01554">arXiv:2311.01554</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2311.01554">pdf</a>, <a href="https://arxiv.org/format/2311.01554">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Astrophysics of Galaxies">astro-ph.GA</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1007/s10909-024-03096-z">10.1007/s10909-024-03096-z <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Characterization of the phonon sensor of the CRYOSEL detector with IR photons </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">Hugues Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Guy%2C+E">Elsa Guy</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">Julien Billard</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">Jules Colas</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">Maryvonne De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">Jules Gascon</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">Alexandre Juillard</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">Stefanos Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Oriol%2C+C">Christine Oriol</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2311.01554v1-abstract-short" style="display: inline;"> The sensitivities of light Dark Matter (DM) particle searches with cryogenic detectors are mostly limited by large backgrounds of events that do not produce ionization signal. The CRYOSEL project develops a new technique where this background in a germanium cryogenic detector is rejected by using the signals from a Superconducting Single Electron Device (SSED) sensor designed to detect the phonons&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.01554v1-abstract-full').style.display = 'inline'; document.getElementById('2311.01554v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2311.01554v1-abstract-full" style="display: none;"> The sensitivities of light Dark Matter (DM) particle searches with cryogenic detectors are mostly limited by large backgrounds of events that do not produce ionization signal. The CRYOSEL project develops a new technique where this background in a germanium cryogenic detector is rejected by using the signals from a Superconducting Single Electron Device (SSED) sensor designed to detect the phonons emitted through the Neganov-Trofimov-Luke effect by the e$^-$h$^+$ pairs as they drift in a close-by very high-field region. A tag on signals from this device should suppress the heat-only background. The measurement of the response to IR laser pulses of the first CRYOSEL prototype show the relevance of such sensor technology. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.01554v1-abstract-full').style.display = 'none'; document.getElementById('2311.01554v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 November, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">9 pages, 3 figures, LTD20</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> J Low Temp Phys (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2307.14086">arXiv:2307.14086</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2307.14086">pdf</a>, <a href="https://arxiv.org/format/2307.14086">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurement of the $2谓尾尾$ decay rate and spectral shape of $^{100}$Mo from the CUPID-Mo experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+6+M">6 M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berge%2C+L">L. Berge</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Celi%2C+E">E. Celi</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chiesa%2C+D">D. Chiesa</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Fujikawa%2C+B+K">B. K. Fujikawa</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Gironi%2C+L">L. Gironi</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a> , et al. (59 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2307.14086v1-abstract-short" style="display: inline;"> Neutrinoless double beta decay ($0谓尾尾$) is a yet unobserved nuclear process which would demonstrate Lepton Number violation, a clear evidence of beyond Standard Model physics. The process two neutrino double beta decay ($2谓尾尾)$ is allowed by the Standard Model and has been measured in numerous experiments. In this letter, we report a measurement of $2谓尾尾$ decay half-life of $^{100}$Mo to the groun&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2307.14086v1-abstract-full').style.display = 'inline'; document.getElementById('2307.14086v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2307.14086v1-abstract-full" style="display: none;"> Neutrinoless double beta decay ($0谓尾尾$) is a yet unobserved nuclear process which would demonstrate Lepton Number violation, a clear evidence of beyond Standard Model physics. The process two neutrino double beta decay ($2谓尾尾)$ is allowed by the Standard Model and has been measured in numerous experiments. In this letter, we report a measurement of $2谓尾尾$ decay half-life of $^{100}$Mo to the ground state of $^{100}$Ru of $(7.07~\pm~0.02~\text{(stat.)}~\pm~0.11~\text{(syst.)})~\times~10^{18}$~yr by the CUPID-Mo experiment. With a relative precision of $\pm~1.6$ \% this is the most precise measurement to date of a $2谓尾尾$ decay rate in $^{100}$Mo. In addition, we constrain higher-order corrections to the spectral shape which provides complementary nuclear structure information. We report a novel measurement of the shape factor $尉_{3,1}=0.45~\pm 0.03~\text{(stat.)} \ \pm 0.05 \ \text{(syst.)}$, which is compared to theoretical predictions for different nuclear models. We also extract the first value for the effective axial vector coupling constant obtained from a spectral shape study of $2谓尾尾$ decay. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2307.14086v1-abstract-full').style.display = 'none'; document.getElementById('2307.14086v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 26 July, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">8 pages, 5 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2306.00166">arXiv:2306.00166</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2306.00166">pdf</a>, <a href="https://arxiv.org/format/2306.00166">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> </div> </div> <p class="title is-5 mathjax"> First demonstration of 30 eVee ionization energy resolution with Ricochet germanium cryogenic bolometers </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Baulieu%2C+G">G. Baulieu</a>, <a href="/search/?searchtype=author&amp;query=Belov%2C+V">V. Belov</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J+-">J. -L. Bret</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Calvo%2C+M">M. Calvo</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=Chala%2C+M">M. Chala</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chaplinsky%2C+L">L. Chaplinsky</a>, <a href="/search/?searchtype=author&amp;query=Chemin%2C+G">G. Chemin</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+R">R. Chen</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=Cudmore%2C+E">E. Cudmore</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Exshaw%2C+O">O. Exshaw</a>, <a href="/search/?searchtype=author&amp;query=Ferriol%2C+S">S. Ferriol</a>, <a href="/search/?searchtype=author&amp;query=Figueroa-Feliciano%2C+E">E. Figueroa-Feliciano</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+-">J. -B. Filippini</a> , et al. (55 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2306.00166v1-abstract-short" style="display: inline;"> The future Ricochet experiment aims to search for new physics in the electroweak sector by measuring the Coherent Elastic Neutrino-Nucleus Scattering process from reactor antineutrinos with high precision down to the sub-100 eV nuclear recoil energy range. While the Ricochet collaboration is currently building the experimental setup at the reactor site, it is also finalizing the cryogenic detector&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.00166v1-abstract-full').style.display = 'inline'; document.getElementById('2306.00166v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2306.00166v1-abstract-full" style="display: none;"> The future Ricochet experiment aims to search for new physics in the electroweak sector by measuring the Coherent Elastic Neutrino-Nucleus Scattering process from reactor antineutrinos with high precision down to the sub-100 eV nuclear recoil energy range. While the Ricochet collaboration is currently building the experimental setup at the reactor site, it is also finalizing the cryogenic detector arrays that will be integrated into the cryostat at the Institut Laue Langevin in early 2024. In this paper, we report on recent progress from the Ge cryogenic detector technology, called the CryoCube. More specifically, we present the first demonstration of a 30~eVee (electron equivalent) baseline ionization resolution (RMS) achieved with an early design of the detector assembly and its dedicated High Electron Mobility Transistor (HEMT) based front-end electronics. This represents an order of magnitude improvement over the best ionization resolutions obtained on similar heat-and-ionization germanium cryogenic detectors from the EDELWEISS and SuperCDMS dark matter experiments, and a factor of three improvement compared to the first fully-cryogenic HEMT-based preamplifier coupled to a CDMS-II germanium detector. Additionally, we discuss the implications of these results in the context of the future Ricochet experiment and its expected background mitigation performance. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.00166v1-abstract-full').style.display = 'none'; document.getElementById('2306.00166v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 31 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">10 pages, 5 figures, 1 table</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2305.01402">arXiv:2305.01402</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2305.01402">pdf</a>, <a href="https://arxiv.org/format/2305.01402">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-023-11830-2">10.1140/epjc/s10052-023-11830-2 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The background model of the CUPID-Mo $0谓尾尾$ experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Collaboration%2C+C">CUPID-Mo Collaboration</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Celi%2C+E">E. Celi</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chiesa%2C+D">D. Chiesa</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Fujikawa%2C+B+K">B. K. Fujikawa</a> , et al. (58 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2305.01402v1-abstract-short" style="display: inline;"> CUPID-Mo, located in the Laboratoire Souterrain de Modane (France), was a demonstrator for the next generation $0谓尾尾$ decay experiment, CUPID. It consisted of an array of 20 enriched Li$_{2}$$ ^{100}$MoO$_4$ bolometers and 20 Ge light detectors and has demonstrated that the technology of scintillating bolometers with particle identification capabilities is mature. Furthermore, CUPID-Mo can inform&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.01402v1-abstract-full').style.display = 'inline'; document.getElementById('2305.01402v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2305.01402v1-abstract-full" style="display: none;"> CUPID-Mo, located in the Laboratoire Souterrain de Modane (France), was a demonstrator for the next generation $0谓尾尾$ decay experiment, CUPID. It consisted of an array of 20 enriched Li$_{2}$$ ^{100}$MoO$_4$ bolometers and 20 Ge light detectors and has demonstrated that the technology of scintillating bolometers with particle identification capabilities is mature. Furthermore, CUPID-Mo can inform and validate the background prediction for CUPID. In this paper, we present a detailed model of the CUPID-Mo backgrounds. This model is able to describe well the features of the experimental data and enables studies of the $2谓尾尾$ decay and other processes with high precision. We also measure the radio-purity of the Li$_{2}$$^{100}$MoO$_4$ crystals which are found to be sufficient for the CUPID goals. Finally, we also obtain a background index in the region of interest of 3.7$^{+0.9}_{-0.8}$(stat)$^{+1.5}_{-0.7}$(syst)$\times10^{-3}$counts/$螖$E$_{FWHM}$/mol$_{iso}$/yr, the lowest in a bolometric $0谓尾尾$ decay experiment. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.01402v1-abstract-full').style.display = 'none'; document.getElementById('2305.01402v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2023. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2304.14926">arXiv:2304.14926</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2304.14926">pdf</a>, <a href="https://arxiv.org/format/2304.14926">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1016/j.nima.2023.168765">10.1016/j.nima.2023.168765 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Results from a Prototype TES Detector for the Ricochet Experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ricochet+Collaboration"> Ricochet Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Baulieu%2C+G">G. Baulieu</a>, <a href="/search/?searchtype=author&amp;query=Belov%2C+V">V. Belov</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J+L">J-. L. Bret</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Calvo%2C+M">M. Calvo</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=Chala%2C+M">M. Chala</a>, <a href="/search/?searchtype=author&amp;query=Chang%2C+C+L">C. L. Chang</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chaplinsky%2C+L">L. Chaplinsky</a>, <a href="/search/?searchtype=author&amp;query=Chemin%2C+G">G. Chemin</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+R">R. Chen</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=Cudmore%2C+E">E. Cudmore</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Exshaw%2C+O">O. Exshaw</a>, <a href="/search/?searchtype=author&amp;query=Ferriol%2C+S">S. Ferriol</a> , et al. (66 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2304.14926v2-abstract-short" style="display: inline;"> Coherent elastic neutrino-nucleus scattering (CE$谓$NS) offers valuable sensitivity to physics beyond the Standard Model. The Ricochet experiment will use cryogenic solid-state detectors to perform a precision measurement of the CE$谓$NS spectrum induced by the high neutrino flux from the Institut Laue-Langevin nuclear reactor. The experiment will employ an array of detectors, each with a mass of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2304.14926v2-abstract-full').style.display = 'inline'; document.getElementById('2304.14926v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2304.14926v2-abstract-full" style="display: none;"> Coherent elastic neutrino-nucleus scattering (CE$谓$NS) offers valuable sensitivity to physics beyond the Standard Model. The Ricochet experiment will use cryogenic solid-state detectors to perform a precision measurement of the CE$谓$NS spectrum induced by the high neutrino flux from the Institut Laue-Langevin nuclear reactor. The experiment will employ an array of detectors, each with a mass of $\sim$30 g and a targeted energy threshold of 50 eV. Nine of these detectors (the &#34;Q-Array&#34;) will be based on a novel Transition-Edge Sensor (TES) readout style, in which the TES devices are thermally coupled to the absorber using a gold wire bond. We present initial characterization of a Q-Array-style detector using a 1 gram silicon absorber, obtaining a baseline root-mean-square resolution of less than 40 eV. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2304.14926v2-abstract-full').style.display = 'none'; document.getElementById('2304.14926v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 January, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 April, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">18 pages, 8 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nuclear Inst. and Methods in Physics Research, A 1057 (2023) 168765 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2304.04674">arXiv:2304.04674</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2304.04674">pdf</a>, <a href="https://arxiv.org/format/2304.04674">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/18/06/P06033">10.1088/1748-0221/18/06/P06033 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> A first test of CUPID prototypal light detectors with NTD-Ge sensors in a pulse-tube cryostat </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=CUPID+collaboration"> CUPID collaboration</a>, <a href="/search/?searchtype=author&amp;query=Alfonso%2C+K">K. Alfonso</a>, <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Balata%2C+M">M. Balata</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Berest%2C+V">V. Berest</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Bettelli%2C+M">M. Bettelli</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a>, <a href="/search/?searchtype=author&amp;query=Camilleri%2C+J">J. Camilleri</a>, <a href="/search/?searchtype=author&amp;query=Campani%2C+A">A. Campani</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+C">C. Capelli</a> , et al. (154 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2304.04674v1-abstract-short" style="display: inline;"> CUPID is a next-generation bolometric experiment aiming at searching for neutrinoless double-beta decay with ~250 kg of isotopic mass of $^{100}$Mo. It will operate at $\sim$10 mK in a cryostat currently hosting a similar-scale bolometric array for the CUORE experiment at the Gran Sasso National Laboratory (Italy). CUPID will be based on large-volume scintillating bolometers consisting of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2304.04674v1-abstract-full').style.display = 'inline'; document.getElementById('2304.04674v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2304.04674v1-abstract-full" style="display: none;"> CUPID is a next-generation bolometric experiment aiming at searching for neutrinoless double-beta decay with ~250 kg of isotopic mass of $^{100}$Mo. It will operate at $\sim$10 mK in a cryostat currently hosting a similar-scale bolometric array for the CUORE experiment at the Gran Sasso National Laboratory (Italy). CUPID will be based on large-volume scintillating bolometers consisting of $^{100}$Mo-enriched Li$_2$MoO$_4$ crystals, facing thin Ge-wafer-based bolometric light detectors. In the CUPID design, the detector structure is novel and needs to be validated. In particular, the CUORE cryostat presents a high level of mechanical vibrations due to the use of pulse tubes and the effect of vibrations on the detector performance must be investigated. In this paper we report the first test of the CUPID-design bolometric light detectors with NTD-Ge sensors in a dilution refrigerator equipped with a pulse tube in an above-ground lab. Light detectors are characterized in terms of sensitivity, energy resolution, pulse time constants, and noise power spectrum. Despite the challenging noisy environment due to pulse-tube-induced vibrations, we demonstrate that all the four tested light detectors comply with the CUPID goal in terms of intrinsic energy resolution of 100 eV RMS baseline noise. Indeed, we have measured 70--90 eV RMS for the four devices, which show an excellent reproducibility. We have also obtained outstanding energy resolutions at the 356 keV line from a $^{133}$Ba source with one light detector achieving 0.71(5) keV FWHM, which is -- to our knowledge -- the best ever obtained when compared to $纬$ detectors of any technology in this energy range. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2304.04674v1-abstract-full').style.display = 'none'; document.getElementById('2304.04674v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 April, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Prepared for submission to JINST; 16 pages, 7 figures, and 1 table</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2304.04611">arXiv:2304.04611</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2304.04611">pdf</a>, <a href="https://arxiv.org/format/2304.04611">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/18/06/P06018">10.1088/1748-0221/18/06/P06018 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Twelve-crystal prototype of Li$_2$MoO$_4$ scintillating bolometers for CUPID and CROSS experiments </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=CUPID"> CUPID</a>, <a href="/search/?searchtype=author&amp;query=collaborations%2C+C">CROSS collaborations</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Alfonso%2C+K">K. Alfonso</a>, <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Balata%2C+M">M. Balata</a>, <a href="/search/?searchtype=author&amp;query=Bandac%2C+I+C">I. C. Bandac</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Berest%2C+V">V. Berest</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Bettelli%2C+M">M. Bettelli</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a> , et al. (160 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2304.04611v1-abstract-short" style="display: inline;"> An array of twelve 0.28 kg lithium molybdate (LMO) low-temperature bolometers equipped with 16 bolometric Ge light detectors, aiming at optimization of detector structure for CROSS and CUPID double-beta decay experiments, was constructed and tested in a low-background pulse-tube-based cryostat at the Canfranc underground laboratory in Spain. Performance of the scintillating bolometers was studied&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2304.04611v1-abstract-full').style.display = 'inline'; document.getElementById('2304.04611v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2304.04611v1-abstract-full" style="display: none;"> An array of twelve 0.28 kg lithium molybdate (LMO) low-temperature bolometers equipped with 16 bolometric Ge light detectors, aiming at optimization of detector structure for CROSS and CUPID double-beta decay experiments, was constructed and tested in a low-background pulse-tube-based cryostat at the Canfranc underground laboratory in Spain. Performance of the scintillating bolometers was studied depending on the size of phonon NTD-Ge sensors glued to both LMO and Ge absorbers, shape of the Ge light detectors (circular vs. square, from two suppliers), in different light collection conditions (with and without reflector, with aluminum coated LMO crystal surface). The scintillating bolometer array was operated over 8 months in the low-background conditions that allowed to probe a very low, $渭$Bq/kg, level of the LMO crystals radioactive contamination by $^{228}$Th and $^{226}$Ra. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2304.04611v1-abstract-full').style.display = 'none'; document.getElementById('2304.04611v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 April, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Prepared for submission to JINST; 23 pages, 9 figures, and 4 tables</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2303.02067">arXiv:2303.02067</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.02067">pdf</a>, <a href="https://arxiv.org/format/2303.02067">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.108.022006">10.1103/PhysRevD.108.022006 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Tagging and localisation of ionizing events using NbSi transition edge phonon sensors for Dark Matter searches </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=EDELWEISS+Collaboration"> EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+B">J. B. Filippini</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Guy%2C+E">E. Guy</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Martini%2C+N">N. Martini</a> , et al. (14 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2303.02067v1-abstract-short" style="display: inline;"> In the context of direct searches of sub-GeV Dark Matter particles with germanium detectors, the EDELWEISS collaboration has tested a new technique to tag ionizing events using NbSi transition edge athermal phonon sensors. The emission of the athermal phonons generated by the Neganov-Trofimov-Luke effect associated with the drift of electrons and holes through the detectors is used to tag ionizati&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.02067v1-abstract-full').style.display = 'inline'; document.getElementById('2303.02067v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.02067v1-abstract-full" style="display: none;"> In the context of direct searches of sub-GeV Dark Matter particles with germanium detectors, the EDELWEISS collaboration has tested a new technique to tag ionizing events using NbSi transition edge athermal phonon sensors. The emission of the athermal phonons generated by the Neganov-Trofimov-Luke effect associated with the drift of electrons and holes through the detectors is used to tag ionization events generated in specific parts of the detector localized in front of the NbSi sensor and to reject by more than a factor 5 (at 90% C.L.) the background from heat-only events that dominates the spectrum above 3 keV. This method is able to improve by a factor 2.8 the previous limit on spin-independent interactions of 1 GeV/c2 WIMPs obtained with the same detector and data set but without this tagging technique. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.02067v1-abstract-full').style.display = 'none'; document.getElementById('2303.02067v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">13 pages, 11 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2208.01760">arXiv:2208.01760</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2208.01760">pdf</a>, <a href="https://arxiv.org/format/2208.01760">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-022-11150-x">10.1140/epjc/s10052-022-11150-x <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Fast neutron background characterization of the future Ricochet experiment at the ILL research nuclear reactor </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Baulieu%2C+G">G. Baulieu</a>, <a href="/search/?searchtype=author&amp;query=Belov%2C+V">V. Belov</a>, <a href="/search/?searchtype=author&amp;query=Berge%2C+L">L. Berge</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J+-">J. -L. Bret</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Calvo%2C+M">M. Calvo</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chaplinsky%2C+L">L. Chaplinsky</a>, <a href="/search/?searchtype=author&amp;query=Chemin%2C+G">G. Chemin</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+R">R. Chen</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Exshaw%2C+O">O. Exshaw</a>, <a href="/search/?searchtype=author&amp;query=Ferriol%2C+S">S. Ferriol</a>, <a href="/search/?searchtype=author&amp;query=Figueroa-Feliciano%2C+E">E. Figueroa-Feliciano</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+-">J. -B. Filippini</a>, <a href="/search/?searchtype=author&amp;query=Formaggio%2C+J+A">J. A. Formaggio</a>, <a href="/search/?searchtype=author&amp;query=Fuard%2C+S">S. Fuard</a> , et al. (58 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2208.01760v1-abstract-short" style="display: inline;"> The future Ricochet experiment aims at searching for new physics in the electroweak sector by providing a high precision measurement of the Coherent Elastic Neutrino-Nucleus Scattering (CENNS) process down to the sub-100 eV nuclear recoil energy range. The experiment will deploy a kg-scale low-energy-threshold detector array combining Ge and Zn target crystals 8.8 meters away from the 58 MW resear&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2208.01760v1-abstract-full').style.display = 'inline'; document.getElementById('2208.01760v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2208.01760v1-abstract-full" style="display: none;"> The future Ricochet experiment aims at searching for new physics in the electroweak sector by providing a high precision measurement of the Coherent Elastic Neutrino-Nucleus Scattering (CENNS) process down to the sub-100 eV nuclear recoil energy range. The experiment will deploy a kg-scale low-energy-threshold detector array combining Ge and Zn target crystals 8.8 meters away from the 58 MW research nuclear reactor core of the Institut Laue Langevin (ILL) in Grenoble, France. Currently, the Ricochet collaboration is characterizing the backgrounds at its future experimental site in order to optimize the experiment&#39;s shielding design. The most threatening background component, which cannot be actively rejected by particle identification, consists of keV-scale neutron-induced nuclear recoils. These initial fast neutrons are generated by the reactor core and surrounding experiments (reactogenics), and by the cosmic rays producing primary neutrons and muon-induced neutrons in the surrounding materials. In this paper, we present the Ricochet neutron background characterization using $^3$He proportional counters which exhibit a high sensitivity to thermal, epithermal and fast neutrons. We compare these measurements to the Ricochet Geant4 simulations to validate our reactogenic and cosmogenic neutron background estimations. Eventually, we present our estimated neutron background for the future Ricochet experiment and the resulting CENNS detection significance. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2208.01760v1-abstract-full').style.display = 'none'; document.getElementById('2208.01760v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 August, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">14 pages, 14 figures, 1 table</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2207.09577">arXiv:2207.09577</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2207.09577">pdf</a>, <a href="https://arxiv.org/format/2207.09577">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> New measurement of double beta decays of $^{100}$Mo to excited states of $^{100}$Ru with the CUPID-Mo experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Collaboration%2C+C">CUPID-Mo Collaboration</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chiesa%2C+D">D. Chiesa</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Fujikawa%2C+B+K">B. K. Fujikawa</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Gironi%2C+L">L. Gironi</a> , et al. (58 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2207.09577v1-abstract-short" style="display: inline;"> The CUPID-Mo experiment, located at Laboratoire Souterrain de Modane (France), was a demonstrator experiment for CUPID. It consisted of an array of 20 Li$_2^{100}$MoO$_4$ (LMO) calorimeters each equipped with a Ge light detector (LD) for particle identification. In this work, we present the result of a search for two-neutrino and neutrinoless double beta decays of $^{100}$Mo to the first 0$^+$ and&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.09577v1-abstract-full').style.display = 'inline'; document.getElementById('2207.09577v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2207.09577v1-abstract-full" style="display: none;"> The CUPID-Mo experiment, located at Laboratoire Souterrain de Modane (France), was a demonstrator experiment for CUPID. It consisted of an array of 20 Li$_2^{100}$MoO$_4$ (LMO) calorimeters each equipped with a Ge light detector (LD) for particle identification. In this work, we present the result of a search for two-neutrino and neutrinoless double beta decays of $^{100}$Mo to the first 0$^+$ and $2^+$ excited states of $^{100}$Ru using the full CUPID-Mo exposure (2.71 kg$\times$yr of LMO). We measure the half-life of $2谓尾尾$ decay to the $0^{+}_1$ state as $T_{1/2}^{2谓\rightarrow 0_1^+}=7.5\pm 0.8 \ \text{(stat.)} \ ^{+ 0.4}_{-0.3} \ \text{(syst.)} )\times 10^{20} \ \mathrm{yr}$. The bolometric technique enables measurement of the electron energies as well as the gamma rays from nuclear de-excitation and this allows us to set new limits on the two-neutrino decay to the $2_1^+$ state of $T^{2谓\rightarrow 2_1^+}_{1/2}&gt;4.4\times 10^{21} \ \mathrm{yr} \ \text{(90 % c.i.)}$ and on the neutrinoless modes of $T_{1/2}^{0谓\rightarrow 2_1^+}&gt;2.1\times10^{23} \ \mathrm{yr}\ \text{(90 % c.i.)}$, $T_{1/2}^{0谓\rightarrow 0_1^+}&gt;1.2\times10^{23} \ \mathrm{yr}\ \text{(90 % c.i.)}$. Information on the electrons spectral shape is obtained which allows us to make the first comparison of the single state (SSD) and higher state (HSD) $2谓尾尾$ decay models for the $0_1^+$ excited state of $^{100}$Ru. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.09577v1-abstract-full').style.display = 'none'; document.getElementById('2207.09577v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">22 pages, 15 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2204.14161">arXiv:2204.14161</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2204.14161">pdf</a>, <a href="https://arxiv.org/format/2204.14161">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> First cryogenic tests on BINGO innovations </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Carniti%2C+P">P. Carniti</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charrier%2C+A">A. Charrier</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F">F. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Combarieu%2C+M">M. De Combarieu</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gomez%2C+H">H. Gomez</a>, <a href="/search/?searchtype=author&amp;query=Gotti%2C+C">C. Gotti</a>, <a href="/search/?searchtype=author&amp;query=Gras%2C+P">Ph. Gras</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Khalife%2C+H">H. Khalife</a>, <a href="/search/?searchtype=author&amp;query=Kobychev%2C+V+V">V. V. Kobychev</a>, <a href="/search/?searchtype=author&amp;query=Lefevre%2C+M">M. Lefevre</a>, <a href="/search/?searchtype=author&amp;query=Loaiza%2C+P">P. Loaiza</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a> , et al. (11 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2204.14161v1-abstract-short" style="display: inline;"> Neutrinoless double-beta decay ($0\nu2尾$) is a hypothetical rare nuclear transition. Its observation would provide an important insight about the nature of neutrinos (Dirac or Majorana particle) demonstrating that the lepton number is not conserved. BINGO (Bi-Isotope $0\nu2尾$ Next Generation Observatory) aims to set the technological grounds for future bolometric $0\nu2尾$ experiments. It is based&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.14161v1-abstract-full').style.display = 'inline'; document.getElementById('2204.14161v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2204.14161v1-abstract-full" style="display: none;"> Neutrinoless double-beta decay ($0\nu2尾$) is a hypothetical rare nuclear transition. Its observation would provide an important insight about the nature of neutrinos (Dirac or Majorana particle) demonstrating that the lepton number is not conserved. BINGO (Bi-Isotope $0\nu2尾$ Next Generation Observatory) aims to set the technological grounds for future bolometric $0\nu2尾$ experiments. It is based on a dual heat-light readout, i.e. a main scintillating absorber embedding the double-beta decay isotope accompanied by a cryogenic light detector. BINGO will study two of the most promising isotopes: $^{100}$Mo embedded in Li$_2$MoO$_4$ (LMO) crystals and $^{130}$Te embedded in TeO$_2$. BINGO technology will reduce dramatically the background in the region of interest, thus boosting the discovery sensitivity of $0\nu2尾$. The proposed solutions will have a high impact on next-generation bolometric tonne-scale experiments, like CUPID. In this contribution, we present the results obtained during the first tests performed in the framework of BINGO R&amp;D. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.14161v1-abstract-full').style.display = 'none'; document.getElementById('2204.14161v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 29 April, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">4 pages, 2 figures. Contribution to the proceedings of 32nd Rencontres de Blois, Blois, France, 17-22 October 2021</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.08386">arXiv:2203.08386</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.08386">pdf</a>, <a href="https://arxiv.org/format/2203.08386">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Toward CUPID-1T </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Balata%2C+M">M. Balata</a>, <a href="/search/?searchtype=author&amp;query=Ballen%2C+K">K. Ballen</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Bettelli%2C+M">M. Bettelli</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a>, <a href="/search/?searchtype=author&amp;query=Camilleri%2C+J">J. Camilleri</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+C">C. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+S">S. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Cappelli%2C+L">L. Cappelli</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a> , et al. (150 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2203.08386v2-abstract-short" style="display: inline;"> Current experiments to search for broken lepton-number symmetry through the observation of neutrinoless double-beta decay ($0\mathrm{谓尾尾}$) provide the most stringent limits on the Majorana nature of neutrinos and the effective Majorana neutrino mass ($m_{尾尾}$). The next-generation experiments will focus on the sensitivity to the $0\mathrm{谓尾尾}$ half-life of $\mathcal{O}(10^{27}$--$10^{28}$~years&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.08386v2-abstract-full').style.display = 'inline'; document.getElementById('2203.08386v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.08386v2-abstract-full" style="display: none;"> Current experiments to search for broken lepton-number symmetry through the observation of neutrinoless double-beta decay ($0\mathrm{谓尾尾}$) provide the most stringent limits on the Majorana nature of neutrinos and the effective Majorana neutrino mass ($m_{尾尾}$). The next-generation experiments will focus on the sensitivity to the $0\mathrm{谓尾尾}$ half-life of $\mathcal{O}(10^{27}$--$10^{28}$~years$)$ and $m_{尾尾}\lesssim15$~meV, which would provide complete coverage of the so-called Inverted Ordering region of the neutrino mass parameter space. By taking advantage of recent technological breakthroughs, new, future calorimetric experiments at the 1-ton scale can increase the sensitivity by at least another order of magnitude, exploring the large fraction of the parameter space that corresponds to the Normal neutrino mass ordering. In case of a discovery, such experiments could provide important insights toward a new understanding of the mechanism of $0\mathrm{谓尾尾}$. We present here a series of projects underway that will provide advancements in background reduction, cryogenic readout, and physics searches beyond $0\mathrm{谓尾尾}$, all moving toward the next-to-next generation CUPID-1T detector. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.08386v2-abstract-full').style.display = 'none'; document.getElementById('2203.08386v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 April, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">contribution to Snowmass 2021</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.07361">arXiv:2203.07361</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.07361">pdf</a>, <a href="https://arxiv.org/format/2203.07361">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Astrophysical Phenomena">astro-ph.HE</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Coherent elastic neutrino-nucleus scattering: Terrestrial and astrophysical applications </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdullah%2C+M">M. Abdullah</a>, <a href="/search/?searchtype=author&amp;query=Abele%2C+H">H. Abele</a>, <a href="/search/?searchtype=author&amp;query=Akimov%2C+D">D. Akimov</a>, <a href="/search/?searchtype=author&amp;query=Angloher%2C+G">G. Angloher</a>, <a href="/search/?searchtype=author&amp;query=Aristizabal-Sierra%2C+D">D. Aristizabal-Sierra</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Balantekin%2C+A+B">A. B. Balantekin</a>, <a href="/search/?searchtype=author&amp;query=Balogh%2C+L">L. Balogh</a>, <a href="/search/?searchtype=author&amp;query=Barbeau%2C+P+S">P. S. Barbeau</a>, <a href="/search/?searchtype=author&amp;query=Baudis%2C+L">L. Baudis</a>, <a href="/search/?searchtype=author&amp;query=Baxter%2C+A+L">A. L. Baxter</a>, <a href="/search/?searchtype=author&amp;query=Beaufort%2C+C">C. Beaufort</a>, <a href="/search/?searchtype=author&amp;query=Beaulieu%2C+G">G. Beaulieu</a>, <a href="/search/?searchtype=author&amp;query=Belov%2C+V">V. Belov</a>, <a href="/search/?searchtype=author&amp;query=Bento%2C+A">A. Bento</a>, <a href="/search/?searchtype=author&amp;query=Berge%2C+L">L. Berge</a>, <a href="/search/?searchtype=author&amp;query=Bernardi%2C+I+A">I. A. Bernardi</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bolozdynya%2C+A">A. Bolozdynya</a>, <a href="/search/?searchtype=author&amp;query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J+L">J-. L. Bret</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Brossard%2C+A">A. Brossard</a>, <a href="/search/?searchtype=author&amp;query=Buck%2C+C">C. Buck</a> , et al. (250 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2203.07361v1-abstract-short" style="display: inline;"> Coherent elastic neutrino-nucleus scattering (CE$谓$NS) is a process in which neutrinos scatter on a nucleus which acts as a single particle. Though the total cross section is large by neutrino standards, CE$谓$NS has long proven difficult to detect, since the deposited energy into the nucleus is $\sim$ keV. In 2017, the COHERENT collaboration announced the detection of CE$谓$NS using a stopped-pion&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.07361v1-abstract-full').style.display = 'inline'; document.getElementById('2203.07361v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.07361v1-abstract-full" style="display: none;"> Coherent elastic neutrino-nucleus scattering (CE$谓$NS) is a process in which neutrinos scatter on a nucleus which acts as a single particle. Though the total cross section is large by neutrino standards, CE$谓$NS has long proven difficult to detect, since the deposited energy into the nucleus is $\sim$ keV. In 2017, the COHERENT collaboration announced the detection of CE$谓$NS using a stopped-pion source with CsI detectors, followed up the detection of CE$谓$NS using an Ar target. The detection of CE$谓$NS has spawned a flurry of activities in high-energy physics, inspiring new constraints on beyond the Standard Model (BSM) physics, and new experimental methods. The CE$谓$NS process has important implications for not only high-energy physics, but also astrophysics, nuclear physics, and beyond. This whitepaper discusses the scientific importance of CE$谓$NS, highlighting how present experiments such as COHERENT are informing theory, and also how future experiments will provide a wealth of information across the aforementioned fields of physics. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.07361v1-abstract-full').style.display = 'none'; document.getElementById('2203.07361v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">contribution to Snowmasss 2021. Contact authors: P. S. Barbeau, R. Strauss, L. E. Strigari</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.03993">arXiv:2203.03993</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.03993">pdf</a>, <a href="https://arxiv.org/format/2203.03993">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Astrophysics of Galaxies">astro-ph.GA</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.106.062004">10.1103/PhysRevD.106.062004 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for sub-GeV Dark Matter via Migdal effect with an EDELWEISS germanium detector with NbSi TES sensors </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Caze%2C+A">A. Caze</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+B">J. B. Filippini</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Guy%2C+E">E. Guy</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a> , et al. (15 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2203.03993v4-abstract-short" style="display: inline;"> The EDELWEISS collaboration reports on the search for Dark Matter (DM) particle interactions via Migdal effect with masses between $32$ MeV$\cdot$c$^{-2}$ to $2$ GeV$\cdot$c$^{-2}$ using a $200$ g cryogenic Ge detector sensitive to simultaneously heat and ionization signals and operated underground at the Laboratoire Souterrain de Modane in France. The phonon signal was read out using a Transition&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.03993v4-abstract-full').style.display = 'inline'; document.getElementById('2203.03993v4-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.03993v4-abstract-full" style="display: none;"> The EDELWEISS collaboration reports on the search for Dark Matter (DM) particle interactions via Migdal effect with masses between $32$ MeV$\cdot$c$^{-2}$ to $2$ GeV$\cdot$c$^{-2}$ using a $200$ g cryogenic Ge detector sensitive to simultaneously heat and ionization signals and operated underground at the Laboratoire Souterrain de Modane in France. The phonon signal was read out using a Transition Edge Sensor made of a NbSi thin film. The detector was biased at $66$ V in order to benefit from the Neganov-Trofimov-Luke amplification and resulting in a resolution on the energy of electron recoils of $4.46$ eV$_{ee}$ (RMS) and an analysis threshold of $30$ eV$_{ee}$. The sensitivity is limited by a dominant background not associated to charge creation in the detector. The search constrains a new region of parameter space for cross-sections down to $10^{-29}$ cm$^2$ and masses between $32$ and $100$ MeV$\cdot$c$^{-2}$. The achieved low threshold with the NbSi sensor shows the relevance of its use for athermal-phonon sensitive devices for low-mass DM searches. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.03993v4-abstract-full').style.display = 'none'; document.getElementById('2203.03993v4-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 October, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 8 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">10 pages, 9 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 106, 062004 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.08716">arXiv:2202.08716</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.08716">pdf</a>, <a href="https://arxiv.org/format/2202.08716">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-022-10942-5">10.1140/epjc/s10052-022-10942-5 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Final results on the $0谓尾尾$ decay half-life limit of $^{100}$Mo from the CUPID-Mo experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chiesa%2C+D">D. Chiesa</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Ferri%2C+F">F. Ferri</a>, <a href="/search/?searchtype=author&amp;query=Fujikawa%2C+B+K">B. K. Fujikawa</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Gironi%2C+L">L. Gironi</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a> , et al. (54 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2202.08716v2-abstract-short" style="display: inline;"> The CUPID-Mo experiment to search for 0$谓尾尾$ decay in $^{100}$Mo has been recently completed after about 1.5 years of operation at Laboratoire Souterrain de Modane (France). It served as a demonstrator for CUPID, a next generation 0$谓尾尾$ decay experiment. CUPID-Mo was comprised of 20 enriched Li$_2$$^{100}$MoO$_4$ scintillating calorimeters, each with a mass of $\sim$ 0.2 kg, operated at $\sim$20&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.08716v2-abstract-full').style.display = 'inline'; document.getElementById('2202.08716v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.08716v2-abstract-full" style="display: none;"> The CUPID-Mo experiment to search for 0$谓尾尾$ decay in $^{100}$Mo has been recently completed after about 1.5 years of operation at Laboratoire Souterrain de Modane (France). It served as a demonstrator for CUPID, a next generation 0$谓尾尾$ decay experiment. CUPID-Mo was comprised of 20 enriched Li$_2$$^{100}$MoO$_4$ scintillating calorimeters, each with a mass of $\sim$ 0.2 kg, operated at $\sim$20 mK. We present here the final analysis with the full exposure of CUPID-Mo ($^{100}$Mo exposure of 1.47 kg$\times$yr) used to search for lepton number violation via 0$谓尾尾$ decay. We report on various analysis improvements since the previous result on a subset of data, reprocessing all data with these new techniques. We observe zero events in the region of interest and set a new limit on the $^{100}$Mo 0$谓尾尾$ decay half-life of $T^{0谓}_{1/2} &gt; 1.8 \times 10^{24}$ year (stat.+syst.) at 90% CI. Under the light Majorana neutrino exchange mechanism this corresponds to an effective Majorana neutrino mass of $\left&lt;m_{尾尾}\right&gt; &lt; (0.28$--$0.49)$ eV, dependent upon the nuclear matrix element utilized. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.08716v2-abstract-full').style.display = 'none'; document.getElementById('2202.08716v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 December, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur. Phys. J. C 82, 1033 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.06279">arXiv:2202.06279</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.06279">pdf</a>, <a href="https://arxiv.org/format/2202.06279">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Optimization of the first CUPID detector module </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=CUPID+collaboration"> CUPID collaboration</a>, <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Balata%2C+M">M. Balata</a>, <a href="/search/?searchtype=author&amp;query=Ballen%2C+K">K. Ballen</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Bettelli%2C+M">M. Bettelli</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a>, <a href="/search/?searchtype=author&amp;query=Camilleri%2C+J">J. Camilleri</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+C">C. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+S">S. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Cappelli%2C+L">L. Cappelli</a> , et al. (153 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2202.06279v1-abstract-short" style="display: inline;"> CUPID will be a next generation experiment searching for the neutrinoless double $尾$ decay, whose discovery would establish the Majorana nature of the neutrino. Based on the experience achieved with the CUORE experiment, presently taking data at LNGS, CUPID aims to reach a background free environment by means of scintillating Li$_{2}$$^{100}$MoO$_4$ crystals coupled to light detectors. Indeed, the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.06279v1-abstract-full').style.display = 'inline'; document.getElementById('2202.06279v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.06279v1-abstract-full" style="display: none;"> CUPID will be a next generation experiment searching for the neutrinoless double $尾$ decay, whose discovery would establish the Majorana nature of the neutrino. Based on the experience achieved with the CUORE experiment, presently taking data at LNGS, CUPID aims to reach a background free environment by means of scintillating Li$_{2}$$^{100}$MoO$_4$ crystals coupled to light detectors. Indeed, the simultaneous heat and light detection allows us to reject the dominant background of $伪$ particles, as proven by the CUPID-0 and CUPID-Mo demonstrators. In this work we present the results of the first test of the CUPID baseline module. In particular, we propose a new optimized detector structure and light sensors design to enhance the engineering and the light collection, respectively. We characterized the heat detectors, achieving an energy resolution of (5.9 $\pm$ 0.2) keV FWHM at the $Q$-value of $^{100}$Mo (about 3034 keV). We studied the light collection of the baseline CUPID design with respect to an alternative configuration which features gravity-assisted light detectors&#39; mounting. In both cases we obtained an improvement in the light collection with respect to past measures and we validated the particle identification capability of the detector, which ensures an $伪$ particle rejection higher than 99.9%, fully satisfying the requirements for CUPID. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.06279v1-abstract-full').style.display = 'none'; document.getElementById('2202.06279v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 13 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">10 pages, 5 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.05097">arXiv:2202.05097</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.05097">pdf</a>, <a href="https://arxiv.org/format/2202.05097">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.21468/SciPostPhysProc.9.001">10.21468/SciPostPhysProc.9.001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> EXCESS workshop: Descriptions of rising low-energy spectra </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Adari%2C+P">P. Adari</a>, <a href="/search/?searchtype=author&amp;query=Aguilar-Arevalo%2C+A">A. Aguilar-Arevalo</a>, <a href="/search/?searchtype=author&amp;query=Amidei%2C+D">D. Amidei</a>, <a href="/search/?searchtype=author&amp;query=Angloher%2C+G">G. Angloher</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Balogh%2C+L">L. Balogh</a>, <a href="/search/?searchtype=author&amp;query=Banik%2C+S">S. Banik</a>, <a href="/search/?searchtype=author&amp;query=Baxter%2C+D">D. Baxter</a>, <a href="/search/?searchtype=author&amp;query=Beaufort%2C+C">C. Beaufort</a>, <a href="/search/?searchtype=author&amp;query=Beaulieu%2C+G">G. Beaulieu</a>, <a href="/search/?searchtype=author&amp;query=Belov%2C+V">V. Belov</a>, <a href="/search/?searchtype=author&amp;query=Gal%2C+Y+B">Y. Ben Gal</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Bento%2C+A">A. Bento</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Bertolini%2C+A">A. Bertolini</a>, <a href="/search/?searchtype=author&amp;query=Bhattacharyya%2C+R">R. Bhattacharyya</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bloch%2C+I+M">I. M. Bloch</a>, <a href="/search/?searchtype=author&amp;query=Botti%2C+A">A. Botti</a>, <a href="/search/?searchtype=author&amp;query=Breier%2C+R">R. Breier</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J+L">J-. L. Bret</a> , et al. (281 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2202.05097v2-abstract-short" style="display: inline;"> Many low-threshold experiments observe sharply rising event rates of yet unknown origins below a few hundred eV, and larger than expected from known backgrounds. Due to the significant impact of this excess on the dark matter or neutrino sensitivity of these experiments, a collective effort has been started to share the knowledge about the individual observations. For this, the EXCESS Workshop was&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.05097v2-abstract-full').style.display = 'inline'; document.getElementById('2202.05097v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.05097v2-abstract-full" style="display: none;"> Many low-threshold experiments observe sharply rising event rates of yet unknown origins below a few hundred eV, and larger than expected from known backgrounds. Due to the significant impact of this excess on the dark matter or neutrino sensitivity of these experiments, a collective effort has been started to share the knowledge about the individual observations. For this, the EXCESS Workshop was initiated. In its first iteration in June 2021, ten rare event search collaborations contributed to this initiative via talks and discussions. The contributing collaborations were CONNIE, CRESST, DAMIC, EDELWEISS, MINER, NEWS-G, NUCLEUS, RICOCHET, SENSEI and SuperCDMS. They presented data about their observed energy spectra and known backgrounds together with details about the respective measurements. In this paper, we summarize the presented information and give a comprehensive overview of the similarities and differences between the distinct measurements. The provided data is furthermore publicly available on the workshop&#39;s data repository together with a plotting tool for visualization. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.05097v2-abstract-full').style.display = 'none'; document.getElementById('2202.05097v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 10 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">44 pages, 20 figures; Editors: A. Fuss, M. Kaznacheeva, F. Reindl, F. Wagner; updated copyright statements and funding information</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> SciPost Phys. Proc. 9, 001 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2201.01639">arXiv:2201.01639</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2201.01639">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1007/s10909-022-02899-2">10.1007/s10909-022-02899-2 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> High impedance TES bolometers for EDELWEISS </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Fillipini%2C+J+-">J. -B. Fillipini</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a> , et al. (13 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2201.01639v1-abstract-short" style="display: inline;"> The EDELWEISS collaboration aims for direct detection of light dark matter using germanium cryogenic detectors with low threshold phonon sensor technologies and efficient charge readout designs. We describe here the development of Ge bolometers equipped with high impedance thermistors based on a NbxSi1-x TES alloy. High aspect ratio spiral designs allow the TES impedance to match with JFET or HEMT&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2201.01639v1-abstract-full').style.display = 'inline'; document.getElementById('2201.01639v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2201.01639v1-abstract-full" style="display: none;"> The EDELWEISS collaboration aims for direct detection of light dark matter using germanium cryogenic detectors with low threshold phonon sensor technologies and efficient charge readout designs. We describe here the development of Ge bolometers equipped with high impedance thermistors based on a NbxSi1-x TES alloy. High aspect ratio spiral designs allow the TES impedance to match with JFET or HEMT front-end amplifiers. We detail the behavior of the superconducting transition properties of these sensors and the detector optimization in terms of sensitivity to out-of-equilibrium phonons. We report preliminary results of a 200 g Ge detector that was calibrated using 71Ge activation by neutrons at the LSM underground laboratory. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2201.01639v1-abstract-full').style.display = 'none'; document.getElementById('2201.01639v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Submitted to Journal of Low Temperature Physics, Special Issue for the 19th International Workshop on Low Temperature Detectors 19-29 July 2021 (Virtual event hold by NIST)</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2112.11759">arXiv:2112.11759</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2112.11759">pdf</a>, <a href="https://arxiv.org/format/2112.11759">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1007/s10909-022-02826-5">10.1007/s10909-022-02826-5 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Phonon and charge signals from IR and X excitation in the SELENDIS Ge cryogenic detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Oriol%2C+C">C. Oriol</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2112.11759v1-abstract-short" style="display: inline;"> The aim of the SELENDIS project within the EDELWEISS collaboration is to observe single $e^- h^+$ pairs in lightweight (3.3 g) cryogenic germanium bolometers with charge and phonon readout at biases up to $\sim 100$ V. These devices are ideal to characterize in detail the mechanism of charge creation and collection in cryogenic germanium detectors. Electron-hole pairs are produced in the bulk of t&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.11759v1-abstract-full').style.display = 'inline'; document.getElementById('2112.11759v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2112.11759v1-abstract-full" style="display: none;"> The aim of the SELENDIS project within the EDELWEISS collaboration is to observe single $e^- h^+$ pairs in lightweight (3.3 g) cryogenic germanium bolometers with charge and phonon readout at biases up to $\sim 100$ V. These devices are ideal to characterize in detail the mechanism of charge creation and collection in cryogenic germanium detectors. Electron-hole pairs are produced in the bulk of the detector either by the injection of pulsed IR laser or by neutron activation of germanium inducing the K, L and M lines from $^{71}$Ge electron capture decays. Low-energy laser pulses are also used to probe the single $e^- h^+$ pair sensitivity of Ge bolometers. Preliminary results are used to compare these two modes of charge creation, an important step toward a detailed characterization of Ge bolometers for their use in sub-MeV Dark Matter (DM) searches. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.11759v1-abstract-full').style.display = 'none'; document.getElementById('2112.11759v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 22 December, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">8 pages, 6 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JLTP (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2112.05467">arXiv:2112.05467</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2112.05467">pdf</a>, <a href="https://arxiv.org/format/2112.05467">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> Low-mass Dark Matter searches with EDELWEISS </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Benoit%2C+A">A. Benoit</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+-">J. -B. Filippini</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a> , et al. (13 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2112.05467v2-abstract-short" style="display: inline;"> The EDELWEISS collaboration searches for light Dark Matter (DM) particles using germanium detectors equipped with a charge and phonon signal readout. Using the Neganov-Trofimov-Luke effect, an rms resolution of 0.53 electron-hole pair was obtained on a massive (33.4 g) Ge detector operated underground at the Laboratoire Souterrain de Modane. This record sensitivity made possible a search for Dark&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.05467v2-abstract-full').style.display = 'inline'; document.getElementById('2112.05467v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2112.05467v2-abstract-full" style="display: none;"> The EDELWEISS collaboration searches for light Dark Matter (DM) particles using germanium detectors equipped with a charge and phonon signal readout. Using the Neganov-Trofimov-Luke effect, an rms resolution of 0.53 electron-hole pair was obtained on a massive (33.4 g) Ge detector operated underground at the Laboratoire Souterrain de Modane. This record sensitivity made possible a search for Dark Photon DM down to 1 eV/c2 and to DM-electron interactions below 1 MeV/c2. This demonstrates for the first time the high relevance of cryogenic Ge detectors in searches at low thresholds and is an important step of the development of Ge detectors with improved performance in the context of the EDELWEISS-SubGeV program. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.05467v2-abstract-full').style.display = 'none'; document.getElementById('2112.05467v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 10 December, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Submitted to Journal of Low Temperature Physics, Special Issue for the 19th International Workshop on Low Temperature Detectors 19-29 July 2021 (Virtual event hold by NIST)</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2111.12857">arXiv:2111.12857</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.12857">pdf</a>, <a href="https://arxiv.org/format/2111.12857">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> Improvement of contact-less KID design using multilayered Al/Ti material for resonator </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=Calvo%2C+M">M. Calvo</a>, <a href="/search/?searchtype=author&amp;query=Goupy%2C+J">J. Goupy</a>, <a href="/search/?searchtype=author&amp;query=Monfardini%2C+A">A. Monfardini</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Vagneron%2C+L">L. Vagneron</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2111.12857v1-abstract-short" style="display: inline;"> The necessity to increase exposure in rare event searches experiments by maintaining a low energy threshold and a good energy resolution leads to segmented detectors as in EDELWEISS (Dark Matter), CUORE (0谓\b{eta}\b{eta}) or RICOCHET (CE谓NS) for example. However, the large number of sub-elements can dramatically increase the complexity of such detector arrays. In this work we report on our progres&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.12857v1-abstract-full').style.display = 'inline'; document.getElementById('2111.12857v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.12857v1-abstract-full" style="display: none;"> The necessity to increase exposure in rare event searches experiments by maintaining a low energy threshold and a good energy resolution leads to segmented detectors as in EDELWEISS (Dark Matter), CUORE (0谓\b{eta}\b{eta}) or RICOCHET (CE谓NS) for example. However, the large number of sub-elements can dramatically increase the complexity of such detector arrays. In this work we report on our progress towards designing a flexible detector technology based on KID resonators evaporated on massive target crystals readout by a contact-less feed-line. Providing that we achieve O(100) eV energy threshold, such approach could easily be scaled to tens of kilogram detector arrays thanks to the intrinsic multiplexing capability of mKIDs. Using a 30 g silicon target absorber with Al/Ti multilayers for the KID resonator, we report a significant improvement of our detector response exhibiting a keV-scale energy resolution combined with the absence of position dependence on the event location. Indeed, compared to our previous work, we are now able to properly identify calibration lines from surface (20 keV X-rays) and bulk events (60 keV gamma rays). This significant improvement is an important step toward a better understanding of phonons and quasiparticles dynamics which is pivotal in optimizing this technology. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.12857v1-abstract-full').style.display = 'none'; document.getElementById('2111.12857v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 November, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2021. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2111.12438">arXiv:2111.12438</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.12438">pdf</a>, <a href="https://arxiv.org/format/2111.12438">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Optimization and performance of the CryoCube detector for the future RICOCHET low-energy neutrino experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Salagnac%2C+T">T. Salagnac</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+-">J. -B. Filippini</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a>, <a href="/search/?searchtype=author&amp;query=Oriol%2C+C">C. Oriol</a>, <a href="/search/?searchtype=author&amp;query=Vagneron%2C+L">L. Vagneron</a>, <a href="/search/?searchtype=author&amp;query=collaboration%2C+t+R">the RICOCHET collaboration</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2111.12438v1-abstract-short" style="display: inline;"> The RICOCHET reactor neutrino observatory is planned to be installed at Institut Laue-Langevin starting in mid-2022. The scientific goal of the RICOCHET collaboration is to perform a low-energy and percentage-precision CENNS measurement in order to explore exotic physics scenarios beyond the standard model. To that end, RICOCHET will host two cryogenic detector arrays : the CryoCube (Ge target) an&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.12438v1-abstract-full').style.display = 'inline'; document.getElementById('2111.12438v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.12438v1-abstract-full" style="display: none;"> The RICOCHET reactor neutrino observatory is planned to be installed at Institut Laue-Langevin starting in mid-2022. The scientific goal of the RICOCHET collaboration is to perform a low-energy and percentage-precision CENNS measurement in order to explore exotic physics scenarios beyond the standard model. To that end, RICOCHET will host two cryogenic detector arrays : the CryoCube (Ge target) and the Q-ARRAY (Zn target), both with unprecedented sensitivity to O(10)eV nuclear recoils. The CryoCube will be composed of 27 Ge crystals of 38g instrumented with NTD-Ge thermal sensor as well as aluminum electrodes operated at 10mK in order to measure both the ionization and the heat energies arising from a particle interaction. To be a competitive CENNS detector, the CryoCube array is designed with the following specifications : a low energy threshold ($\sim 50$eV), the ability to identify and reject with a high efficiency the overwhelming electromagnetic backgrounds (gamma, betas, X-rays) and a sufficient payload ($\sim 1$kg). After a brief introduction of the future RICOCHET experiment and its CryoCube, the current works and first performance results on the optimization of the heat channel and the electrode designs will be presented. We conclude with a preliminary estimation of the CryoCube sensitivity to the CENNS signal within RICOCHET. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.12438v1-abstract-full').style.display = 'none'; document.getElementById('2111.12438v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 November, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Submitted to Journal of Low Temperature Physics, Special Issue for the 19th International Workshop on Low Temperature Detectors 19-29 July 2021 (Virtual event hold by NIST)</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2111.10308">arXiv:2111.10308</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.10308">pdf</a>, <a href="https://arxiv.org/format/2111.10308">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1007/s10909-022-02896-5">10.1007/s10909-022-02896-5 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> HEMT-based 1K front-end electronics for the heat and ionization Ge CryoCube of the future RICOCHET CE$谓$NS experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Baulieu%2C+G">G. Baulieu</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J">J-L Bret</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=Dong%2C+Q">Q. Dong</a>, <a href="/search/?searchtype=author&amp;query=Exshaw%2C+O">O. Exshaw</a>, <a href="/search/?searchtype=author&amp;query=Guerin%2C+C">C. Guerin</a>, <a href="/search/?searchtype=author&amp;query=Ferriol%2C+S">S. Ferriol</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J">J-B Filippini</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Lamblin%2C+J">J. Lamblin</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a>, <a href="/search/?searchtype=author&amp;query=Minet%2C+J">J. Minet</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a>, <a href="/search/?searchtype=author&amp;query=Monfardini%2C+A">A. Monfardini</a>, <a href="/search/?searchtype=author&amp;query=Rarbi%2C+F">F. Rarbi</a>, <a href="/search/?searchtype=author&amp;query=Salagnac%2C+T">T. Salagnac</a>, <a href="/search/?searchtype=author&amp;query=Vagneron%2C+L">L. Vagneron</a>, <a href="/search/?searchtype=author&amp;query=Collaboration%2C+t+R">the RICOCHET Collaboration</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2111.10308v2-abstract-short" style="display: inline;"> The RICOCHET reactor neutrino observatory is planned to be installed at the Laue Langevin Institute (ILL) starting mid-2022. Its scientific goal is to perform a low-energy and high precision measurement of the coherent elastic neutrino-nucleus scattering (CE$谓$NS) spectrum in order to explore exotic physics scenarios. RICOCHET will host two cryogenic detector arrays: the CryoCube (Ge target) and t&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.10308v2-abstract-full').style.display = 'inline'; document.getElementById('2111.10308v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.10308v2-abstract-full" style="display: none;"> The RICOCHET reactor neutrino observatory is planned to be installed at the Laue Langevin Institute (ILL) starting mid-2022. Its scientific goal is to perform a low-energy and high precision measurement of the coherent elastic neutrino-nucleus scattering (CE$谓$NS) spectrum in order to explore exotic physics scenarios. RICOCHET will host two cryogenic detector arrays: the CryoCube (Ge target) and the Q-ARRAY (Zn target), operated at 10 mK. The 1 kg Ge CryoCube will consist of 27 Ge crystals instrumented with NTD-Ge thermal sensors and charge collection electrodes for a simultaneous heat and ionization readout to reject the electromagnetic backgrounds (gamma, beta, x-rays). We present the status of its front-end electronics. The first stage of amplification is made of High Electron Mobility Transistor (HEMT) developed by CNRS/C2N laboratory, optimized to achieve ultra-low noise performance at 1K with a dissipation as low as 15 $渭$W per channel. Our noise model predicts that 10 eV heat and 20 eVee RMS baseline resolutions are feasible with a high dynamic range for the deposited energy (up to 10 MeV) thanks to loop amplification schemes. Such resolutions are mandatory to have a high discrimination power between nuclear and electron recoils at the lowest energies. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.10308v2-abstract-full').style.display = 'none'; document.getElementById('2111.10308v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 30 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 19 November, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">submitted to Journal of Low Temperature Physics. Special Issue for the 19th International Workshop on Low Temperature Detectors 19-29 July 2021 - Virtual event hold by NIST</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Journal of Low Temperature Physics 209, pages 570-580 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2111.06745">arXiv:2111.06745</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.06745">pdf</a>, <a href="https://arxiv.org/format/2111.06745">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Ricochet Progress and Status </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Ricochet+Collaboration"> Ricochet Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Beaulieu%2C+G">G. Beaulieu</a>, <a href="/search/?searchtype=author&amp;query=Belov%2C+V">V. Belov</a>, <a href="/search/?searchtype=author&amp;query=Berge%2C+L">L. Berge</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Bret%2C+J+L">J-. L. Bret</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Calvo%2C+M">M. Calvo</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Chaplinsky%2C+L">L. Chaplinsky</a>, <a href="/search/?searchtype=author&amp;query=Chemin%2C+G">G. Chemin</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+R">R. Chen</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">J. Colas</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Exshaw%2C+O">O. Exshaw</a>, <a href="/search/?searchtype=author&amp;query=Ferriol%2C+S">S. Ferriol</a>, <a href="/search/?searchtype=author&amp;query=Figueroa-Feliciano%2C+E">E. Figueroa-Feliciano</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J+B">J. B. Filippini</a>, <a href="/search/?searchtype=author&amp;query=Formaggio%2C+J+A">J. A. Formaggio</a>, <a href="/search/?searchtype=author&amp;query=Fuard%2C+S">S. Fuard</a> , et al. (55 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2111.06745v1-abstract-short" style="display: inline;"> We present an overview of recent progress towards the Ricochet coherent elastic neutrino nucleus scattering CE$谓$NS experiment. The ILL research reactor in Grenoble, France has been selected as the experiment site, after in situ studies of vibration and particle backgrounds. We present background rate estimates specific to that site, along with descriptions of the planned CryoCube and Q-Array dete&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.06745v1-abstract-full').style.display = 'inline'; document.getElementById('2111.06745v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.06745v1-abstract-full" style="display: none;"> We present an overview of recent progress towards the Ricochet coherent elastic neutrino nucleus scattering CE$谓$NS experiment. The ILL research reactor in Grenoble, France has been selected as the experiment site, after in situ studies of vibration and particle backgrounds. We present background rate estimates specific to that site, along with descriptions of the planned CryoCube and Q-Array detector payloads. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.06745v1-abstract-full').style.display = 'none'; document.getElementById('2111.06745v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 November, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Proceedings for the 19th International Workshop on Low Temperature Detectors (LTD19)</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.13806">arXiv:2011.13806</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.13806">pdf</a>, <a href="https://arxiv.org/format/2011.13806">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/16/02/P02037">10.1088/1748-0221/16/02/P02037 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> A CUPID Li$_{2}$$^{100}$MoO$_4$ scintillating bolometer tested in the CROSS underground facility </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=The+CUPID+Interest+Group"> The CUPID Interest Group</a>, <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Armstrong%2C+W">W. Armstrong</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Bandac%2C+I+C">I. C. Bandac</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Bourgeois%2C+C">Ch. Bourgeois</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a>, <a href="/search/?searchtype=author&amp;query=Calvo-Mozota%2C+J+M">J. M. Calvo-Mozota</a>, <a href="/search/?searchtype=author&amp;query=Camilleri%2C+J">J. Camilleri</a> , et al. (156 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2011.13806v1-abstract-short" style="display: inline;"> A scintillating bolometer based on a large cubic Li$_{2}$$^{100}$MoO$_4$ crystal (45 mm side) and a Ge wafer (scintillation detector) has been operated in the CROSS cryogenic facility at the Canfranc underground laboratory in Spain. The dual-readout detector is a prototype of the technology that will be used in the next-generation $0\nu2尾$ experiment CUPID. The measurements were performed at 18 an&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.13806v1-abstract-full').style.display = 'inline'; document.getElementById('2011.13806v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.13806v1-abstract-full" style="display: none;"> A scintillating bolometer based on a large cubic Li$_{2}$$^{100}$MoO$_4$ crystal (45 mm side) and a Ge wafer (scintillation detector) has been operated in the CROSS cryogenic facility at the Canfranc underground laboratory in Spain. The dual-readout detector is a prototype of the technology that will be used in the next-generation $0\nu2尾$ experiment CUPID. The measurements were performed at 18 and 12 mK temperature in a pulse tube dilution refrigerator. This setup utilizes the same technology as the CUORE cryostat that will host CUPID and so represents an accurate estimation of the expected performance. The Li$_{2}$$^{100}$MoO$_4$ bolometer shows a high energy resolution of 6 keV FWHM at the 2615 keV $纬$ line. The detection of scintillation light for each event triggered by the Li$_{2}$$^{100}$MoO$_4$ bolometer allowed for a full separation ($\sim$8$蟽$) between $纬$($尾$) and $伪$ events above 2 MeV. The Li$_{2}$$^{100}$MoO$_4$ crystal also shows a high internal radiopurity with $^{228}$Th and $^{226}$Ra activities of less than 3 and 8 $渭$Bq/kg, respectively. Taking also into account the advantage of a more compact and massive detector array, which can be made of cubic-shaped crystals (compared to the cylindrical ones), this test demonstrates the great potential of cubic Li$_{2}$$^{100}$MoO$_4$ scintillating bolometers for high-sensitivity searches for the $^{100}$Mo $0\nu2尾$ decay in CROSS and CUPID projects. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.13806v1-abstract-full').style.display = 'none'; document.getElementById('2011.13806v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 27 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">19 pages, 7 figures, 1 table</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.13656">arXiv:2011.13656</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.13656">pdf</a>, <a href="https://arxiv.org/format/2011.13656">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Characterization of cubic Li$_{2}$$^{100}$MoO$_4$ crystals for the CUPID experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Armstrong%2C+W">W. Armstrong</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A">A. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A8%2C+L">L. Berg猫</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a>, <a href="/search/?searchtype=author&amp;query=Camilleri%2C+J">J. Camilleri</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+S">S. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Cappelli%2C+L">L. Cappelli</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Carniti%2C+P">P. Carniti</a> , et al. (147 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2011.13656v1-abstract-short" style="display: inline;"> The CUPID Collaboration is designing a tonne-scale, background-free detector to search for double beta decay with sufficient sensitivity to fully explore the parameter space corresponding to the inverted neutrino mass hierarchy scenario. One of the CUPID demonstrators, CUPID-Mo, has proved the potential of enriched Li$_{2}$$^{100}$MoO$_4$ crystals as suitable detectors for neutrinoless double beta&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.13656v1-abstract-full').style.display = 'inline'; document.getElementById('2011.13656v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.13656v1-abstract-full" style="display: none;"> The CUPID Collaboration is designing a tonne-scale, background-free detector to search for double beta decay with sufficient sensitivity to fully explore the parameter space corresponding to the inverted neutrino mass hierarchy scenario. One of the CUPID demonstrators, CUPID-Mo, has proved the potential of enriched Li$_{2}$$^{100}$MoO$_4$ crystals as suitable detectors for neutrinoless double beta decay search. In this work, we characterised cubic crystals that, compared to the cylindrical crystals used by CUPID-Mo, are more appealing for the construction of tightly packed arrays. We measured an average energy resolution of (6.7$\pm$0.6) keV FWHM in the region of interest, approaching the CUPID target of 5 keV FWHM. We assessed the identification of $伪$ particles with and without a reflecting foil that enhances the scintillation light collection efficiency, proving that the baseline design of CUPID already ensures a complete suppression of this $伪$-induced background contribution. We also used the collected data to validate a Monte Carlo simulation modelling the light collection efficiency, which will enable further optimisations of the detector. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.13656v1-abstract-full').style.display = 'none'; document.getElementById('2011.13656v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 27 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2020. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.13243">arXiv:2011.13243</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.13243">pdf</a>, <a href="https://arxiv.org/format/2011.13243">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevLett.126.181802">10.1103/PhysRevLett.126.181802 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> New Limit for Neutrinoless Double-Beta Decay of $^{100}$Mo from the CUPID-Mo Experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Bourgeois%2C+C">Ch. Bourgeois</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V+B">V. B. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=Chiesa%2C+D">D. Chiesa</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a> , et al. (69 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2011.13243v2-abstract-short" style="display: inline;"> The CUPID-Mo experiment at the Laboratoire Souterrain de Modane (France) is a demonstrator for CUPID, the next-generation ton-scale cryogenic $0谓尾尾$ experiment. It consists of a 4.2 kg array of 20 enriched Li$_{2}$$^{100}$MoO$_4$ scintillating bolometers to search for the lepton number violating process of $0谓尾尾$ decay in $^{100}$Mo. With more than one year of operation (2.16 kg$\times$yr of physi&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.13243v2-abstract-full').style.display = 'inline'; document.getElementById('2011.13243v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.13243v2-abstract-full" style="display: none;"> The CUPID-Mo experiment at the Laboratoire Souterrain de Modane (France) is a demonstrator for CUPID, the next-generation ton-scale cryogenic $0谓尾尾$ experiment. It consists of a 4.2 kg array of 20 enriched Li$_{2}$$^{100}$MoO$_4$ scintillating bolometers to search for the lepton number violating process of $0谓尾尾$ decay in $^{100}$Mo. With more than one year of operation (2.16 kg$\times$yr of physics data), no event in the region of interest and hence no evidence for $0谓尾尾$ is observed. We report a new limit on the half-life of $0谓尾尾$ decay in $^{100}$Mo of $T_{1/2} &gt; 1.5 \times 10^{24}\,$yr at 90 % C.I. The limit corresponds to an effective Majorana neutrino mass $\langle m_{尾尾} \rangle$ $&lt;$ (0.31--0.54)$\,$eV, dependent on the nuclear matrix element in the light Majorana neutrino exchange interpretation. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.13243v2-abstract-full').style.display = 'none'; document.getElementById('2011.13243v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 May, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 126, 181802 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.11726">arXiv:2011.11726</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.11726">pdf</a>, <a href="https://arxiv.org/format/2011.11726">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.104.015501">10.1103/PhysRevC.104.015501 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Novel technique for the study of pile-up events in cryogenic bolometers </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armatol%2C+A">A. Armatol</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Armstrong%2C+W">W. Armstrong</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Avignone%2C+F+T">F. T. Avignone III</a>, <a href="/search/?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A">A. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bari%2C+G">G. Bari</a>, <a href="/search/?searchtype=author&amp;query=Barresi%2C+A">A. Barresi</a>, <a href="/search/?searchtype=author&amp;query=Baudin%2C+D">D. Baudin</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Biassoni%2C+M">M. Biassoni</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boldrini%2C+V">V. Boldrini</a>, <a href="/search/?searchtype=author&amp;query=Branca%2C+A">A. Branca</a>, <a href="/search/?searchtype=author&amp;query=Brofferio%2C+C">C. Brofferio</a>, <a href="/search/?searchtype=author&amp;query=Bucci%2C+C">C. Bucci</a>, <a href="/search/?searchtype=author&amp;query=Camilleri%2C+J">J. Camilleri</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+S">S. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Cappelli%2C+L">L. Cappelli</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Carniti%2C+P">P. Carniti</a> , et al. (144 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2011.11726v2-abstract-short" style="display: inline;"> Precise characterization of detector time resolution is of crucial importance for next-generation cryogenic-bolometer experiments searching for neutrinoless double-beta decay, such as CUPID, in order to reject background due to pile-up of two-neutrino double-beta decay events. In this paper, we describe a technique developed to study the pile-up rejection capability of cryogenic bolometers. Our ap&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.11726v2-abstract-full').style.display = 'inline'; document.getElementById('2011.11726v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.11726v2-abstract-full" style="display: none;"> Precise characterization of detector time resolution is of crucial importance for next-generation cryogenic-bolometer experiments searching for neutrinoless double-beta decay, such as CUPID, in order to reject background due to pile-up of two-neutrino double-beta decay events. In this paper, we describe a technique developed to study the pile-up rejection capability of cryogenic bolometers. Our approach, which consists of producing controlled pile-up events with a programmable waveform generator, has the benefit that we can reliably and reproducibly control the time separation and relative energy of the individual components of the generated pile-up events. The resulting data allow us to optimize and benchmark analysis strategies to discriminate between individual and pile-up pulses. We describe a test of this technique performed with a small array of detectors at the Laboratori Nazionali del Gran Sasso, in Italy; we obtain a 90% rejection efficiency against pulser-generated pile-up events with rise time of ~15ms down to time separation between the individual events of about 2ms. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.11726v2-abstract-full').style.display = 'none'; document.getElementById('2011.11726v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 July, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 23 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 104, 015501 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2010.04033">arXiv:2010.04033</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2010.04033">pdf</a>, <a href="https://arxiv.org/format/2010.04033">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Data Analysis, Statistics and Probability">physics.data-an</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/16/03/P03032">10.1088/1748-0221/16/03/P03032 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Pulse Shape Discrimination in CUPID-Mo using Principal Component Analysis </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Huang%2C+R">R. Huang</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Bourgeois%2C+C">Ch. Bourgeois</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V+B">V. B. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dixon%2C+T">T. Dixon</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a> , et al. (64 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2010.04033v2-abstract-short" style="display: inline;"> CUPID-Mo is a cryogenic detector array designed to search for neutrinoless double-beta decay ($0谓尾尾$) of $^{100}$Mo. It uses 20 scintillating $^{100}$Mo-enriched Li$_2$MoO$_4$ bolometers instrumented with Ge light detectors to perform active suppression of $伪$ backgrounds, drastically reducing the expected background in the $0谓尾尾$ signal region. As a result, pileup events and small detector instab&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2010.04033v2-abstract-full').style.display = 'inline'; document.getElementById('2010.04033v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2010.04033v2-abstract-full" style="display: none;"> CUPID-Mo is a cryogenic detector array designed to search for neutrinoless double-beta decay ($0谓尾尾$) of $^{100}$Mo. It uses 20 scintillating $^{100}$Mo-enriched Li$_2$MoO$_4$ bolometers instrumented with Ge light detectors to perform active suppression of $伪$ backgrounds, drastically reducing the expected background in the $0谓尾尾$ signal region. As a result, pileup events and small detector instabilities that mimic normal signals become non-negligible potential backgrounds. These types of events can in principle be eliminated based on their signal shapes, which are different from those of regular bolometric pulses. We show that a purely data-driven principal component analysis based approach is able to filter out these anomalous events, without the aid of detector response simulations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2010.04033v2-abstract-full').style.display = 'none'; document.getElementById('2010.04033v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 23 March, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 8 October, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JINST 16 (2021) P03032 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2003.01046">arXiv:2003.01046</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2003.01046">pdf</a>, <a href="https://arxiv.org/format/2003.01046">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Astrophysics of Galaxies">astro-ph.GA</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevLett.125.141301">10.1103/PhysRevLett.125.141301 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> First germanium-based constraints on sub-MeV Dark Matter with the EDELWEISS experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=EDELWEISS+Collaboration"> EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Elkhoury%2C+E">E. Elkhoury</a>, <a href="/search/?searchtype=author&amp;query=Fillipini%2C+J+-">J. -B. Fillipini</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Lattaud%2C+H">H. Lattaud</a> , et al. (17 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2003.01046v2-abstract-short" style="display: inline;"> The EDELWEISS collaboration has performed a search for Dark Matter (DM) particles interacting with electrons using a 33.4 g Ge cryogenic detector operated underground at the LSM. A charge resolution of 0.53 electron-hole pairs (RMS) has been achieved using the Neganov-Trofimov-Luke amplification with a bias of 78 V. We set the first Ge-based constraints on sub-MeV/c$^{2}$ DM particles interacting&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2003.01046v2-abstract-full').style.display = 'inline'; document.getElementById('2003.01046v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2003.01046v2-abstract-full" style="display: none;"> The EDELWEISS collaboration has performed a search for Dark Matter (DM) particles interacting with electrons using a 33.4 g Ge cryogenic detector operated underground at the LSM. A charge resolution of 0.53 electron-hole pairs (RMS) has been achieved using the Neganov-Trofimov-Luke amplification with a bias of 78 V. We set the first Ge-based constraints on sub-MeV/c$^{2}$ DM particles interacting with electrons, as well as on dark photons down to 1 eV/c$^2$. These are competitive with other searches. In particular, new limits are set on the kinetic mixing of dark photon DM in a so far unconstrained parameter space region in the 6 to 9 eV/c$^2$ mass range. These results demonstrate the high relevance of cryogenic Ge detectors for the search of DM interactions producing eV-scale electron signals. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2003.01046v2-abstract-full').style.display = 'none'; document.getElementById('2003.01046v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 2 March, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">6 pages, 4 figures, corrected typos</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 125, 141301 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1912.07272">arXiv:1912.07272</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1912.07272">pdf</a>, <a href="https://arxiv.org/ps/1912.07272">ps</a>, <a href="https://arxiv.org/format/1912.07272">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-020-8203-4">10.1140/epjc/s10052-020-8203-4 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Precise measurement of $2谓尾尾$ decay of $^{100}$Mo with the CUPID-Mo detection technology </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Bourgeois%2C+C">Ch. Bourgeois</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+M">M. Briere</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V">V. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a> , et al. (65 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1912.07272v1-abstract-short" style="display: inline;"> We report the measurement of the two-neutrino double-beta ($2谓尾尾$) decay of $^{100}$Mo to the ground state of $^{100}$Ru using lithium molybdate (\crystal) scintillating bolometers. The detectors were developed for the CUPID-Mo program and operated at the EDELWEISS-III low background facility in the Modane underground laboratory. From a total exposure of $42.235$ kg$\times$d, the half-life of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1912.07272v1-abstract-full').style.display = 'inline'; document.getElementById('1912.07272v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1912.07272v1-abstract-full" style="display: none;"> We report the measurement of the two-neutrino double-beta ($2谓尾尾$) decay of $^{100}$Mo to the ground state of $^{100}$Ru using lithium molybdate (\crystal) scintillating bolometers. The detectors were developed for the CUPID-Mo program and operated at the EDELWEISS-III low background facility in the Modane underground laboratory. From a total exposure of $42.235$ kg$\times$d, the half-life of $^{100}$Mo is determined to be $T_{1/2}^{2谓}=[7.12^{+0.18}_{-0.14}\,\mathrm{(stat.)}\pm0.10\,\mathrm{(syst.)}]\times10^{18}$ years. This is the most accurate determination of the $2谓尾尾$ half-life of $^{100}$Mo to date. We also confirm, with the statistical significance of $&gt;3蟽$, that the single-state dominance model of the $2谓尾尾$ decay of $^{100}$Mo is favored over the high-state dominance model. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1912.07272v1-abstract-full').style.display = 'none'; document.getElementById('1912.07272v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 16 December, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">11 pages, 6 figures, 4 tables</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1911.10426">arXiv:1911.10426</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1911.10426">pdf</a>, <a href="https://arxiv.org/format/1911.10426">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1742-6596/1468/1/012129">10.1088/1742-6596/1468/1/012129 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> First data from the CUPID-Mo neutrinoless double beta decay experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Schmidt%2C+B">B. Schmidt</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Bourgeois%2C+C">Ch. Bourgeois</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+M">M. Briere</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V+B">V. B. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a> , et al. (65 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1911.10426v1-abstract-short" style="display: inline;"> The CUPID-Mo experiment is searching for neutrinoless double beta decay in $^{100}$Mo, evaluating the technology of cryogenic scintillating Li$_{2}^{100}$MoO$_4$ detectors for CUPID (CUORE Upgrade with Particle ID). CUPID-Mo detectors feature background suppression using a dual-readout scheme with Li$_{2}$MoO$_4$ crystals complemented by Ge bolometers for light detection. The detection of both hea&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1911.10426v1-abstract-full').style.display = 'inline'; document.getElementById('1911.10426v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1911.10426v1-abstract-full" style="display: none;"> The CUPID-Mo experiment is searching for neutrinoless double beta decay in $^{100}$Mo, evaluating the technology of cryogenic scintillating Li$_{2}^{100}$MoO$_4$ detectors for CUPID (CUORE Upgrade with Particle ID). CUPID-Mo detectors feature background suppression using a dual-readout scheme with Li$_{2}$MoO$_4$ crystals complemented by Ge bolometers for light detection. The detection of both heat and scintillation light signals allows the efficient discrimination of $伪$ from $纬$&amp;$尾$ events. In this proceedings, we discuss results from the first 2 months of data taking in spring 2019. In addition to an excellent bolometric performance of 6.7$\,$keV (FWHM) at 2615$\,$keV and an $伪$ separation of better than 99.9\% for all detectors, we report on bulk radiopurity for Th and U. Finally, we interpret the accumulated physics data in terms of a limit of $T_{1/2}^{0谓}\,&gt; 3\times10^{23}\,$yr for $^{100}$Mo and discuss the sensitivity of CUPID-Mo until the expected end of physics data taking in early 2020. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1911.10426v1-abstract-full').style.display = 'none'; document.getElementById('1911.10426v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 23 November, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Proceedings for TAUP 2019, submitted to IOP Journal of Physics: Conference Series</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Journal of Physics: Conference Series 1468 (2020) 012129 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1909.02994">arXiv:1909.02994</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1909.02994">pdf</a>, <a href="https://arxiv.org/format/1909.02994">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-019-7578-6">10.1140/epjc/s10052-019-7578-6 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The CUPID-Mo experiment for neutrinoless double-beta decay: performance and prospects </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Benato%2C+G">G. Benato</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Beretta%2C+M">M. Beretta</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Borovlev%2C+Y+A">Yu. A. Borovlev</a>, <a href="/search/?searchtype=author&amp;query=Bourgeois%2C+C">Ch. Bourgeois</a>, <a href="/search/?searchtype=author&amp;query=Briere%2C+M">M. Briere</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V+B">V. B. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a> , et al. (64 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1909.02994v1-abstract-short" style="display: inline;"> CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($0谓尾尾$) of $^{100}$Mo. In this article, we detail the CUPID-Mo detector concept, assembly, installation in the underground laboratory in Modane in 2018, and provide results from the first datasets. The demonstrator consists of an array of 20 scintillating bolometers comprised of $^{100}$Mo-enriched 0.2 kg Li$_2$MoO&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.02994v1-abstract-full').style.display = 'inline'; document.getElementById('1909.02994v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1909.02994v1-abstract-full" style="display: none;"> CUPID-Mo is a bolometric experiment to search for neutrinoless double-beta decay ($0谓尾尾$) of $^{100}$Mo. In this article, we detail the CUPID-Mo detector concept, assembly, installation in the underground laboratory in Modane in 2018, and provide results from the first datasets. The demonstrator consists of an array of 20 scintillating bolometers comprised of $^{100}$Mo-enriched 0.2 kg Li$_2$MoO$_4$ crystals. The detectors are complemented by 20 thin cryogenic Ge bolometers acting as light detectors to distinguish $伪$ from $纬$/$尾$ events by the detection of both heat and scintillation light signals. We observe good detector uniformity, facilitating the operation of a large detector array as well as excellent energy resolution of 5.3 keV (6.5 keV) FWHM at 2615 keV, in calibration (physics) data. Based on the observed energy resolutions and light yields a separation of $伪$ particles at much better than 99.9\% with equally high acceptance for $纬$/$尾$ events is expected for events in the region of interest for $^{100}$Mo $0谓尾尾$. We present limits on the crystals&#39; radiopurity ($\leq$3 $渭$Bq/kg of $^{226}$Ra and $\leq$2 $渭$Bq/kg of $^{232}$Th). Based on these initial results we also discuss a sensitivity study for the science reach of the CUPID-Mo experiment, in particular, the ability to set the most stringent half-life limit on the $^{100}$Mo $0谓尾尾$ decay after half a year of livetime. The achieved results show that CUPID-Mo is a successful demonstrator of the technology - developed in the framework of the LUMINEU project - selected for the CUPID experiment, a proposed follow-up of CUORE, the currently running first tonne-scale cryogenic $0谓尾尾$ experiment. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.02994v1-abstract-full').style.display = 'none'; document.getElementById('1909.02994v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 6 September, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">15 pages, 18 figures, 3 tables; to be submitted to EPJC</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1909.02879">arXiv:1909.02879</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1909.02879">pdf</a>, <a href="https://arxiv.org/format/1909.02879">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1007/s10909-019-02269-5">10.1007/s10909-019-02269-5 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Low-noise HEMTs for Coherent Elastic Neutrino Scattering and Low-Mass Dark Matter Cryogenic Semiconductor Detectors </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Chaize%2C+D">D. Chaize</a>, <a href="/search/?searchtype=author&amp;query=Filippini%2C+J">J-B Filippini</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a>, <a href="/search/?searchtype=author&amp;query=Vagneron%2C+L">L. Vagneron</a>, <a href="/search/?searchtype=author&amp;query=Cavanna%2C+A">A. Cavanna</a>, <a href="/search/?searchtype=author&amp;query=Dong%2C+Q">Q. Dong</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Ulysse%2C+C">C. Ulysse</a>, <a href="/search/?searchtype=author&amp;query=Bounab%2C+A">A. Bounab</a>, <a href="/search/?searchtype=author&amp;query=de+la+Broise%2C+X">X. de la Broise</a>, <a href="/search/?searchtype=author&amp;query=Nones%2C+C">C. Nones</a>, <a href="/search/?searchtype=author&amp;query=Phipps%2C+A">A. Phipps</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1909.02879v2-abstract-short" style="display: inline;"> We present the noise performance of High Electron Mobility Transistors (HEMT) developed by CNRS-C2N laboratory. Various HEMT&#39;s gate geometries with 2 pF to 230 pF input capacitance have been studied at 4 K. A model for both voltage and current noises has been developed with frequency dependence up to 1 MHz. These HEMTs exhibit low dissipation, excellent noise performance and can advantageously rep&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.02879v2-abstract-full').style.display = 'inline'; document.getElementById('1909.02879v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1909.02879v2-abstract-full" style="display: none;"> We present the noise performance of High Electron Mobility Transistors (HEMT) developed by CNRS-C2N laboratory. Various HEMT&#39;s gate geometries with 2 pF to 230 pF input capacitance have been studied at 4 K. A model for both voltage and current noises has been developed with frequency dependence up to 1 MHz. These HEMTs exhibit low dissipation, excellent noise performance and can advantageously replace traditional Si-JFETs for the readout of high impedance thermal sensor and semiconductor ionization cryogenic detectors. Our model predicts that cryogenic germanium detectors of 30 g with 10 eV heat and 20 eVee baseline resolution are feasible if read out by HEMT based amplifiers. Such resolution allows for high discrimination between nuclear and electron recoils at low threshold. This capability is of major interest for Coherent Elastic Neutrino Scattering and low-mass dark matter experiments such as Ricochet and EDELWEISS. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.02879v2-abstract-full').style.display = 'none'; document.getElementById('1909.02879v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 December, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 6 September, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">submitted to Journal of Low Temperature Physics, special issue for the 18th International Workshop on Low Temperature Detectors 22-26 July 2019 - Milano, Italia</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Journal of Low Temperature Physics 2019 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1906.10397">arXiv:1906.10397</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1906.10397">pdf</a>, <a href="https://arxiv.org/format/1906.10397">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-ph</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1063/1.5116405">10.1063/1.5116405 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Contact-less phonon detection with massive cryogenic absorbers </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Goupy%2C+J">Johannes Goupy</a>, <a href="/search/?searchtype=author&amp;query=Colas%2C+J">Jules Colas</a>, <a href="/search/?searchtype=author&amp;query=Calvo%2C+M">Martino Calvo</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">Julien Billard</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">Philippe Camus</a>, <a href="/search/?searchtype=author&amp;query=Germond%2C+R">Richard Germond</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">Alexandre Juillard</a>, <a href="/search/?searchtype=author&amp;query=Vagneron%2C+L">Lionel Vagneron</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">Maryvonne De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Levy-Bertrand%2C+F">Florence Levy-Bertrand</a>, <a href="/search/?searchtype=author&amp;query=Monfardini%2C+A">Alessandro Monfardini</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1906.10397v2-abstract-short" style="display: inline;"> We have developed a contact-less technique for the real time measurement of a-thermal (Cooper-pair breaking) phonons in an absorber held at sub-Kelvin temperatures. In particular, a thin-film aluminum superconducting resonator was realized on a 30-grams high-resistivity silicon crystal. The lumped-element resonator is inductively excited/read-out by a radio-frequency microstrip feed-line deposited&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1906.10397v2-abstract-full').style.display = 'inline'; document.getElementById('1906.10397v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1906.10397v2-abstract-full" style="display: none;"> We have developed a contact-less technique for the real time measurement of a-thermal (Cooper-pair breaking) phonons in an absorber held at sub-Kelvin temperatures. In particular, a thin-film aluminum superconducting resonator was realized on a 30-grams high-resistivity silicon crystal. The lumped-element resonator is inductively excited/read-out by a radio-frequency microstrip feed-line deposited on another wafer; the sensor, a Kinetic Inductance Detector (KID), is read-out without any physical contact or wiring to the absorber. The resonator demonstrates excellent electrical properties, particularly in terms of its internal quality factor. The detection of alphas and gammas in the massive absorber is achieved, with an RMS energy resolution of about 1.4 keV, which is already interesting for particle physics applications. The resolution of this prototype detector is mainly limited by the low (about 0.3%) conversion efficiency of deposited energy to superconducting excitations (quasi-particles). The demonstrated technique can be further optimized, and used to produce large arrays of a-thermal phonon detectors, for use in rare events searches such as: dark matter direct detection,neutrino-less double beta decay, or coherent elastic neutrino-nucleus scattering. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1906.10397v2-abstract-full').style.display = 'none'; document.getElementById('1906.10397v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 November, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 25 June, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Accepted for publication on Applied Physics Letters</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Appl. Phys. Lett. 115, 223506 (2019) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1901.03588">arXiv:1901.03588</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1901.03588">pdf</a>, <a href="https://arxiv.org/format/1901.03588">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Astrophysics of Galaxies">astro-ph.GA</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.99.082003">10.1103/PhysRevD.99.082003 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Searching for low-mass dark matter particles with a massive Ge bolometer operated above-ground </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Benoit%2C+A">A. Benoit</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapelier%2C+M">M. Chapelier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=Ducimeti%C3%A8re%2C+D">D. Ducimeti猫re</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Maisonobe%2C+R">R. Maisonobe</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a> , et al. (16 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1901.03588v2-abstract-short" style="display: inline;"> The EDELWEISS collaboration has performed a search for dark matter particles with masses below the GeV-scale with a 33.4-g germanium cryogenic detector operated in a surface lab. The energy deposits were measured using a neutron-transmutation-doped Ge thermal sensor with a 17.7~eV (RMS) baseline heat energy resolution leading to a 60~eV analysis energy threshold. Despite a moderate lead shielding&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1901.03588v2-abstract-full').style.display = 'inline'; document.getElementById('1901.03588v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1901.03588v2-abstract-full" style="display: none;"> The EDELWEISS collaboration has performed a search for dark matter particles with masses below the GeV-scale with a 33.4-g germanium cryogenic detector operated in a surface lab. The energy deposits were measured using a neutron-transmutation-doped Ge thermal sensor with a 17.7~eV (RMS) baseline heat energy resolution leading to a 60~eV analysis energy threshold. Despite a moderate lead shielding and the high-background environment, the first sub-GeV spin-independent dark matter limit based on a germanium target has been achieved. The experiment provides the most stringent, nuclear recoil based, above-ground limit on spin-independent interactions above 600~MeV/c$^{2}$. The experiment also provides the most stringent limits on spin-dependent interactions with protons and neutrons below 1.3~GeV/c$^{2}$. Furthermore, the dark matter search results were studied in the context of Strongly Interacting Massive Particles, taking into account Earth-shielding effects, for which new regions of the available parameter space have been excluded. Finally, the dark matter search has also been extended to interactions via the Migdal effect, resulting for the first time in the exclusion of particles with masses between 45 and 150~MeV/c$^{2}$ with spin-independent cross sections ranging from $10^{-29}$ to $10^{-26}$~cm$^2$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1901.03588v2-abstract-full').style.display = 'none'; document.getElementById('1901.03588v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 April, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 11 January, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">16 pages, 8 figures. New figure added for Spin-Dependent interactions. Accepted in Phys. Rev. D</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 99, 082003 (2019) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1808.02340">arXiv:1808.02340</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1808.02340">pdf</a>, <a href="https://arxiv.org/format/1808.02340">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.98.082004">10.1103/PhysRevD.98.082004 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Searches for electron interactions induced by new physics in the EDELWEISS-III germanium bolometers </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Kozlov%2C+V">V. Kozlov</a>, <a href="/search/?searchtype=author&amp;query=Kraus%2C+H">H. Kraus</a>, <a href="/search/?searchtype=author&amp;query=Kudryavtsev%2C+V+A">V. A. Kudryavtsev</a>, <a href="/search/?searchtype=author&amp;query=Le-Sueur%2C+H">H. Le-Sueur</a>, <a href="/search/?searchtype=author&amp;query=Maisonobe%2C+R">R. Maisonobe</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a> , et al. (17 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1808.02340v2-abstract-short" style="display: inline;"> We make use of the EDELWEISS-III array of germanium bolometers to search for electron interactions at the keV scale induced by phenomena beyond the Standard Model. A 90% C.L. lower limit is set on the electron lifetime decaying to invisibles, $蟿&gt; 1.2\times 10^{24}$ years. We investigate the emission of axions or axionlike particles (ALPs) by the Sun, constraining the coupling parameters&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1808.02340v2-abstract-full').style.display = 'inline'; document.getElementById('1808.02340v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1808.02340v2-abstract-full" style="display: none;"> We make use of the EDELWEISS-III array of germanium bolometers to search for electron interactions at the keV scale induced by phenomena beyond the Standard Model. A 90% C.L. lower limit is set on the electron lifetime decaying to invisibles, $蟿&gt; 1.2\times 10^{24}$ years. We investigate the emission of axions or axionlike particles (ALPs) by the Sun, constraining the coupling parameters $g_{ae}&lt;1.1\times 10^{-11}$ and $g_{ae}\times g_{aN}^{\rm eff} &lt; 3.5\times 10^{-17}$ at 90% C.L. in the massless limit. We also directly search for the absorption of bosonic dark matter particles that would constitute our local galactic halo. Limits are placed on the couplings of ALPs or hidden photon dark matter in the mass range $0.8 - 500$ keV/c$^2$. Prospects for searching for dark matter particles with masses down to 150 eV/c$^2$ using improved detectors are presented. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1808.02340v2-abstract-full').style.display = 'none'; document.getElementById('1808.02340v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 November, 2018; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 7 August, 2018; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2018. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">8 pages, 5 figures, matches published version</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 98, 082004 (2018) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1803.03463">arXiv:1803.03463</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1803.03463">pdf</a>, <a href="https://arxiv.org/format/1803.03463">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/13/08/T08009">10.1088/1748-0221/13/08/T08009 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Vibration decoupling system for massive bolometers in dry cryostats </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Maisonobe%2C+R">R. Maisonobe</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Misiak%2C+D">D. Misiak</a>, <a href="/search/?searchtype=author&amp;query=Olivieri%2C+E">E. Olivieri</a>, <a href="/search/?searchtype=author&amp;query=Sayah%2C+S">S. Sayah</a>, <a href="/search/?searchtype=author&amp;query=Vagneron%2C+L">L. Vagneron</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1803.03463v3-abstract-short" style="display: inline;"> Pulse-tube based dilution refrigerators are massively employed in low temperature physics. They allow to reduce the running costs and to be operated with unprecedented easiness. However, the main drawback of this technology is the mechanical vibrations induced by the pulse-tube cryocooler. These perturbations can cause extra-noises drastically affecting the detector performance. In this paper, we&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1803.03463v3-abstract-full').style.display = 'inline'; document.getElementById('1803.03463v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1803.03463v3-abstract-full" style="display: none;"> Pulse-tube based dilution refrigerators are massively employed in low temperature physics. They allow to reduce the running costs and to be operated with unprecedented easiness. However, the main drawback of this technology is the mechanical vibrations induced by the pulse-tube cryocooler. These perturbations can cause extra-noises drastically affecting the detector performance. In this paper, we propose a solution to mitigate the impact of these vibrations by mounting the detectors in an elastic-pendulum based suspended tower. Based on vibration modeling and experimental tests, we show that the vibration levels are attenuated by up to two orders of magnitude at most frequencies, especially above $\sim20$ Hz, for both vertical and radial directions. Thanks to this passive isolation solution, vibration levels, both along vertical and radial directions, below 1 $渭\textrm{g/}\sqrt{\text{Hz}}$ in the frequency range [1-1000] Hz are obtained. This provides a convenient environment to test the ultimate performance of low temperature detectors. As a result, we report an improvement by one to two orders of magnitude on the noise levels of massive cryogenic bolometers, leading to thermal energy resolutions improved by a factor 5 to 40. Finally, we conclude that the energy resolution of our cryogenic bolometers are no longer limited from any residual vibrations, hence allowing the perspective of further improving our bolometer performance in the context of low-mass dark matter searches and neutrino physics applications. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1803.03463v3-abstract-full').style.display = 'none'; document.getElementById('1803.03463v3-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 September, 2018; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 9 March, 2018; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2018. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1710.03459">arXiv:1710.03459</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1710.03459">pdf</a>, <a href="https://arxiv.org/ps/1710.03459">ps</a>, <a href="https://arxiv.org/format/1710.03459">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.97.032501">10.1103/PhysRevC.97.032501 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Complete event-by-event $伪$/$纬(尾)$ separation in a full-size TeO$_2$ CUORE bolometer by Neganov-Luke-magnified light detection </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=de+Marcillac%2C+P">P. de Marcillac</a>, <a href="/search/?searchtype=author&amp;query=Marnieros%2C+S">S. Marnieros</a>, <a href="/search/?searchtype=author&amp;query=Nones%2C+C">C. Nones</a>, <a href="/search/?searchtype=author&amp;query=Novati%2C+V">V. Novati</a>, <a href="/search/?searchtype=author&amp;query=Olivieri%2C+E">E. Olivieri</a>, <a href="/search/?searchtype=author&amp;query=Paul%2C+B">B. Paul</a>, <a href="/search/?searchtype=author&amp;query=Poda%2C+D+V">D. V. Poda</a>, <a href="/search/?searchtype=author&amp;query=Redon%2C+T">T. Redon</a>, <a href="/search/?searchtype=author&amp;query=Siebenborn%2C+B">B. Siebenborn</a>, <a href="/search/?searchtype=author&amp;query=Zolotarova%2C+A+S">A. S. Zolotarova</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a> , et al. (19 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1710.03459v2-abstract-short" style="display: inline;"> In the present work, we describe the results obtained with a large ($\approx 133$ cm$^3$) TeO$_2$ bolometer, with a view to a search for neutrinoless double-beta decay ($0谓尾尾$) of $^{130}$Te. We demonstrate an efficient $伪$ particle discrimination (99.9\%) with a high acceptance of the $0谓尾尾$ signal (about 96\%), expected at $\approx 2.5$ MeV. This unprecedented result was possible thanks to the s&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1710.03459v2-abstract-full').style.display = 'inline'; document.getElementById('1710.03459v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1710.03459v2-abstract-full" style="display: none;"> In the present work, we describe the results obtained with a large ($\approx 133$ cm$^3$) TeO$_2$ bolometer, with a view to a search for neutrinoless double-beta decay ($0谓尾尾$) of $^{130}$Te. We demonstrate an efficient $伪$ particle discrimination (99.9\%) with a high acceptance of the $0谓尾尾$ signal (about 96\%), expected at $\approx 2.5$ MeV. This unprecedented result was possible thanks to the superior performance (10 eV rms baseline noise) of a Neganov-Luke-assisted germanium bolometer used to detect a tiny (70 eV) light signal from the TeO$_2$ detector, dominated by $纬$($尾$)-induced Cherenkov radiation but exhibiting also a clear scintillation component. The obtained results represent a major breakthrough towards the TeO$_2$-based version of CUORE Upgrade with Particle IDentification (CUPID), a ton-scale cryogenic $0谓尾尾$ experiment proposed as a follow-up to the CUORE project with particle identification. The CUORE experiment began recently a search for neutrinoless double-beta decay of $^{130}$Te with an array of 988 125-cm$^3$ TeO$_2$ bolometers. The lack of $伪$ discrimination in CUORE makes $伪$ decays at the detector surface the dominant background component, at the level of $\approx 0.01$ counts/(keV kg y) in the region of interest. We show here, for the first time with a CUORE-size bolometer and using the same technology as CUORE for the readout of both heat and light signals, that surface $伪$ background can be fully rejected. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1710.03459v2-abstract-full').style.display = 'none'; document.getElementById('1710.03459v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 25 April, 2018; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 10 October, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2017. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">The second version reflects the changes made after PRC referees&#39; comments</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 97, 032501(R) (2018) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1707.04308">arXiv:1707.04308</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1707.04308">pdf</a>, <a href="https://arxiv.org/format/1707.04308">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.97.022003">10.1103/PhysRevD.97.022003 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Optimizing EDELWEISS detectors for low-mass WIMP searches </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=EDELWEISS+Collaboration"> EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Foerster%2C+N">N. Foerster</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Hehn%2C+L">L. Hehn</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Kleifges%2C+M">M. Kleifges</a>, <a href="/search/?searchtype=author&amp;query=Kozlov%2C+V">V. Kozlov</a>, <a href="/search/?searchtype=author&amp;query=Kraus%2C+H">H. Kraus</a> , et al. (18 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1707.04308v1-abstract-short" style="display: inline;"> The physics potential of EDELWEISS detectors for the search of low-mass Weakly Interacting Massive Particles (WIMPs) is studied. Using a data-driven background model, projected exclusion limits are computed using frequentist and multivariate analysis approaches, namely profile likelihood and boosted decision tree. Both current and achievable experimental performance are considered. The optimal str&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1707.04308v1-abstract-full').style.display = 'inline'; document.getElementById('1707.04308v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1707.04308v1-abstract-full" style="display: none;"> The physics potential of EDELWEISS detectors for the search of low-mass Weakly Interacting Massive Particles (WIMPs) is studied. Using a data-driven background model, projected exclusion limits are computed using frequentist and multivariate analysis approaches, namely profile likelihood and boosted decision tree. Both current and achievable experimental performance are considered. The optimal strategy for detector optimization depends critically on whether the emphasis is put on WIMP masses below or above $\sim$ 5 GeV/c$^2$. The projected sensitivity for the next phase of the EDELWEISS-III experiment at the Modane Underground Laboratory (LSM) for low-mass WIMP search is presented. By 2018 an upper limit on the spin-independent WIMP-nucleon cross-section of $蟽_{SI} = 7 \times 10^{-42}$ cm$^2$ is expected for a WIMP mass in the range 2$-$5 GeV/c$^2$. The requirements for a future hundred-kilogram scale experiment designed to reach the bounds imposed by the coherent scattering of solar neutrinos are also described. By improving the ionization resolution down to 50 eV$_{ee}$, we show that such an experiment installed in an even lower background environment (e.g. at SNOLAB) should allow to observe about 80 $^8$B neutrino events after discrimination. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1707.04308v1-abstract-full').style.display = 'none'; document.getElementById('1707.04308v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 11 July, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2017. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">21 pages, 12 figures, submitted to Phys. Rev. D</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 97, 022003 (2018) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1706.01070">arXiv:1706.01070</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1706.01070">pdf</a>, <a href="https://arxiv.org/format/1706.01070">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/12/08/P08010">10.1088/1748-0221/12/08/P08010 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Performance of the EDELWEISS-III experiment for direct dark matter searches </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Bergmann%2C+T">T. Bergmann</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=de+Boissi%C3%A8re%2C+T">T. de Boissi猫re</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V">V. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Foerster%2C+N">N. Foerster</a>, <a href="/search/?searchtype=author&amp;query=Fourches%2C+N">N. Fourches</a>, <a href="/search/?searchtype=author&amp;query=Garde%2C+G">G. Garde</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Grollier%2C+M">M. Grollier</a> , et al. (38 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1706.01070v1-abstract-short" style="display: inline;"> We present the results of measurements demonstrating the efficiency of the EDELWEISS-III array of cryogenic germanium detectors for direct dark matter searches. The experimental setup and the FID (Fully Inter-Digitized) detector array is described, as well as the efficiency of the double measurement of heat and ionization signals in background rejection. For the whole set of 24 FID detectors used&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1706.01070v1-abstract-full').style.display = 'inline'; document.getElementById('1706.01070v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1706.01070v1-abstract-full" style="display: none;"> We present the results of measurements demonstrating the efficiency of the EDELWEISS-III array of cryogenic germanium detectors for direct dark matter searches. The experimental setup and the FID (Fully Inter-Digitized) detector array is described, as well as the efficiency of the double measurement of heat and ionization signals in background rejection. For the whole set of 24 FID detectors used for coincidence studies, the baseline resolutions for the fiducial ionization energy are mainly below 0.7 keV$_{ee}$ (FHWM) whereas the baseline resolutions for heat energies are mainly below 1.5 keV$_{ee}$ (FWHM). The response to nuclear recoils as well as the very good discrimination capability of the FID design has been measured with an AmBe source. The surface $尾$- and $伪$-decay rejection power of $R_{\rm surf} &lt; 4 \times 10^{-5}$ per $伪$ at 90% C.L. has been determined with a $^{210}$Pb source, the rejection of bulk $纬$-ray events has been demonstrated using $纬$-calibrations with $^{133}$Ba sources leading to a value of $R_{纬{\rm -mis-fid}} &lt; 2.5 \times 10^{-6}$ at 90% C.L.. The current levels of natural radioactivity measured in the detector array are shown as the rate of single $纬$ background. The fiducial volume fraction of the FID detectors has been measured to a weighted average value of $(74.6 \pm 0.4)\%$ using the cosmogenic activation of the $^{65}$Zn and $^{68,71}$Ge isotopes. The stability and uniformity of the detector response is also discussed. The achieved resolutions, thresholds and background levels of the upgraded EDELWEISS-III detectors in their setup are thus well suited to the direct search of WIMP dark matter over a large mass range. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1706.01070v1-abstract-full').style.display = 'none'; document.getElementById('1706.01070v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 June, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2017. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1704.01758">arXiv:1704.01758</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1704.01758">pdf</a>, <a href="https://arxiv.org/ps/1704.01758">ps</a>, <a href="https://arxiv.org/format/1704.01758">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-017-5343-2">10.1140/epjc/s10052-017-5343-2 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Development of $^{100}$Mo-containing scintillating bolometers for a high-sensitivity neutrinoless double-beta decay search </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Barabash%2C+A+S">A. S. Barabash</a>, <a href="/search/?searchtype=author&amp;query=Beeman%2C+J+W">J. W. Beeman</a>, <a href="/search/?searchtype=author&amp;query=Bekker%2C+T+B">T. B. Bekker</a>, <a href="/search/?searchtype=author&amp;query=Bellini%2C+F">F. Bellini</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Bergmann%2C+T">T. Bergmann</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Boiko%2C+R+S">R. S. Boiko</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V">V. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Capelli%2C+S">S. Capelli</a>, <a href="/search/?searchtype=author&amp;query=Cardani%2C+L">L. Cardani</a>, <a href="/search/?searchtype=author&amp;query=Casali%2C+N">N. Casali</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=Chernyak%2C+D+M">D. M. Chernyak</a>, <a href="/search/?searchtype=author&amp;query=de+Combarieu%2C+M">M. de Combarieu</a>, <a href="/search/?searchtype=author&amp;query=Coron%2C+N">N. Coron</a>, <a href="/search/?searchtype=author&amp;query=Danevich%2C+F+A">F. A. Danevich</a>, <a href="/search/?searchtype=author&amp;query=Dafinei%2C+I">I. Dafinei</a> , et al. (77 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1704.01758v2-abstract-short" style="display: inline;"> This paper reports on the development of a technology involving $^{100}$Mo-enriched scintillating bolometers, compatible with the goals of CUPID, a proposed next-generation bolometric experiment to search for neutrinoless double-beta decay. Large mass ($\sim$1~kg), high optical quality, radiopure $^{100}$Mo-containing zinc and lithium molybdate crystals have been produced and used to develop high&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1704.01758v2-abstract-full').style.display = 'inline'; document.getElementById('1704.01758v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1704.01758v2-abstract-full" style="display: none;"> This paper reports on the development of a technology involving $^{100}$Mo-enriched scintillating bolometers, compatible with the goals of CUPID, a proposed next-generation bolometric experiment to search for neutrinoless double-beta decay. Large mass ($\sim$1~kg), high optical quality, radiopure $^{100}$Mo-containing zinc and lithium molybdate crystals have been produced and used to develop high performance single detector modules based on 0.2--0.4~kg scintillating bolometers. In particular, the energy resolution of the lithium molybdate detectors near the $Q$-value of the double-beta transition of $^{100}$Mo (3034~keV) is 4--6~keV FWHM. The rejection of the $伪$-induced dominant background above 2.6~MeV is better than 8$蟽$. Less than 10~$渭$Bq/kg activity of $^{232}$Th ($^{228}$Th) and $^{226}$Ra in the crystals is ensured by boule recrystallization. The potential of $^{100}$Mo-enriched scintillating bolometers to perform high sensitivity double-beta decay searches has been demonstrated with only 10~kg$\times$d exposure: the two neutrino double-beta decay half-life of $^{100}$Mo has been measured with the up-to-date highest accuracy as $T_{1/2}$ = [6.90 $\pm$ 0.15(stat.) $\pm$ 0.37(syst.)] $\times$ 10$^{18}$~yr. Both crystallization and detector technologies favor lithium molybdate, which has been selected for the ongoing construction of the CUPID-0/Mo demonstrator, containing several kg of $^{100}$Mo. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1704.01758v2-abstract-full').style.display = 'none'; document.getElementById('1704.01758v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 October, 2017; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 6 April, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2017. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">25 pages, 12 figures, 8 tables; submitted to EPJC</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur. Phys. J. C 77 (2017) 785 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1703.08957">arXiv:1703.08957</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1703.08957">pdf</a>, <a href="https://arxiv.org/ps/1703.08957">ps</a>, <a href="https://arxiv.org/format/1703.08957">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1016/j.nima.2017.03.045">10.1016/j.nima.2017.03.045 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Vibrations on pulse tube based Dry Dilution Refrigerators for low noise measurements </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Olivieri%2C+E">E. Olivieri</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=De+Jesus%2C+M">M. De Jesus</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Leder%2C+A">A. Leder</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1703.08957v2-abstract-short" style="display: inline;"> Dry Dilution Refrigerators (DDR) based on pulse tube cryo-coolers have started to replace Wet Dilution Refrigerators (WDR) due to the ease and low cost of operation. However these advantages come at the cost of increased vibrations, induced by the pulse tube. In this work, we present the vibration measurements performed on three different commercial DDRs. We describe in detail the vibration measur&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1703.08957v2-abstract-full').style.display = 'inline'; document.getElementById('1703.08957v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1703.08957v2-abstract-full" style="display: none;"> Dry Dilution Refrigerators (DDR) based on pulse tube cryo-coolers have started to replace Wet Dilution Refrigerators (WDR) due to the ease and low cost of operation. However these advantages come at the cost of increased vibrations, induced by the pulse tube. In this work, we present the vibration measurements performed on three different commercial DDRs. We describe in detail the vibration measurement system we assembled, based on commercial accelerometers, conditioner and DAQ, and examined the effects of the various damping solutions utilized on three different DDRs, both in the low and high frequency regions. Finally, we ran low temperature, pseudo-massive (30 and 250 g) germanium bolometers in the best vibration-performing system under study and report on the results. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1703.08957v2-abstract-full').style.display = 'none'; document.getElementById('1703.08957v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 30 March, 2017; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 27 March, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2017. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1611.09712">arXiv:1611.09712</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1611.09712">pdf</a>, <a href="https://arxiv.org/format/1611.09712">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1016/j.nima.2019.06.022">10.1016/j.nima.2019.06.022 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> A HEMT-Based Cryogenic Charge Amplifier with sub-100 eVee Ionization Resolution for Massive Semiconductor Dark Matter Detectors </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Phipps%2C+A">A. Phipps</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a>, <a href="/search/?searchtype=author&amp;query=Sadoulet%2C+B">B. Sadoulet</a>, <a href="/search/?searchtype=author&amp;query=Serfass%2C+B">B. Serfass</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1611.09712v4-abstract-short" style="display: inline;"> We present the measured baseline ionization resolution of a HEMT-based cryogenic charge amplifier coupled to a CDMS-II detector. The amplifier has been developed to allow massive semiconductor dark matter detectors to retain background discrimination at the low recoil energies produced by low-mass WIMPs. We find a calibrated baseline ionization resolution of $蟽_E = 91\,\text{eV}_{ee}$. To our know&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1611.09712v4-abstract-full').style.display = 'inline'; document.getElementById('1611.09712v4-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1611.09712v4-abstract-full" style="display: none;"> We present the measured baseline ionization resolution of a HEMT-based cryogenic charge amplifier coupled to a CDMS-II detector. The amplifier has been developed to allow massive semiconductor dark matter detectors to retain background discrimination at the low recoil energies produced by low-mass WIMPs. We find a calibrated baseline ionization resolution of $蟽_E = 91\,\text{eV}_{ee}$. To our knowledge, this is the best direct ionization resolution achieved with such massive ($\approx$150 pF capacitance) radiation detectors. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1611.09712v4-abstract-full').style.display = 'none'; document.getElementById('1611.09712v4-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 18 June, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 November, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2016. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Published in Nuclear Instruments and Methods in Physics Research Section A</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1607.04560">arXiv:1607.04560</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1607.04560">pdf</a>, <a href="https://arxiv.org/format/1607.04560">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> Measurement of the cosmogenic activation of germanium detectors in EDELWEISS-III </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=The+EDELWEISS+Collaboration"> The EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bl%C3%BCmer%2C+J">J. Bl眉mer</a>, <a href="/search/?searchtype=author&amp;query=de+Boissi%C3%A8re%2C+T">T. de Boissi猫re</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Foerster%2C+N">N. Foerster</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Hehn%2C+L">L. Hehn</a>, <a href="/search/?searchtype=author&amp;query=Heuermann%2C+G">G. Heuermann</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a> , et al. (24 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1607.04560v1-abstract-short" style="display: inline;"> We present a measurement of the cosmogenic activation in the germanium cryogenic detectors of the EDELWEISS III direct dark matter search experiment. The decay rates measured in detectors with different exposures to cosmic rays above ground are converted into production rates of different isotopes. The measured production rates in units of nuclei/kg/day are 82 $\pm$ 21 for $^3$H, 2.8 $\pm$ 0.6 for&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1607.04560v1-abstract-full').style.display = 'inline'; document.getElementById('1607.04560v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1607.04560v1-abstract-full" style="display: none;"> We present a measurement of the cosmogenic activation in the germanium cryogenic detectors of the EDELWEISS III direct dark matter search experiment. The decay rates measured in detectors with different exposures to cosmic rays above ground are converted into production rates of different isotopes. The measured production rates in units of nuclei/kg/day are 82 $\pm$ 21 for $^3$H, 2.8 $\pm$ 0.6 for $^{49}$V, 4.6 $\pm$ 0.7 for $^{55}$Fe, and 106 $\pm$ 13 for $^{65}$Zn. These results are the most accurate for these isotopes. A lower limit on the production rate of $^{68}$Ge of 74 nuclei/kg/day is also presented. They are compared to model predictions present in literature and to estimates calculated with the ACTIVIA code. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1607.04560v1-abstract-full').style.display = 'none'; document.getElementById('1607.04560v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 15 July, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2016. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1607.03367">arXiv:1607.03367</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1607.03367">pdf</a>, <a href="https://arxiv.org/format/1607.03367">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-016-4388-y">10.1140/epjc/s10052-016-4388-y <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Improved EDELWEISS-III sensitivity for low-mass WIMPs using a profile likelihood approach </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=EDELWEISS+Collaboration"> EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Hehn%2C+L">L. Hehn</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bl%C3%BCmer%2C+J">J. Bl眉mer</a>, <a href="/search/?searchtype=author&amp;query=de+Boissi%C3%A8re%2C+T">T. de Boissi猫re</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Foerster%2C+N">N. Foerster</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Heuermann%2C+G">G. Heuermann</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a>, <a href="/search/?searchtype=author&amp;query=Juillard%2C+A">A. Juillard</a> , et al. (24 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1607.03367v2-abstract-short" style="display: inline;"> We report on a dark matter search for a Weakly Interacting Massive Particle (WIMP) in the mass range $m_蠂\in [4, 30]\,\mathrm{GeV}/c^2$ with the EDELWEISS-III experiment. A 2D profile likelihood analysis is performed on data from eight selected detectors with the lowest energy thresholds leading to a combined fiducial exposure of 496 kg-days. External backgrounds from $纬$- and $尾$-radiation, recoi&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1607.03367v2-abstract-full').style.display = 'inline'; document.getElementById('1607.03367v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1607.03367v2-abstract-full" style="display: none;"> We report on a dark matter search for a Weakly Interacting Massive Particle (WIMP) in the mass range $m_蠂\in [4, 30]\,\mathrm{GeV}/c^2$ with the EDELWEISS-III experiment. A 2D profile likelihood analysis is performed on data from eight selected detectors with the lowest energy thresholds leading to a combined fiducial exposure of 496 kg-days. External backgrounds from $纬$- and $尾$-radiation, recoils from $^{206}$Pb and neutrons as well as detector intrinsic backgrounds were modelled from data outside the region of interest and constrained in the analysis. The basic data selection and most of the background models are the same as those used in a previously published analysis based on Boosted Decision Trees (BDT). For the likelihood approach applied in the analysis presented here, a larger signal efficiency and a subtraction of the expected background lead to a higher sensitivity, especially for the lowest WIMP masses probed. No statistically significant signal was found and upper limits on the spin-independent WIMP-nucleon scattering cross section can be set with a hypothesis test based on the profile likelihood test statistics. The 90% C.L. exclusion limit set for WIMPs with $m_蠂= 4\,\mathrm{GeV/}c^2$ is $1.6 \times 10^{-39}\,\mathrm{cm^2}$, which is an improvement of a factor of seven with respect to the BDT-based analysis. For WIMP masses above $15\,\mathrm{GeV/}c^2$ the exclusion limits found with both analyses are in good agreement. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1607.03367v2-abstract-full').style.display = 'none'; document.getElementById('1607.03367v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 20 September, 2016; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 12 July, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2016. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">11 pages, 6 figures, 2 tables (updated to accepted version)</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> EPJ C (2016) 76:548 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1606.08097">arXiv:1606.08097</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1606.08097">pdf</a>, <a href="https://arxiv.org/format/1606.08097">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Methods for Astrophysics">astro-ph.IM</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/11/10/P10008">10.1088/1748-0221/11/10/P10008 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Signals induced by charge-trapping in EDELWEISS FID detectors: analytical modeling and applications </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=The+EDELWEISS+Collaboration"> The EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bl%C3%BCmer%2C+J">J. Bl眉mer</a>, <a href="/search/?searchtype=author&amp;query=de+Boissi%C3%A8re%2C+T">T. de Boissi猫re</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Foerster%2C+N">N. Foerster</a>, <a href="/search/?searchtype=author&amp;query=Fourches%2C+N">N. Fourches</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a>, <a href="/search/?searchtype=author&amp;query=Giuliani%2C+A">A. Giuliani</a>, <a href="/search/?searchtype=author&amp;query=Gros%2C+M">M. Gros</a>, <a href="/search/?searchtype=author&amp;query=Hehn%2C+L">L. Hehn</a>, <a href="/search/?searchtype=author&amp;query=Heuermann%2C+G">G. Heuermann</a>, <a href="/search/?searchtype=author&amp;query=De+J%C3%A9sus%2C+M">M. De J茅sus</a>, <a href="/search/?searchtype=author&amp;query=Jin%2C+Y">Y. Jin</a> , et al. (25 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1606.08097v2-abstract-short" style="display: inline;"> The EDELWEISS-III direct dark matter search experiment uses cryogenic HP-Ge detectors Fully covered with Inter-Digitized electrodes (FID). They are operated at low fields ($&lt;1\;\mathrm{V/cm}$), and as a consequence charge-carrier trapping significantly affects both the ionization and heat energy measurements. This paper describes an analytical model of the signals induced by trapped charges in FID&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1606.08097v2-abstract-full').style.display = 'inline'; document.getElementById('1606.08097v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1606.08097v2-abstract-full" style="display: none;"> The EDELWEISS-III direct dark matter search experiment uses cryogenic HP-Ge detectors Fully covered with Inter-Digitized electrodes (FID). They are operated at low fields ($&lt;1\;\mathrm{V/cm}$), and as a consequence charge-carrier trapping significantly affects both the ionization and heat energy measurements. This paper describes an analytical model of the signals induced by trapped charges in FID detectors based on the Shockley-Ramo theorem. It is used to demonstrate that veto electrodes, initially designed for the sole purpose of surface event rejection, can be used to provide a sensitivity to the depth of the energy deposits, characterize the trapping in the crystals, perform heat and ionization energy corrections and improve the ionization baseline resolutions. These procedures are applied successfully to actual data. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1606.08097v2-abstract-full').style.display = 'none'; document.getElementById('1606.08097v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 29 June, 2016; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 June, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2016. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">17 pages 12 figures, submitted to JINST, author list updated</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1603.05120">arXiv:1603.05120</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1603.05120">pdf</a>, <a href="https://arxiv.org/format/1603.05120">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1475-7516/2016/05/019">10.1088/1475-7516/2016/05/019 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Constraints on low-mass WIMPs from the EDELWEISS-III dark matter search </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=EDELWEISS+Collaboration"> EDELWEISS Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Armengaud%2C+E">E. Armengaud</a>, <a href="/search/?searchtype=author&amp;query=Arnaud%2C+Q">Q. Arnaud</a>, <a href="/search/?searchtype=author&amp;query=Augier%2C+C">C. Augier</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Beno%C3%AEt%2C+A">A. Beno卯t</a>, <a href="/search/?searchtype=author&amp;query=Berg%C3%A9%2C+L">L. Berg茅</a>, <a href="/search/?searchtype=author&amp;query=Bergmann%2C+T">T. Bergmann</a>, <a href="/search/?searchtype=author&amp;query=Billard%2C+J">J. Billard</a>, <a href="/search/?searchtype=author&amp;query=Bl%C3%BCmer%2C+J">J. Bl眉mer</a>, <a href="/search/?searchtype=author&amp;query=de+Boissi%C3%A8re%2C+T">T. de Boissi猫re</a>, <a href="/search/?searchtype=author&amp;query=Bres%2C+G">G. Bres</a>, <a href="/search/?searchtype=author&amp;query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/?searchtype=author&amp;query=Brudanin%2C+V">V. Brudanin</a>, <a href="/search/?searchtype=author&amp;query=Camus%2C+P">P. Camus</a>, <a href="/search/?searchtype=author&amp;query=Cazes%2C+A">A. Cazes</a>, <a href="/search/?searchtype=author&amp;query=Chapellier%2C+M">M. Chapellier</a>, <a href="/search/?searchtype=author&amp;query=Charlieux%2C+F">F. Charlieux</a>, <a href="/search/?searchtype=author&amp;query=Dumoulin%2C+L">L. Dumoulin</a>, <a href="/search/?searchtype=author&amp;query=Eitel%2C+K">K. Eitel</a>, <a href="/search/?searchtype=author&amp;query=Filosofov%2C+D">D. Filosofov</a>, <a href="/search/?searchtype=author&amp;query=Foerster%2C+N">N. Foerster</a>, <a href="/search/?searchtype=author&amp;query=Fourches%2C+N">N. Fourches</a>, <a href="/search/?searchtype=author&amp;query=Garde%2C+G">G. Garde</a>, <a href="/search/?searchtype=author&amp;query=Gascon%2C+J">J. Gascon</a> , et al. (42 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1603.05120v2-abstract-short" style="display: inline;"> We present the results of a search for elastic scattering from galactic dark matter in the form of Weakly Interacting Massive Particles (WIMPs) in the 4-30 GeV/$c^2$ mass range. We make use of a 582 kg-day fiducial exposure from an array of 800 g Germanium bolometers equipped with a set of interleaved electrodes with full surface coverage. We searched specifically for $\sim 2.5-20$ keV nuclear rec&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1603.05120v2-abstract-full').style.display = 'inline'; document.getElementById('1603.05120v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1603.05120v2-abstract-full" style="display: none;"> We present the results of a search for elastic scattering from galactic dark matter in the form of Weakly Interacting Massive Particles (WIMPs) in the 4-30 GeV/$c^2$ mass range. We make use of a 582 kg-day fiducial exposure from an array of 800 g Germanium bolometers equipped with a set of interleaved electrodes with full surface coverage. We searched specifically for $\sim 2.5-20$ keV nuclear recoils inside the detector fiducial volume. As an illustration the number of observed events in the search for 5 (resp. 20) GeV/$c^2$ WIMPs are 9 (resp. 4), compared to an expected background of 6.1 (resp. 1.4). A 90% CL limit of $4.3\times 10^{-40}$ cm$^2$ (resp. $9.4\times 10^{-44}$ cm$^2$) is set on the spin-independent WIMP-nucleon scattering cross-section for 5 (resp. 20) GeV/$c^2$ WIMPs. This result represents a 41-fold improvement with respect to the previous EDELWEISS-II low-mass WIMP search for 7 GeV/$c^2$ WIMPs. The derived constraint is in tension with hints of WIMP signals from some recent experiments, thus confirming results obtained with different detection techniques. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1603.05120v2-abstract-full').style.display = 'none'; document.getElementById('1603.05120v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 May, 2016; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 March, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2016. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Matches published version</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal 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