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class="tag is-small is-grey 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="Computation">stat.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/10.1051/0004-6361/202450617">10.1051/0004-6361/202450617 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Euclid preparation. LIII. LensMC, weak lensing cosmic shear measurement with forward modelling and Markov Chain Monte Carlo sampling </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Euclid+Collaboration"> Euclid Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Congedo%2C+G">G. Congedo</a>, <a href="/search/physics?searchtype=author&amp;query=Miller%2C+L">L. Miller</a>, <a href="/search/physics?searchtype=author&amp;query=Taylor%2C+A+N">A. N. Taylor</a>, <a href="/search/physics?searchtype=author&amp;query=Cross%2C+N">N. Cross</a>, <a href="/search/physics?searchtype=author&amp;query=Duncan%2C+C+A+J">C. A. J. Duncan</a>, <a href="/search/physics?searchtype=author&amp;query=Kitching%2C+T">T. Kitching</a>, <a href="/search/physics?searchtype=author&amp;query=Martinet%2C+N">N. Martinet</a>, <a href="/search/physics?searchtype=author&amp;query=Matthew%2C+S">S. Matthew</a>, <a href="/search/physics?searchtype=author&amp;query=Schrabback%2C+T">T. Schrabback</a>, <a href="/search/physics?searchtype=author&amp;query=Tewes%2C+M">M. Tewes</a>, <a href="/search/physics?searchtype=author&amp;query=Welikala%2C+N">N. Welikala</a>, <a href="/search/physics?searchtype=author&amp;query=Aghanim%2C+N">N. Aghanim</a>, <a href="/search/physics?searchtype=author&amp;query=Amara%2C+A">A. Amara</a>, <a href="/search/physics?searchtype=author&amp;query=Andreon%2C+S">S. Andreon</a>, <a href="/search/physics?searchtype=author&amp;query=Auricchio%2C+N">N. Auricchio</a>, <a href="/search/physics?searchtype=author&amp;query=Baldi%2C+M">M. Baldi</a>, <a href="/search/physics?searchtype=author&amp;query=Bardelli%2C+S">S. Bardelli</a>, <a href="/search/physics?searchtype=author&amp;query=Bender%2C+R">R. Bender</a>, <a href="/search/physics?searchtype=author&amp;query=Bodendorf%2C+C">C. Bodendorf</a>, <a href="/search/physics?searchtype=author&amp;query=Bonino%2C+D">D. Bonino</a>, <a href="/search/physics?searchtype=author&amp;query=Branchini%2C+E">E. Branchini</a>, <a href="/search/physics?searchtype=author&amp;query=Brescia%2C+M">M. Brescia</a>, <a href="/search/physics?searchtype=author&amp;query=Brinchmann%2C+J">J. Brinchmann</a>, <a href="/search/physics?searchtype=author&amp;query=Camera%2C+S">S. Camera</a> , et al. (217 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="2405.00669v3-abstract-short" style="display: inline;"> LensMC is a weak lensing shear measurement method developed for Euclid and Stage-IV surveys. It is based on forward modelling in order to deal with convolution by a point spread function (PSF) with comparable size to many galaxies; sampling the posterior distribution of galaxy parameters via Markov Chain Monte Carlo; and marginalisation over nuisance parameters for each of the 1.5 billion galaxies&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2405.00669v3-abstract-full').style.display = 'inline'; document.getElementById('2405.00669v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2405.00669v3-abstract-full" style="display: none;"> LensMC is a weak lensing shear measurement method developed for Euclid and Stage-IV surveys. It is based on forward modelling in order to deal with convolution by a point spread function (PSF) with comparable size to many galaxies; sampling the posterior distribution of galaxy parameters via Markov Chain Monte Carlo; and marginalisation over nuisance parameters for each of the 1.5 billion galaxies observed by Euclid. We quantified the scientific performance through high-fidelity images based on the Euclid Flagship simulations and emulation of the Euclid VIS images; realistic clustering with a mean surface number density of 250 arcmin$^{-2}$ ($I_{\rm E}&lt;29.5$) for galaxies, and 6 arcmin$^{-2}$ ($I_{\rm E}&lt;26$) for stars; and a diffraction-limited chromatic PSF with a full width at half maximum of $0.^{\!\prime\prime}2$ and spatial variation across the field of view. LensMC measured objects with a density of 90 arcmin$^{-2}$ ($I_{\rm E}&lt;26.5$) in 4500 deg$^2$. The total shear bias was broken down into measurement (our main focus here) and selection effects (which will be addressed elsewhere). We found measurement multiplicative and additive biases of $m_1=(-3.6\pm0.2)\times10^{-3}$, $m_2=(-4.3\pm0.2)\times10^{-3}$, $c_1=(-1.78\pm0.03)\times10^{-4}$, $c_2=(0.09\pm0.03)\times10^{-4}$; a large detection bias with a multiplicative component of $1.2\times10^{-2}$ and an additive component of $-3\times10^{-4}$; and a measurement PSF leakage of $伪_1=(-9\pm3)\times10^{-4}$ and $伪_2=(2\pm3)\times10^{-4}$. When model bias is suppressed, the obtained measurement biases are close to Euclid requirement and largely dominated by undetected faint galaxies ($-5\times10^{-3}$). Although significant, model bias will be straightforward to calibrate given the weak sensitivity. LensMC is publicly available at https://gitlab.com/gcongedo/LensMC <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2405.00669v3-abstract-full').style.display = 'none'; document.getElementById('2405.00669v3-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 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 1 May, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">Appearing on A&amp;A. 28 pages, 18 figures, and 2 tables</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> A&amp;A 691, A319 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2311.18647">arXiv:2311.18647</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2311.18647">pdf</a>, <a href="https://arxiv.org/format/2311.18647">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="Cosmology and Nongalactic Astrophysics">astro-ph.CO</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/10.1088/1748-0221/19/05/P05057">10.1088/1748-0221/19/05/P05057 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Long-term temporal stability of the DarkSide-50 dark matter detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Collaboration%2C+T+D">The DarkSide-50 Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Biery%2C+K">K. Biery</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Bussino%2C+S">S. Bussino</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cadoni%2C+M">M. Cadoni</a>, <a href="/search/physics?searchtype=author&amp;query=Calaprice%2C+F">F. Calaprice</a>, <a href="/search/physics?searchtype=author&amp;query=Caminata%2C+A">A. Caminata</a>, <a href="/search/physics?searchtype=author&amp;query=Campos%2C+M+D">M. D. Campos</a>, <a href="/search/physics?searchtype=author&amp;query=Canci%2C+N">N. Canci</a>, <a href="/search/physics?searchtype=author&amp;query=Caravati%2C+M">M. Caravati</a>, <a href="/search/physics?searchtype=author&amp;query=Cargioli%2C+N">N. Cargioli</a>, <a href="/search/physics?searchtype=author&amp;query=Cariello%2C+M">M. Cariello</a>, <a href="/search/physics?searchtype=author&amp;query=Carlini%2C+M">M. Carlini</a>, <a href="/search/physics?searchtype=author&amp;query=Cataudella%2C+V">V. Cataudella</a> , et al. (121 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="2311.18647v3-abstract-short" style="display: inline;"> The stability of a dark matter detector on the timescale of a few years is a key requirement due to the large exposure needed to achieve a competitive sensitivity. It is especially crucial to enable the detector to potentially detect any annual event rate modulation, an expected dark matter signature. In this work, we present the performance history of the DarkSide-50 dual-phase argon time project&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.18647v3-abstract-full').style.display = 'inline'; document.getElementById('2311.18647v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2311.18647v3-abstract-full" style="display: none;"> The stability of a dark matter detector on the timescale of a few years is a key requirement due to the large exposure needed to achieve a competitive sensitivity. It is especially crucial to enable the detector to potentially detect any annual event rate modulation, an expected dark matter signature. In this work, we present the performance history of the DarkSide-50 dual-phase argon time projection chamber over its almost three-year low-radioactivity argon run. In particular, we focus on the electroluminescence signal that enables sensitivity to sub-keV energy depositions. The stability of the electroluminescence yield is found to be better than 0.5%. Finally, we show the temporal evolution of the observed event rate around the sub-keV region being consistent to the background prediction. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.18647v3-abstract-full').style.display = 'none'; document.getElementById('2311.18647v3-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 May, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 30 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">13 pages, 5 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JINST 19 P05057 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2308.15518">arXiv:2308.15518</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2308.15518">pdf</a>, <a href="https://arxiv.org/format/2308.15518">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="Earth and Planetary Astrophysics">astro-ph.EP</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Popular Physics">physics.pop-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/10.26206/gvmj-sn65">10.26206/gvmj-sn65 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Data-Driven Approaches to Searches for the Technosignatures of Advanced Civilizations </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Lazio%2C+T+J+W">T. Joseph W. Lazio</a>, <a href="/search/physics?searchtype=author&amp;query=Djorgovski%2C+S+G">S. G. Djorgovski</a>, <a href="/search/physics?searchtype=author&amp;query=Howard%2C+A">Andrew Howard</a>, <a href="/search/physics?searchtype=author&amp;query=Cutler%2C+C">Curt Cutler</a>, <a href="/search/physics?searchtype=author&amp;query=Sheikh%2C+S+Z">Sofia Z. Sheikh</a>, <a href="/search/physics?searchtype=author&amp;query=Cavuoti%2C+S">Stefano Cavuoti</a>, <a href="/search/physics?searchtype=author&amp;query=Herzing%2C+D">Denise Herzing</a>, <a href="/search/physics?searchtype=author&amp;query=Wagstaff%2C+K">Kiri Wagstaff</a>, <a href="/search/physics?searchtype=author&amp;query=Wright%2C+J+T">Jason T. Wright</a>, <a href="/search/physics?searchtype=author&amp;query=Gajjar%2C+V">Vishal Gajjar</a>, <a href="/search/physics?searchtype=author&amp;query=Hand%2C+K">Kevin Hand</a>, <a href="/search/physics?searchtype=author&amp;query=Rebbapragada%2C+U">Umaa Rebbapragada</a>, <a href="/search/physics?searchtype=author&amp;query=Allen%2C+B">Bruce Allen</a>, <a href="/search/physics?searchtype=author&amp;query=Cartmill%2C+E">Erica Cartmill</a>, <a href="/search/physics?searchtype=author&amp;query=Foster%2C+J">Jacob Foster</a>, <a href="/search/physics?searchtype=author&amp;query=Gelino%2C+D">Dawn Gelino</a>, <a href="/search/physics?searchtype=author&amp;query=Graham%2C+M+J">Matthew J. Graham</a>, <a href="/search/physics?searchtype=author&amp;query=Longo%2C+G">Giuseppe Longo</a>, <a href="/search/physics?searchtype=author&amp;query=Mahabal%2C+A+A">Ashish A. Mahabal</a>, <a href="/search/physics?searchtype=author&amp;query=Pachter%2C+L">Lior Pachter</a>, <a href="/search/physics?searchtype=author&amp;query=Ravi%2C+V">Vikram Ravi</a>, <a href="/search/physics?searchtype=author&amp;query=Sussman%2C+G">Gerald Sussman</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="2308.15518v1-abstract-short" style="display: inline;"> Humanity has wondered whether we are alone for millennia. The discovery of life elsewhere in the Universe, particularly intelligent life, would have profound effects, comparable to those of recognizing that the Earth is not the center of the Universe and that humans evolved from previous species. There has been rapid growth in the fields of extrasolar planets and data-driven astronomy. In a relati&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2308.15518v1-abstract-full').style.display = 'inline'; document.getElementById('2308.15518v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2308.15518v1-abstract-full" style="display: none;"> Humanity has wondered whether we are alone for millennia. The discovery of life elsewhere in the Universe, particularly intelligent life, would have profound effects, comparable to those of recognizing that the Earth is not the center of the Universe and that humans evolved from previous species. There has been rapid growth in the fields of extrasolar planets and data-driven astronomy. In a relatively short interval, we have seen a change from knowing of no extrasolar planets to now knowing more potentially habitable extrasolar planets than there are planets in the Solar System. In approximately the same interval, astronomy has transitioned to a field in which sky surveys can generate 1 PB or more of data. The Data-Driven Approaches to Searches for the Technosignatures of Advanced Civilizations_ study at the W. M. Keck Institute for Space Studies was intended to revisit searches for evidence of alien technologies in light of these developments. Data-driven searches, being able to process volumes of data much greater than a human could, and in a reproducible manner, can identify *anomalies* that could be clues to the presence of technosignatures. A key outcome of this workshop was that technosignature searches should be conducted in a manner consistent with Freeman Dyson&#39;s &#34;First Law of SETI Investigations,&#34; namely &#34;every search for alien civilizations should be planned to give interesting results even when no aliens are discovered.&#34; This approach to technosignatures is commensurate with NASA&#39;s approach to biosignatures in that no single observation or measurement can be taken as providing full certainty for the detection of life. Areas of particular promise identified during the workshop were (*) Data Mining of Large Sky Surveys, (*) All-Sky Survey at Far-Infrared Wavelengths, (*) Surveys with Radio Astronomical Interferometers, and (*) Artifacts in the Solar System. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2308.15518v1-abstract-full').style.display = 'none'; document.getElementById('2308.15518v1-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 August, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 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">Final Report prepared for the W. M. Keck Institute for Space Studies (KISS), http://kiss.caltech.edu/workshops/technosignatures/technosignatures.html ; eds. Lazio, Djorgovski, Howard, &amp; Cutler; The study leads gratefully acknowledge the outstanding support of Michele Judd, KISS Executive Director, and her dedicated staff, who made the study experience invigorating and enormously productive</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2307.15454">arXiv:2307.15454</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2307.15454">pdf</a>, <a href="https://arxiv.org/format/2307.15454">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"> Directionality of nuclear recoils in a liquid argon time projection chamber </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Collaboration%2C+T+D">The DarkSide-20k Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+I">I. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Albergo%2C+S">S. Albergo</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P">P. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Corona%2C+M+A">M. Atzori Corona</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Avetisov%2C+I+C">I. Ch. Avetisov</a>, <a href="/search/physics?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Balmforth%2C+Z">Z. Balmforth</a>, <a href="/search/physics?searchtype=author&amp;query=Barrado-Olmedo%2C+A">A. Barrado-Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Barrillon%2C+P">P. Barrillon</a>, <a href="/search/physics?searchtype=author&amp;query=Basco%2C+A">A. Basco</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Boulay%2C+M+G">M. G. Boulay</a>, <a href="/search/physics?searchtype=author&amp;query=Busto%2C+J">J. Busto</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a> , et al. (243 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="2307.15454v1-abstract-short" style="display: inline;"> The direct search for dark matter in the form of weakly interacting massive particles (WIMP) is performed by detecting nuclear recoils (NR) produced in a target material from the WIMP elastic scattering. A promising experimental strategy for direct dark matter search employs argon dual-phase time projection chambers (TPC). One of the advantages of the TPC is the capability to detect both the scint&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2307.15454v1-abstract-full').style.display = 'inline'; document.getElementById('2307.15454v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2307.15454v1-abstract-full" style="display: none;"> The direct search for dark matter in the form of weakly interacting massive particles (WIMP) is performed by detecting nuclear recoils (NR) produced in a target material from the WIMP elastic scattering. A promising experimental strategy for direct dark matter search employs argon dual-phase time projection chambers (TPC). One of the advantages of the TPC is the capability to detect both the scintillation and charge signals produced by NRs. Furthermore, the existence of a drift electric field in the TPC breaks the rotational symmetry: the angle between the drift field and the momentum of the recoiling nucleus can potentially affect the charge recombination probability in liquid argon and then the relative balance between the two signal channels. This fact could make the detector sensitive to the directionality of the WIMP-induced signal, enabling unmistakable annual and daily modulation signatures for future searches aiming for discovery. The Recoil Directionality (ReD) experiment was designed to probe for such directional sensitivity. The TPC of ReD was irradiated with neutrons at the INFN Laboratori Nazionali del Sud, and data were taken with 72 keV NRs of known recoil directions. The direction-dependent liquid argon charge recombination model by Cataudella et al. was adopted and a likelihood statistical analysis was performed, which gave no indications of significant dependence of the detector response to the recoil direction. The aspect ratio R of the initial ionization cloud is estimated to be 1.037 +/- 0.027 and the upper limit is R &lt; 1.072 with 90% confidence level <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2307.15454v1-abstract-full').style.display = 'none'; document.getElementById('2307.15454v1-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> 28 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">20 pages, 10 figures, submitted to Eur. Phys. J. C</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 84:24 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2302.14639">arXiv:2302.14639</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2302.14639">pdf</a>, <a href="https://arxiv.org/format/2302.14639">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/10.1140/epjc/s10052-023-11678-6">10.1140/epjc/s10052-023-11678-6 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Precision Measurement of the Specific Activity of $^{39}$Ar in Atmospheric Argon with the DEAP-3600 Detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Adhikari%2C+P">P. Adhikari</a>, <a href="/search/physics?searchtype=author&amp;query=Ajaj%2C+R">R. Ajaj</a>, <a href="/search/physics?searchtype=author&amp;query=Alp%C3%ADzar-Venegas%2C+M">M. Alp铆zar-Venegas</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P+-">P. -A. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Anstey%2C+J">J. Anstey</a>, <a href="/search/physics?searchtype=author&amp;query=Araujo%2C+G+R">G. R. Araujo</a>, <a href="/search/physics?searchtype=author&amp;query=Auty%2C+D+J">D. J. Auty</a>, <a href="/search/physics?searchtype=author&amp;query=Baldwin%2C+M">M. Baldwin</a>, <a href="/search/physics?searchtype=author&amp;query=Batygov%2C+M">M. Batygov</a>, <a href="/search/physics?searchtype=author&amp;query=Beltran%2C+B">B. Beltran</a>, <a href="/search/physics?searchtype=author&amp;query=Benmansour%2C+H">H. Benmansour</a>, <a href="/search/physics?searchtype=author&amp;query=Bina%2C+C+E">C. E. Bina</a>, <a href="/search/physics?searchtype=author&amp;query=Bonatt%2C+J">J. Bonatt</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W">W. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Boulay%2C+M+G">M. G. Boulay</a>, <a href="/search/physics?searchtype=author&amp;query=Broerman%2C+B">B. Broerman</a>, <a href="/search/physics?searchtype=author&amp;query=Bueno%2C+J+F">J. F. Bueno</a>, <a href="/search/physics?searchtype=author&amp;query=Burghardt%2C+P+M">P. M. Burghardt</a>, <a href="/search/physics?searchtype=author&amp;query=Butcher%2C+A">A. Butcher</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cai%2C+B">B. Cai</a>, <a href="/search/physics?searchtype=author&amp;query=C%C3%A1rdenas-Montes%2C+M">M. C谩rdenas-Montes</a>, <a href="/search/physics?searchtype=author&amp;query=Cavuoti%2C+S">S. Cavuoti</a>, <a href="/search/physics?searchtype=author&amp;query=Chen%2C+M">M. Chen</a>, <a href="/search/physics?searchtype=author&amp;query=Chen%2C+Y">Y. Chen</a> , et al. (125 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="2302.14639v2-abstract-short" style="display: inline;"> The specific activity of the beta decay of $^{39}$Ar in atmospheric argon is measured using the DEAP-3600 detector. DEAP-3600, located 2 km underground at SNOLAB, uses a total of (3269 $\pm$ 24) kg of liquid argon distilled from the atmosphere to search for dark matter. This detector with very low background uses pulseshape discrimination to differentiate between nuclear recoils and electron recoi&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2302.14639v2-abstract-full').style.display = 'inline'; document.getElementById('2302.14639v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2302.14639v2-abstract-full" style="display: none;"> The specific activity of the beta decay of $^{39}$Ar in atmospheric argon is measured using the DEAP-3600 detector. DEAP-3600, located 2 km underground at SNOLAB, uses a total of (3269 $\pm$ 24) kg of liquid argon distilled from the atmosphere to search for dark matter. This detector with very low background uses pulseshape discrimination to differentiate between nuclear recoils and electron recoils and is well-suited to measure the decay of $^{39}$Ar. With 167 live-days of data, the measured specific activity at the time of atmospheric extraction is [0.964 $\pm$ 0.001 (stat) $\pm$ 0.024 (sys)] Bq/kg$_{\rm atmAr}$ which is consistent with results from other experiments. A cross-check analysis using different event selection criteria provides a consistent result. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2302.14639v2-abstract-full').style.display = 'none'; document.getElementById('2302.14639v2-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 October, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 27 February, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur. Phys. J. C 83, 642 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2209.01177">arXiv:2209.01177</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2209.01177">pdf</a>, <a href="https://arxiv.org/format/2209.01177">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/PhysRevD.107.112006">10.1103/PhysRevD.107.112006 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Sensitivity projections for a dual-phase argon TPC optimized for light dark matter searches through the ionization channel </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Ahmad%2C+I">I. Ahmad</a>, <a href="/search/physics?searchtype=author&amp;query=Albergo%2C+S">S. Albergo</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P">P. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Corona%2C+M+A">M. Atzori Corona</a>, <a href="/search/physics?searchtype=author&amp;query=Auty%2C+D+J">D. J. Auty</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Avetisov%2C+I+C">I. Ch. Avetisov</a>, <a href="/search/physics?searchtype=author&amp;query=Avetisov%2C+R+I">R. I. Avetisov</a>, <a href="/search/physics?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Balmforth%2C+Z">Z. Balmforth</a>, <a href="/search/physics?searchtype=author&amp;query=Barbarian%2C+V">V. Barbarian</a>, <a href="/search/physics?searchtype=author&amp;query=Olmedo%2C+A+B">A. Barrado Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Barrillon%2C+P">P. Barrillon</a>, <a href="/search/physics?searchtype=author&amp;query=Basco%2C+A">A. Basco</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Berzin%2C+E">E. Berzin</a>, <a href="/search/physics?searchtype=author&amp;query=Bondar%2C+A">A. Bondar</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Borisova%2C+E">E. Borisova</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a> , et al. (274 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="2209.01177v2-abstract-short" style="display: inline;"> Dark matter lighter than 10 GeV/c$^2$ encompasses a promising range of candidates. A conceptual design for a new detector, DarkSide-LowMass, is presented, based on the DarkSide-50 detector and progress toward DarkSide-20k, optimized for a low-threshold electron-counting measurement. Sensitivity to light dark matter is explored for various potential energy thresholds and background rates. These stu&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2209.01177v2-abstract-full').style.display = 'inline'; document.getElementById('2209.01177v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2209.01177v2-abstract-full" style="display: none;"> Dark matter lighter than 10 GeV/c$^2$ encompasses a promising range of candidates. A conceptual design for a new detector, DarkSide-LowMass, is presented, based on the DarkSide-50 detector and progress toward DarkSide-20k, optimized for a low-threshold electron-counting measurement. Sensitivity to light dark matter is explored for various potential energy thresholds and background rates. These studies show that DarkSide-LowMass can achieve sensitivity to light dark matter down to the solar neutrino floor for GeV-scale masses and significant sensitivity down to 10 MeV/c$^2$ considering the Migdal effect or interactions with electrons. Requirements for optimizing the detector&#39;s sensitivity are explored, as are potential sensitivity gains from modeling and mitigating spurious electron backgrounds that may dominate the signal at the lowest energies. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2209.01177v2-abstract-full').style.display = 'none'; document.getElementById('2209.01177v2-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 June, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 2 September, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 107, 112006 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2107.08087">arXiv:2107.08087</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2107.08087">pdf</a>, <a href="https://arxiv.org/format/2107.08087">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> <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/PhysRevD.104.082005">10.1103/PhysRevD.104.082005 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Calibration of the liquid argon ionization response to low energy electronic and nuclear recoils with DarkSide-50 </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=The+DarkSide+collaboration"> The DarkSide collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Biery%2C+K">K. Biery</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Bussino%2C+S">S. Bussino</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cadoni%2C+M">M. Cadoni</a>, <a href="/search/physics?searchtype=author&amp;query=Calaprice%2C+F">F. Calaprice</a>, <a href="/search/physics?searchtype=author&amp;query=Caminata%2C+A">A. Caminata</a>, <a href="/search/physics?searchtype=author&amp;query=Canci%2C+N">N. Canci</a>, <a href="/search/physics?searchtype=author&amp;query=Caravati%2C+M">M. Caravati</a>, <a href="/search/physics?searchtype=author&amp;query=Cariello%2C+M">M. Cariello</a>, <a href="/search/physics?searchtype=author&amp;query=Carlini%2C+M">M. Carlini</a>, <a href="/search/physics?searchtype=author&amp;query=Carpinelli%2C+M">M. Carpinelli</a>, <a href="/search/physics?searchtype=author&amp;query=Catalanotti%2C+S">S. Catalanotti</a>, <a href="/search/physics?searchtype=author&amp;query=Cataudella%2C+V">V. Cataudella</a>, <a href="/search/physics?searchtype=author&amp;query=Cavalcante%2C+P">P. Cavalcante</a> , et al. (114 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="2107.08087v2-abstract-short" style="display: inline;"> DarkSide-50 has demonstrated the high potential of dual-phase liquid argon time projection chambers in exploring interactions of WIMPs in the GeV/c$^2$ mass range. The technique, based on the detection of the ionization signal amplified via electroluminescence in the gas phase, allows to explore recoil energies down to the sub-keV range. We report here on the DarkSide-50 measurement of the ionizat&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.08087v2-abstract-full').style.display = 'inline'; document.getElementById('2107.08087v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2107.08087v2-abstract-full" style="display: none;"> DarkSide-50 has demonstrated the high potential of dual-phase liquid argon time projection chambers in exploring interactions of WIMPs in the GeV/c$^2$ mass range. The technique, based on the detection of the ionization signal amplified via electroluminescence in the gas phase, allows to explore recoil energies down to the sub-keV range. We report here on the DarkSide-50 measurement of the ionization yield of electronic recoils down to $\sim$180~eV$_{er}$, exploiting $^{37}$Ar and $^{39}$Ar decays, and extrapolated to a few ionization electrons with the Thomas-Imel box model. Moreover, we present a model-dependent determination of the ionization response to nuclear recoils down to $\sim$500~eV$_{nr}$, the lowest ever achieved in liquid argon, using \textit{in situ} neutron calibration sources and external datasets from neutron beam experiments. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.08087v2-abstract-full').style.display = 'none'; document.getElementById('2107.08087v2-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 September, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 July, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 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">11 pages, 12 figures, 1 table</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 104, 082005 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2107.08015">arXiv:2107.08015</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2107.08015">pdf</a>, <a href="https://arxiv.org/format/2107.08015">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"> A study of events with photoelectric emission in the DarkSide-50 liquid argon Time Projection Chamber </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Collaboration%2C+T+D">The DarkSide-50 Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Biery%2C+K">K. Biery</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Bussino%2C+S">S. Bussino</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cadoni%2C+M">M. Cadoni</a>, <a href="/search/physics?searchtype=author&amp;query=Calaprice%2C+F">F. Calaprice</a>, <a href="/search/physics?searchtype=author&amp;query=Caminata%2C+A">A. Caminata</a>, <a href="/search/physics?searchtype=author&amp;query=Canci%2C+N">N. Canci</a>, <a href="/search/physics?searchtype=author&amp;query=Caravati%2C+M">M. Caravati</a>, <a href="/search/physics?searchtype=author&amp;query=Cariello%2C+M">M. Cariello</a>, <a href="/search/physics?searchtype=author&amp;query=Carlini%2C+M">M. Carlini</a>, <a href="/search/physics?searchtype=author&amp;query=Carpinelli%2C+M">M. Carpinelli</a>, <a href="/search/physics?searchtype=author&amp;query=Catalanotti%2C+S">S. Catalanotti</a>, <a href="/search/physics?searchtype=author&amp;query=Cataudella%2C+V">V. Cataudella</a> , et al. (114 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="2107.08015v2-abstract-short" style="display: inline;"> Finding unequivocal evidence of dark matter interactions in a particle detector is a major objective of physics research. Liquid argon time projection chambers offer a path to probe Weakly Interacting Massive Particles scattering cross sections on nucleus down to the so-called neutrino floor, in a mass range from few GeV&#39;s to hundredths of TeV&#39;s. Based on the successful operation of the DarkSide-5&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.08015v2-abstract-full').style.display = 'inline'; document.getElementById('2107.08015v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2107.08015v2-abstract-full" style="display: none;"> Finding unequivocal evidence of dark matter interactions in a particle detector is a major objective of physics research. Liquid argon time projection chambers offer a path to probe Weakly Interacting Massive Particles scattering cross sections on nucleus down to the so-called neutrino floor, in a mass range from few GeV&#39;s to hundredths of TeV&#39;s. Based on the successful operation of the DarkSide-50 detector at LNGS, a new and more sensitive experiment, DarkSide-20k, has been designed and is now under construction. A thorough understanding of the DarkSide-50 detector response and, therefore, of all kind of observed events, is essential for an optimal design of the new experiment. In this paper, we report on a particular set of events, which were not used for dark matter searches. Namely, standard two-pulse scintillation-ionization signals accompanied by a small amplitude third pulse, originating from single or few electrons, in a time window of less than a maximum drift time. We compare our findings to those of a recent paper of the LUX Collaboration (D.S.Akerib et al. Phys.Rev.D 102, 092004). Indeed, both experiments observe events related to photoionization of the cathode. From the measured rate of these events, we estimate for the first time the quantum efficiency of the tetraphenyl butadiene deposited on the DarkSide-50 cathode at wavelengths around 128 nm, in liquid argon. Also, both experiments observe events likely related to photoionization of impurities in the liquid. The probability of photoelectron emission per unit length turns out to be one order of magnitude smaller in DarkSide-50 than in LUX. This result, together with the much larger measured electron lifetime, coherently hints toward a lower concentration of contaminants in DarkSide-50 than in LUX. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.08015v2-abstract-full').style.display = 'none'; document.getElementById('2107.08015v2-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, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 July, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 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">10 pages, 8 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/2103.12202">arXiv:2103.12202</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2103.12202">pdf</a>, <a href="https://arxiv.org/format/2103.12202">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/10.1140/epjc/s10052-021-09514-w">10.1140/epjc/s10052-021-09514-w <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Pulseshape discrimination against low-energy Ar-39 beta decays in liquid argon with 4.5 tonne-years of DEAP-3600 data </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=The+DEAP+Collaboration"> The DEAP Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Adhikari%2C+P">P. Adhikari</a>, <a href="/search/physics?searchtype=author&amp;query=Ajaj%2C+R">R. Ajaj</a>, <a href="/search/physics?searchtype=author&amp;query=Alp%C3%ADzar-Venegas%2C+M">M. Alp铆zar-Venegas</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P+-">P. -A. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Auty%2C+D+J">D. J. Auty</a>, <a href="/search/physics?searchtype=author&amp;query=Batygov%2C+M">M. Batygov</a>, <a href="/search/physics?searchtype=author&amp;query=Beltran%2C+B">B. Beltran</a>, <a href="/search/physics?searchtype=author&amp;query=Benmansour%2C+H">H. Benmansour</a>, <a href="/search/physics?searchtype=author&amp;query=Bina%2C+C+E">C. E. Bina</a>, <a href="/search/physics?searchtype=author&amp;query=Bonatt%2C+J">J. Bonatt</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W">W. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Boulay%2C+M+G">M. G. Boulay</a>, <a href="/search/physics?searchtype=author&amp;query=Broerman%2C+B">B. Broerman</a>, <a href="/search/physics?searchtype=author&amp;query=Bueno%2C+J+F">J. F. Bueno</a>, <a href="/search/physics?searchtype=author&amp;query=Burghardt%2C+P+M">P. M. Burghardt</a>, <a href="/search/physics?searchtype=author&amp;query=Butcher%2C+A">A. Butcher</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cai%2C+B">B. Cai</a>, <a href="/search/physics?searchtype=author&amp;query=C%C3%A1rdenas-Montes%2C+M">M. C谩rdenas-Montes</a>, <a href="/search/physics?searchtype=author&amp;query=Cavuoti%2C+S">S. Cavuoti</a>, <a href="/search/physics?searchtype=author&amp;query=Chen%2C+M">M. Chen</a>, <a href="/search/physics?searchtype=author&amp;query=Chen%2C+Y">Y. Chen</a>, <a href="/search/physics?searchtype=author&amp;query=Cleveland%2C+B+T">B. T. Cleveland</a>, <a href="/search/physics?searchtype=author&amp;query=Corning%2C+J+M">J. M. Corning</a> , et al. (104 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="2103.12202v2-abstract-short" style="display: inline;"> The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $^{39}$Ar beta decays and is suppressed using pulseshape discrimination (PSD). We use two types of PSD algorithm: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window ar&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2103.12202v2-abstract-full').style.display = 'inline'; document.getElementById('2103.12202v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2103.12202v2-abstract-full" style="display: none;"> The DEAP-3600 detector searches for the scintillation signal from dark matter particles scattering on a 3.3 tonne liquid argon target. The largest background comes from $^{39}$Ar beta decays and is suppressed using pulseshape discrimination (PSD). We use two types of PSD algorithm: the prompt-fraction, which considers the fraction of the scintillation signal in a narrow and a wide time window around the event peak, and the log-likelihood-ratio, which compares the observed photon arrival times to a signal and a background model. We furthermore use two algorithms to determine the number of photons detected at a given time: (1) simply dividing the charge of each PMT pulse by the charge of a single photoelectron, and (2) a likelihood analysis that considers the probability to detect a certain number of photons at a given time, based on a model for the scintillation pulseshape and for afterpulsing in the light detectors. The prompt-fraction performs approximately as well as the log-likelihood-ratio PSD algorithm if the photon detection times are not biased by detector effects. We explain this result using a model for the information carried by scintillation photons as a function of the time when they are detected. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2103.12202v2-abstract-full').style.display = 'none'; document.getElementById('2103.12202v2-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 April, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 22 March, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 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">14 pages, 9 figures</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 81, 823 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2101.08686">arXiv:2101.08686</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2101.08686">pdf</a>, <a href="https://arxiv.org/format/2101.08686">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/10.1140/epjc/s10052-021-09121-9">10.1140/epjc/s10052-021-09121-9 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Separating $^{39}$Ar from $^{40}$Ar by cryogenic distillation with Aria for dark matter searches </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=DarkSide+Collaboration"> DarkSide Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albergo%2C+S">S. Albergo</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alici%2C+A">A. Alici</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P">P. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Arba%2C+M">M. Arba</a>, <a href="/search/physics?searchtype=author&amp;query=Arpaia%2C+P">P. Arpaia</a>, <a href="/search/physics?searchtype=author&amp;query=Arcelli%2C+S">S. Arcelli</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Avetissov%2C+I+C">I. Ch. Avetissov</a>, <a href="/search/physics?searchtype=author&amp;query=Avetisov%2C+R+I">R. I. Avetisov</a>, <a href="/search/physics?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Balmforth%2C+Z">Z. Balmforth</a>, <a href="/search/physics?searchtype=author&amp;query=Barbarian%2C+V">V. Barbarian</a>, <a href="/search/physics?searchtype=author&amp;query=Olmedo%2C+A+B">A. Barrado Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Barrillon%2C+P">P. Barrillon</a>, <a href="/search/physics?searchtype=author&amp;query=Basco%2C+A">A. Basco</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Bondar%2C+A">A. Bondar</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Borisova%2C+E">E. Borisova</a> , et al. (287 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="2101.08686v2-abstract-short" style="display: inline;"> The Aria project consists of a plant, hosting a 350 m cryogenic isotopic distillation column, the tallest ever built, which is currently in the installation phase in a mine shaft at Carbosulcis S.p.A., Nuraxi-Figus (SU), Italy. Aria is one of the pillars of the argon dark-matter search experimental program, lead by the Global Argon Dark Matter Collaboration. Aria was designed to reduce the isotopi&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2101.08686v2-abstract-full').style.display = 'inline'; document.getElementById('2101.08686v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2101.08686v2-abstract-full" style="display: none;"> The Aria project consists of a plant, hosting a 350 m cryogenic isotopic distillation column, the tallest ever built, which is currently in the installation phase in a mine shaft at Carbosulcis S.p.A., Nuraxi-Figus (SU), Italy. Aria is one of the pillars of the argon dark-matter search experimental program, lead by the Global Argon Dark Matter Collaboration. Aria was designed to reduce the isotopic abundance of $^{39}$Ar, a $尾$-emitter of cosmogenic origin, whose activity poses background and pile-up concerns in the detectors, in the argon used for the dark-matter searches, the so-called Underground Argon (UAr). In this paper, we discuss the requirements, design, construction, tests, and projected performance of the plant for the isotopic cryogenic distillation of argon. We also present the successful results of isotopic cryogenic distillation of nitrogen with a prototype plant, operating the column at total reflux. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2101.08686v2-abstract-full').style.display = 'none'; document.getElementById('2101.08686v2-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 January, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 21 January, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur.Phys.J.C 81 (2021) 4, 359 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.07819">arXiv:2011.07819</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.07819">pdf</a>, <a href="https://arxiv.org/format/2011.07819">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 Astrophysical Phenomena">astro-ph.HE</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/10.1088/1475-7516/2021/03/043">10.1088/1475-7516/2021/03/043 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Sensitivity of future liquid argon dark matter search experiments to core-collapse supernova neutrinos </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albergo%2C+S">S. Albergo</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alici%2C+A">A. Alici</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P">P. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Arcelli%2C+S">S. Arcelli</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Avetissov%2C+I+C">I. Ch. Avetissov</a>, <a href="/search/physics?searchtype=author&amp;query=Avetisov%2C+R+I">R. I. Avetisov</a>, <a href="/search/physics?searchtype=author&amp;query=Azzolini%2C+O">O. Azzolini</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Balmforth%2C+Z">Z. Balmforth</a>, <a href="/search/physics?searchtype=author&amp;query=Barbarian%2C+V">V. Barbarian</a>, <a href="/search/physics?searchtype=author&amp;query=Olmedo%2C+A+B">A. Barrado Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Barrillon%2C+P">P. Barrillon</a>, <a href="/search/physics?searchtype=author&amp;query=Basco%2C+A">A. Basco</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Bondar%2C+A">A. Bondar</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Borisova%2C+E">E. Borisova</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Boulay%2C+M+G">M. G. Boulay</a>, <a href="/search/physics?searchtype=author&amp;query=Buccino%2C+G">G. Buccino</a> , et al. (251 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="2011.07819v2-abstract-short" style="display: inline;"> Future liquid-argon DarkSide-20k and ARGO detectors, designed for direct dark matter search, will be sensitive also to core-collapse supernova neutrinos, via coherent elastic neutrino-nucleus scattering. This interaction channel is flavor-insensitive with a high-cross section, enabling for a high-statistics neutrino detection with target masses of $\sim$50~t and $\sim$360~t for DarkSide-20k and AR&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.07819v2-abstract-full').style.display = 'inline'; document.getElementById('2011.07819v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.07819v2-abstract-full" style="display: none;"> Future liquid-argon DarkSide-20k and ARGO detectors, designed for direct dark matter search, will be sensitive also to core-collapse supernova neutrinos, via coherent elastic neutrino-nucleus scattering. This interaction channel is flavor-insensitive with a high-cross section, enabling for a high-statistics neutrino detection with target masses of $\sim$50~t and $\sim$360~t for DarkSide-20k and ARGO, respectively. Thanks to the low-energy threshold of $\sim$0.5~keV$_{nr}$ achievable by exploiting the ionization channel, DarkSide-20k and ARGO have the potential to discover supernova bursts throughout our galaxy and up to the Small Magellanic Cloud, respectively, assuming a 11-M$_{\odot}$ progenitor star. We report also on the sensitivity to the neutronization burst, whose electron neutrino flux is suppressed by oscillations when detected via charged current and elastic scattering. Finally, the accuracies in the reconstruction of the average and total neutrino energy in the different phases of the supernova burst, as well as its time profile, are also discussed, taking into account the expected background and the detector response. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.07819v2-abstract-full').style.display = 'none'; document.getElementById('2011.07819v2-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 December, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 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">21 pages, 8 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JCAP 03 (2021) 043 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2004.02024">arXiv:2004.02024</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2004.02024">pdf</a>, <a href="https://arxiv.org/format/2004.02024">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> <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/10.1140/epjc/s10052-020-08801-2">10.1140/epjc/s10052-020-08801-2 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> SiPM-matrix readout of two-phase argon detectors using electroluminescence in the visible and near infrared range </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=The+DarkSide+collaboration"> The DarkSide collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Aalseth%2C+C+E">C. E. Aalseth</a>, <a href="/search/physics?searchtype=author&amp;query=Abdelhakim%2C+S">S. Abdelhakim</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Ajaj%2C+R">R. Ajaj</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alici%2C+A">A. Alici</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P">P. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Ameli%2C+F">F. Ameli</a>, <a href="/search/physics?searchtype=author&amp;query=Anstey%2C+J">J. Anstey</a>, <a href="/search/physics?searchtype=author&amp;query=Antonioli%2C+P">P. Antonioli</a>, <a href="/search/physics?searchtype=author&amp;query=Arba%2C+M">M. Arba</a>, <a href="/search/physics?searchtype=author&amp;query=Arcelli%2C+S">S. Arcelli</a>, <a href="/search/physics?searchtype=author&amp;query=Ardito%2C+R">R. Ardito</a>, <a href="/search/physics?searchtype=author&amp;query=Arnquist%2C+I+J">I. J. Arnquist</a>, <a href="/search/physics?searchtype=author&amp;query=Arpaia%2C+P">P. Arpaia</a>, <a href="/search/physics?searchtype=author&amp;query=Asner%2C+D+M">D. M. Asner</a>, <a href="/search/physics?searchtype=author&amp;query=Asunskis%2C+A">A. Asunskis</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Barbaryan%2C+V">V. Barbaryan</a>, <a href="/search/physics?searchtype=author&amp;query=Olmedo%2C+A+B">A. Barrado Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a> , et al. (290 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="2004.02024v2-abstract-short" style="display: inline;"> Proportional electroluminescence (EL) in noble gases is used in two-phase detectors for dark matter searches to record (in the gas phase) the ionization signal induced by particle scattering in the liquid phase. The &#34;standard&#34; EL mechanism is considered to be due to noble gas excimer emission in the vacuum ultraviolet (VUV). In addition, there are two alternative mechanisms, producing light in the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.02024v2-abstract-full').style.display = 'inline'; document.getElementById('2004.02024v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2004.02024v2-abstract-full" style="display: none;"> Proportional electroluminescence (EL) in noble gases is used in two-phase detectors for dark matter searches to record (in the gas phase) the ionization signal induced by particle scattering in the liquid phase. The &#34;standard&#34; EL mechanism is considered to be due to noble gas excimer emission in the vacuum ultraviolet (VUV). In addition, there are two alternative mechanisms, producing light in the visible and near infrared (NIR) ranges. The first is due to bremsstrahlung of electrons scattered on neutral atoms (&#34;neutral bremsstrahlung&#34;, NBrS). The second, responsible for electron avalanche scintillation in the NIR at higher electric fields, is due to transitions between excited atomic states. In this work, we have for the first time demonstrated two alternative techniques of the optical readout of two-phase argon detectors, in the visible and NIR range, using a silicon photomultiplier matrix and electroluminescence due to either neutral bremsstrahlung or avalanche scintillation. The amplitude yield and position resolution were measured for these readout techniques, which allowed to assess the detection threshold for electron and nuclear recoils in two-phase argon detectors for dark matter searches. To the best of our knowledge, this is the first practical application of the NBrS effect in detection science. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.02024v2-abstract-full').style.display = 'none'; document.getElementById('2004.02024v2-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 February, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 4 April, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 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">26 pages, 22 figures, 3 tables</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 (2021) 81: 153 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2002.07794">arXiv:2002.07794</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2002.07794">pdf</a>, <a href="https://arxiv.org/format/2002.07794">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="High Energy Physics - Phenomenology">hep-ph</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"> Effective field theory interactions for liquid argon target in DarkSide-50 experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Collaboration%2C+T+D">The DarkSide-50 Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Biery%2C+K">K. Biery</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonfini%2C+G">G. Bonfini</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Bussino%2C+S">S. Bussino</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cadoni%2C+M">M. Cadoni</a>, <a href="/search/physics?searchtype=author&amp;query=Calaprice%2C+F">F. Calaprice</a>, <a href="/search/physics?searchtype=author&amp;query=Caminata%2C+A">A. Caminata</a>, <a href="/search/physics?searchtype=author&amp;query=Canci%2C+N">N. Canci</a>, <a href="/search/physics?searchtype=author&amp;query=Candela%2C+A">A. Candela</a>, <a href="/search/physics?searchtype=author&amp;query=Caravati%2C+M">M. Caravati</a>, <a href="/search/physics?searchtype=author&amp;query=Cariello%2C+M">M. Cariello</a>, <a href="/search/physics?searchtype=author&amp;query=Carlini%2C+M">M. Carlini</a>, <a href="/search/physics?searchtype=author&amp;query=Carpinelli%2C+M">M. Carpinelli</a> , et al. (143 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="2002.07794v1-abstract-short" style="display: inline;"> We reanalize data collected with the DarkSide-50 experiment and recently used to set limits on the spin-independent interaction rate of weakly interacting massive particles (WIMPs) on argon nuclei with an effective field theory framework. The dataset corresponds to a total (16660 $\pm$ 270) kg d exposure using a target of low-radioactivity argon extracted from underground sources. We obtain upper&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2002.07794v1-abstract-full').style.display = 'inline'; document.getElementById('2002.07794v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2002.07794v1-abstract-full" style="display: none;"> We reanalize data collected with the DarkSide-50 experiment and recently used to set limits on the spin-independent interaction rate of weakly interacting massive particles (WIMPs) on argon nuclei with an effective field theory framework. The dataset corresponds to a total (16660 $\pm$ 270) kg d exposure using a target of low-radioactivity argon extracted from underground sources. We obtain upper limits on the effective couplings of the 12 leading operators in the nonrelativistic systematic expansion. For each effective coupling we set constraints on WIMP-nucleon cross sections, setting upper limits between $2.4 \times 10^{-45} \, \mathrm{cm}^2$ and $2.3 \times 10^{-42} \, \mathrm{cm}^2$ (8.9 $\times 10^{-45} \, \mathrm{cm}^2$ and 6.0 $\times 10^{-42} \, \mathrm{cm}^2$) for WIMPs of mass of 100 $\mathrm{GeV/c^2}$ (1000 $\mathrm{GeV/c^2}$) at 90\% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2002.07794v1-abstract-full').style.display = 'none'; document.getElementById('2002.07794v1-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 February, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 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">Accepted by PRD</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2001.09855">arXiv:2001.09855</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2001.09855">pdf</a>, <a href="https://arxiv.org/format/2001.09855">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/10.1140/epjc/s10052-020-7789-x">10.1140/epjc/s10052-020-7789-x <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The liquid-argon scintillation pulseshape in DEAP-3600 </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=The+DEAP+collaboration"> The DEAP collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Adhikari%2C+P">P. Adhikari</a>, <a href="/search/physics?searchtype=author&amp;query=Ajaj%2C+R">R. Ajaj</a>, <a href="/search/physics?searchtype=author&amp;query=Batygov%2C+G+R+A+M">G. R. Araujoand M. Batygov</a>, <a href="/search/physics?searchtype=author&amp;query=Beltran%2C+B">B. Beltran</a>, <a href="/search/physics?searchtype=author&amp;query=Bina%2C+C+E">C. E. Bina</a>, <a href="/search/physics?searchtype=author&amp;query=Boulay%2C+M+G">M. G. Boulay</a>, <a href="/search/physics?searchtype=author&amp;query=Broerman%2C+B">B. Broerman</a>, <a href="/search/physics?searchtype=author&amp;query=Bueno%2C+J+F">J. F. Bueno</a>, <a href="/search/physics?searchtype=author&amp;query=Butcher%2C+A">A. Butcher</a>, <a href="/search/physics?searchtype=author&amp;query=Cai%2C+B">B. Cai</a>, <a href="/search/physics?searchtype=author&amp;query=C%C3%A1rdenas-Montes%2C+M">M. C谩rdenas-Montes</a>, <a href="/search/physics?searchtype=author&amp;query=Cavuoti%2C+S">S. Cavuoti</a>, <a href="/search/physics?searchtype=author&amp;query=Chen%2C+Y">Y. Chen</a>, <a href="/search/physics?searchtype=author&amp;query=Cleveland%2C+B+T">B. T. Cleveland</a>, <a href="/search/physics?searchtype=author&amp;query=Corning%2C+J+M">J. M. Corning</a>, <a href="/search/physics?searchtype=author&amp;query=Dering%2C+S+J+D+K">S. J. Daughertyand K. Dering</a>, <a href="/search/physics?searchtype=author&amp;query=Doria%2C+L">L. Doria</a>, <a href="/search/physics?searchtype=author&amp;query=Dunford%2C+F+A+D+a">F. A. Duncan andM. Dunford</a>, <a href="/search/physics?searchtype=author&amp;query=Erlandson%2C+A">A. Erlandson</a>, <a href="/search/physics?searchtype=author&amp;query=Fatemighomi%2C+N">N. Fatemighomi</a>, <a href="/search/physics?searchtype=author&amp;query=Fiorillo%2C+G">G. Fiorillo</a>, <a href="/search/physics?searchtype=author&amp;query=Flower%2C+A">A. Flower</a>, <a href="/search/physics?searchtype=author&amp;query=Ford%2C+R+J">R. J. Ford</a>, <a href="/search/physics?searchtype=author&amp;query=Gagnon%2C+R">R. Gagnon</a> , et al. (76 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="2001.09855v2-abstract-short" style="display: inline;"> DEAP-3600 is a liquid-argon scintillation detector looking for dark matter. Scintillation events in the liquid argon (LAr) are registered by 255 photomultiplier tubes (PMTs), and pulseshape discrimination (PSD) is used to suppress electromagnetic background events. The excellent PSD performance of LAr makes it a viable target for dark matter searches, and the LAr scintillation pulseshape discussed&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2001.09855v2-abstract-full').style.display = 'inline'; document.getElementById('2001.09855v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2001.09855v2-abstract-full" style="display: none;"> DEAP-3600 is a liquid-argon scintillation detector looking for dark matter. Scintillation events in the liquid argon (LAr) are registered by 255 photomultiplier tubes (PMTs), and pulseshape discrimination (PSD) is used to suppress electromagnetic background events. The excellent PSD performance of LAr makes it a viable target for dark matter searches, and the LAr scintillation pulseshape discussed here is the basis of PSD. The observed pulseshape is a combination of LAr scintillation physics with detector effects. We present a model for the pulseshape of electromagnetic background events in the energy region of interest for dark matter searches. The model is composed of a) LAr scintillation physics, including the so-called intermediate component, b) the time response of the TPB wavelength shifter, including delayed TPB emission at $\mathcal O$(ms) time-scales, and c) PMT response. TPB is the wavelength shifter of choice in most LAr detectors. We find that approximately 10\% of the intensity of the wavelength-shifted light is in a long-lived state of TPB. This causes light from an event to spill into subsequent events to an extent not usually accounted for in the design and data analysis of LAr-based detectors. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2001.09855v2-abstract-full').style.display = 'none'; document.getElementById('2001.09855v2-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 June, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 27 January, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur. Phys. J. C 80, 303 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2001.08106">arXiv:2001.08106</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2001.08106">pdf</a>, <a href="https://arxiv.org/format/2001.08106">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/10.1088/1748-0221/15/02/P02024">10.1088/1748-0221/15/02/P02024 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Design and construction of a new detector to measure ultra-low radioactive-isotope contamination of argon </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=The+DarkSide+Collaboration"> The DarkSide Collaboration</a>, <a href="/search/physics?searchtype=author&amp;query=Aalseth%2C+C+E">C. E. Aalseth</a>, <a href="/search/physics?searchtype=author&amp;query=Abdelhakim%2C+S">S. Abdelhakim</a>, <a href="/search/physics?searchtype=author&amp;query=Acerbi%2C+F">F. Acerbi</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Ajaj%2C+R">R. Ajaj</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alici%2C+A">A. Alici</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Amaudruz%2C+P">P. Amaudruz</a>, <a href="/search/physics?searchtype=author&amp;query=Ameli%2C+F">F. Ameli</a>, <a href="/search/physics?searchtype=author&amp;query=Anstey%2C+J">J. Anstey</a>, <a href="/search/physics?searchtype=author&amp;query=Antonioli%2C+P">P. Antonioli</a>, <a href="/search/physics?searchtype=author&amp;query=Arba%2C+M">M. Arba</a>, <a href="/search/physics?searchtype=author&amp;query=Arcelli%2C+S">S. Arcelli</a>, <a href="/search/physics?searchtype=author&amp;query=Ardito%2C+R">R. Ardito</a>, <a href="/search/physics?searchtype=author&amp;query=Arnquist%2C+I+J">I. J. Arnquist</a>, <a href="/search/physics?searchtype=author&amp;query=Arpaia%2C+P">P. Arpaia</a>, <a href="/search/physics?searchtype=author&amp;query=Asner%2C+D+M">D. M. Asner</a>, <a href="/search/physics?searchtype=author&amp;query=Asunskis%2C+A">A. Asunskis</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Olmedo%2C+A+B">A. Barrado Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a> , et al. (306 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="2001.08106v1-abstract-short" style="display: inline;"> Large liquid argon detectors offer one of the best avenues for the detection of galactic weakly interacting massive particles (WIMPs) via their scattering on atomic nuclei. The liquid argon target allows exquisite discrimination between nuclear and electron recoil signals via pulse-shape discrimination of the scintillation signals. Atmospheric argon (AAr), however, has a naturally occurring radioa&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2001.08106v1-abstract-full').style.display = 'inline'; document.getElementById('2001.08106v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2001.08106v1-abstract-full" style="display: none;"> Large liquid argon detectors offer one of the best avenues for the detection of galactic weakly interacting massive particles (WIMPs) via their scattering on atomic nuclei. The liquid argon target allows exquisite discrimination between nuclear and electron recoil signals via pulse-shape discrimination of the scintillation signals. Atmospheric argon (AAr), however, has a naturally occurring radioactive isotope, $^{39}$Ar, a $尾$ emitter of cosmogenic origin. For large detectors, the atmospheric $^{39}$Ar activity poses pile-up concerns. The use of argon extracted from underground wells, deprived of $^{39}$Ar, is key to the physics potential of these experiments. The DarkSide-20k dark matter search experiment will operate a dual-phase time projection chamber with 50 tonnes of radio-pure underground argon (UAr), that was shown to be depleted of $^{39}$Ar with respect to AAr by a factor larger than 1400. Assessing the $^{39}$Ar content of the UAr during extraction is crucial for the success of DarkSide-20k, as well as for future experiments of the Global Argon Dark Matter Collaboration (GADMC). This will be carried out by the DArT in ArDM experiment, a small chamber made with extremely radio-pure materials that will be placed at the centre of the ArDM detector, in the Canfranc Underground Laboratory (LSC) in Spain. The ArDM LAr volume acts as an active veto for background radioactivity, mostly $纬$-rays from the ArDM detector materials and the surrounding rock. This article describes the DArT in ArDM project, including the chamber design and construction, and reviews the background required to achieve the expected performance of the detector. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2001.08106v1-abstract-full').style.display = 'none'; document.getElementById('2001.08106v1-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 January, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 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">13 pages, 8 figures. Corresponding author: E. S谩nchez Garc铆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/1907.09332">arXiv:1907.09332</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1907.09332">pdf</a>, <a href="https://arxiv.org/format/1907.09332">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/10.1088/1748-0221/14/11/P11018">10.1088/1748-0221/14/11/P11018 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of the ion fraction and mobility of $^{218}$Po produced in $^{222}$Rn decays in liquid argon </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Biery%2C+K">K. Biery</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonfini%2C+G">G. Bonfini</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W+M">W. M. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Bussino%2C+S">S. Bussino</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cadoni%2C+M">M. Cadoni</a>, <a href="/search/physics?searchtype=author&amp;query=Calaprice%2C+F">F. Calaprice</a>, <a href="/search/physics?searchtype=author&amp;query=Caminata%2C+A">A. Caminata</a>, <a href="/search/physics?searchtype=author&amp;query=Canci%2C+N">N. Canci</a>, <a href="/search/physics?searchtype=author&amp;query=Candela%2C+A">A. Candela</a>, <a href="/search/physics?searchtype=author&amp;query=Caravati%2C+M">M. Caravati</a>, <a href="/search/physics?searchtype=author&amp;query=Cariello%2C+M">M. Cariello</a>, <a href="/search/physics?searchtype=author&amp;query=Carlini%2C+M">M. Carlini</a>, <a href="/search/physics?searchtype=author&amp;query=Carpinelli%2C+M">M. Carpinelli</a>, <a href="/search/physics?searchtype=author&amp;query=Catalanotti%2C+S">S. Catalanotti</a>, <a href="/search/physics?searchtype=author&amp;query=Cataudella%2C+V">V. Cataudella</a> , et al. (141 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="1907.09332v2-abstract-short" style="display: inline;"> We report measurements of the charged daughter fraction of $^{218}$Po as a result of the $^{222}$Rn alpha decay, and the mobility of $^{218}$Po$^+$ ions, using radon-polonium coincidences from the $^{238}$U chain identified in 532 live-days of DarkSide-50 WIMP-search data. The fraction of $^{218}$Po that is charged is found to be 0.37$\pm$0.03 and the mobility of $^{218}$Po$^+$ is (8.6$\pm$0.1)&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1907.09332v2-abstract-full').style.display = 'inline'; document.getElementById('1907.09332v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1907.09332v2-abstract-full" style="display: none;"> We report measurements of the charged daughter fraction of $^{218}$Po as a result of the $^{222}$Rn alpha decay, and the mobility of $^{218}$Po$^+$ ions, using radon-polonium coincidences from the $^{238}$U chain identified in 532 live-days of DarkSide-50 WIMP-search data. The fraction of $^{218}$Po that is charged is found to be 0.37$\pm$0.03 and the mobility of $^{218}$Po$^+$ is (8.6$\pm$0.1)$\times$10$^{-4}$$\frac{\text{cm}^2}{\text{Vs}}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1907.09332v2-abstract-full').style.display = 'none'; document.getElementById('1907.09332v2-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> 28 October, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 22 July, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JINST 14 P11018 (2019) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1802.01427">arXiv:1802.01427</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1802.01427">pdf</a>, <a href="https://arxiv.org/format/1802.01427">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.2018.06.077">10.1016/j.nima.2018.06.077 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Electroluminescence pulse shape and electron diffusion in liquid argon measured in a dual-phase TPC </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Asner%2C+D+M">D. M. Asner</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M+P">M. P. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Baldin%2C+B">B. Baldin</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Biery%2C+K">K. Biery</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bonfini%2C+G">G. Bonfini</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W">W. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bossa%2C+M">M. Bossa</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a>, <a href="/search/physics?searchtype=author&amp;query=Budano%2C+F">F. Budano</a>, <a href="/search/physics?searchtype=author&amp;query=Bussino%2C+S">S. Bussino</a>, <a href="/search/physics?searchtype=author&amp;query=Cadeddu%2C+M">M. Cadeddu</a>, <a href="/search/physics?searchtype=author&amp;query=Cadoni%2C+M">M. Cadoni</a>, <a href="/search/physics?searchtype=author&amp;query=Calaprice%2C+F">F. Calaprice</a>, <a href="/search/physics?searchtype=author&amp;query=Caminata%2C+A">A. Caminata</a>, <a href="/search/physics?searchtype=author&amp;query=Canci%2C+N">N. Canci</a>, <a href="/search/physics?searchtype=author&amp;query=Candela%2C+A">A. Candela</a>, <a href="/search/physics?searchtype=author&amp;query=Caravati%2C+M">M. Caravati</a>, <a href="/search/physics?searchtype=author&amp;query=Cariello%2C+M">M. Cariello</a> , et al. (141 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="1802.01427v2-abstract-short" style="display: inline;"> We report the measurement of the longitudinal diffusion constant in liquid argon with the DarkSide-50 dual-phase time projection chamber. The measurement is performed at drift electric fields of 100 V/cm, 150 V/cm, and 200 V/cm using high statistics $^{39}$Ar decays from atmospheric argon. We derive an expression to describe the pulse shape of the electroluminescence signal (S2) in dual-phase TPCs&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1802.01427v2-abstract-full').style.display = 'inline'; document.getElementById('1802.01427v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1802.01427v2-abstract-full" style="display: none;"> We report the measurement of the longitudinal diffusion constant in liquid argon with the DarkSide-50 dual-phase time projection chamber. The measurement is performed at drift electric fields of 100 V/cm, 150 V/cm, and 200 V/cm using high statistics $^{39}$Ar decays from atmospheric argon. We derive an expression to describe the pulse shape of the electroluminescence signal (S2) in dual-phase TPCs. The derived S2 pulse shape is fit to events from the uppermost portion of the TPC in order to characterize the radial dependence of the signal. The results are provided as inputs to the measurement of the longitudinal diffusion constant DL, which we find to be (4.12 $\pm$ 0.04) cm$^2$/s for a selection of 140keV electron recoil events in 200V/cm drift field and 2.8kV/cm extraction field. To study the systematics of our measurement we examine datasets of varying event energy, field strength, and detector volume yielding a weighted average value for the diffusion constant of (4.09 $\pm$ 0.09) cm$^2$ /s. The measured longitudinal diffusion constant is observed to have an energy dependence, and within the studied energy range the result is systematically lower than other results in the literature. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1802.01427v2-abstract-full').style.display = 'none'; document.getElementById('1802.01427v2-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 July, 2018; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 5 February, 2018; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2018. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1707.08145">arXiv:1707.08145</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1707.08145">pdf</a>, <a href="https://arxiv.org/format/1707.08145">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/10.1140/epjp/i2018-11973-4">10.1140/epjp/i2018-11973-4 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> DarkSide-20k: A 20 Tonne Two-Phase LAr TPC for Direct Dark Matter Detection at LNGS </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Aalseth%2C+C+E">C. E. Aalseth</a>, <a href="/search/physics?searchtype=author&amp;query=Acerbi%2C+F">F. Acerbi</a>, <a href="/search/physics?searchtype=author&amp;query=Agnes%2C+P">P. Agnes</a>, <a href="/search/physics?searchtype=author&amp;query=Albuquerque%2C+I+F+M">I. F. M. Albuquerque</a>, <a href="/search/physics?searchtype=author&amp;query=Alexander%2C+T">T. Alexander</a>, <a href="/search/physics?searchtype=author&amp;query=Alici%2C+A">A. Alici</a>, <a href="/search/physics?searchtype=author&amp;query=Alton%2C+A+K">A. K. Alton</a>, <a href="/search/physics?searchtype=author&amp;query=Antonioli%2C+P">P. Antonioli</a>, <a href="/search/physics?searchtype=author&amp;query=Arcelli%2C+S">S. Arcelli</a>, <a href="/search/physics?searchtype=author&amp;query=Ardito%2C+R">R. Ardito</a>, <a href="/search/physics?searchtype=author&amp;query=Arnquist%2C+I+J">I. J. Arnquist</a>, <a href="/search/physics?searchtype=author&amp;query=Asner%2C+D+M">D. M. Asner</a>, <a href="/search/physics?searchtype=author&amp;query=Ave%2C+M">M. Ave</a>, <a href="/search/physics?searchtype=author&amp;query=Back%2C+H+O">H. O. Back</a>, <a href="/search/physics?searchtype=author&amp;query=Olmedo%2C+A+I+B">A. I. Barrado Olmedo</a>, <a href="/search/physics?searchtype=author&amp;query=Batignani%2C+G">G. Batignani</a>, <a href="/search/physics?searchtype=author&amp;query=Bertoldo%2C+E">E. Bertoldo</a>, <a href="/search/physics?searchtype=author&amp;query=Bettarini%2C+S">S. Bettarini</a>, <a href="/search/physics?searchtype=author&amp;query=Bisogni%2C+M+G">M. G. Bisogni</a>, <a href="/search/physics?searchtype=author&amp;query=Bocci%2C+V">V. Bocci</a>, <a href="/search/physics?searchtype=author&amp;query=Bondar%2C+A">A. Bondar</a>, <a href="/search/physics?searchtype=author&amp;query=Bonfini%2C+G">G. Bonfini</a>, <a href="/search/physics?searchtype=author&amp;query=Bonivento%2C+W">W. Bonivento</a>, <a href="/search/physics?searchtype=author&amp;query=Bossa%2C+M">M. Bossa</a>, <a href="/search/physics?searchtype=author&amp;query=Bottino%2C+B">B. Bottino</a> , et al. (260 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="1707.08145v1-abstract-short" style="display: inline;"> Building on the successful experience in operating the DarkSide-50 detector, the DarkSide Collaboration is going to construct DarkSide-20k, a direct WIMP search detector using a two-phase Liquid Argon Time Projection Chamber (LArTPC) with an active (fiducial) mass of 23 t (20 t). The DarkSide-20k LArTPC will be deployed within a shield/veto with a spherical Liquid Scintillator Veto (LSV) inside a&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1707.08145v1-abstract-full').style.display = 'inline'; document.getElementById('1707.08145v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1707.08145v1-abstract-full" style="display: none;"> Building on the successful experience in operating the DarkSide-50 detector, the DarkSide Collaboration is going to construct DarkSide-20k, a direct WIMP search detector using a two-phase Liquid Argon Time Projection Chamber (LArTPC) with an active (fiducial) mass of 23 t (20 t). The DarkSide-20k LArTPC will be deployed within a shield/veto with a spherical Liquid Scintillator Veto (LSV) inside a cylindrical Water Cherenkov Veto (WCV). Operation of DarkSide-50 demonstrated a major reduction in the dominant $^{39}$Ar background when using argon extracted from an underground source, before applying pulse shape analysis. Data from DarkSide-50, in combination with MC simulation and analytical modeling, shows that a rejection factor for discrimination between electron and nuclear recoils of $\gt3\times10^9$ is achievable. This, along with the use of the veto system, is the key to unlocking the path to large LArTPC detector masses, while maintaining an &#34;instrumental background-free&#34; experiment, an experiment in which less than 0.1 events (other than $谓$-induced nuclear recoils) is expected to occur within the WIMP search region during the planned exposure. DarkSide-20k will have ultra-low backgrounds than can be measured in situ. This will give sensitivity to WIMP-nucleon cross sections of $1.2\times10^{-47}$ cm$^2$ ($1.1\times10^{-46}$ cm$^2$) for WIMPs of $1$ TeV$/c^2$ ($10$ TeV$/c^2$) mass, to be achieved during a 5 yr run producing an exposure of 100 t yr free from any instrumental background. DarkSide-20k could then extend its operation to a decade, increasing the exposure to 200 t yr, reaching a sensitivity of $7.4\times10^{-48}$ cm$^2$ ($6.9\times10^{-47}$ cm$^2$) for WIMPs of $1$ TeV$/c^2$ ($10$ TeV$/c^2$) mass. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1707.08145v1-abstract-full').style.display = 'none'; document.getElementById('1707.08145v1-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 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">Report number:</span> FERMILAB-PUB-17-298-PPD </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Aalseth, C.E., Acerbi, F., Agnes, P. et al. Eur. Phys. J. Plus (2018) 133: 131 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1501.03915">arXiv:1501.03915</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1501.03915">pdf</a>, <a href="https://arxiv.org/ps/1501.03915">ps</a>, <a href="https://arxiv.org/format/1501.03915">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Medical Physics">physics.med-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Computer Vision and Pattern Recognition">cs.CV</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Machine Learning">cs.LG</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/10.1155/2015/814104">10.1155/2015/814104 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Feature Selection based on Machine Learning in MRIs for Hippocampal Segmentation </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/physics?searchtype=author&amp;query=Tangaro%2C+S">Sabina Tangaro</a>, <a href="/search/physics?searchtype=author&amp;query=Amoroso%2C+N">Nicola Amoroso</a>, <a href="/search/physics?searchtype=author&amp;query=Brescia%2C+M">Massimo Brescia</a>, <a href="/search/physics?searchtype=author&amp;query=Cavuoti%2C+S">Stefano Cavuoti</a>, <a href="/search/physics?searchtype=author&amp;query=Chincarini%2C+A">Andrea Chincarini</a>, <a href="/search/physics?searchtype=author&amp;query=Errico%2C+R">Rosangela Errico</a>, <a href="/search/physics?searchtype=author&amp;query=Inglese%2C+P">Paolo Inglese</a>, <a href="/search/physics?searchtype=author&amp;query=Longo%2C+G">Giuseppe Longo</a>, <a href="/search/physics?searchtype=author&amp;query=Maglietta%2C+R">Rosalia Maglietta</a>, <a href="/search/physics?searchtype=author&amp;query=Tateo%2C+A">Andrea Tateo</a>, <a href="/search/physics?searchtype=author&amp;query=Riccio%2C+G">Giuseppe Riccio</a>, <a href="/search/physics?searchtype=author&amp;query=Bellotti%2C+R">Roberto Bellotti</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="1501.03915v1-abstract-short" style="display: inline;"> Neurodegenerative diseases are frequently associated with structural changes in the brain. Magnetic Resonance Imaging (MRI) scans can show these variations and therefore be used as a supportive feature for a number of neurodegenerative diseases. The hippocampus has been known to be a biomarker for Alzheimer disease and other neurological and psychiatric diseases. However, it requires accurate, rob&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1501.03915v1-abstract-full').style.display = 'inline'; document.getElementById('1501.03915v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1501.03915v1-abstract-full" style="display: none;"> Neurodegenerative diseases are frequently associated with structural changes in the brain. Magnetic Resonance Imaging (MRI) scans can show these variations and therefore be used as a supportive feature for a number of neurodegenerative diseases. The hippocampus has been known to be a biomarker for Alzheimer disease and other neurological and psychiatric diseases. However, it requires accurate, robust and reproducible delineation of hippocampal structures. Fully automatic methods are usually the voxel based approach, for each voxel a number of local features were calculated. In this paper we compared four different techniques for feature selection from a set of 315 features extracted for each voxel: (i) filter method based on the Kolmogorov-Smirnov test; two wrapper methods, respectively, (ii) Sequential Forward Selection and (iii) Sequential Backward Elimination; and (iv) embedded method based on the Random Forest Classifier on a set of 10 T1-weighted brain MRIs and tested on an independent set of 25 subjects. The resulting segmentations were compared with manual reference labelling. By using only 23 features for each voxel (sequential backward elimination) we obtained comparable state of-the-art performances with respect to the standard tool FreeSurfer. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1501.03915v1-abstract-full').style.display = 'none'; document.getElementById('1501.03915v1-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 January, 2015; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2015. </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">To appear on &#34;Computational and Mathematical Methods in Medicine&#34;, Hindawi Publishing Corporation. 19 pages, 7 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Computational and Mathematical Methods in Medicine Volume 2015, Article ID 814104, 10 pages, Hindawi Publishing Corporation </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> <span class="help" style="display: inline-block;"><a href="https://github.com/arXiv/arxiv-search/releases">Search v0.5.6 released 2020-02-24</a>&nbsp;&nbsp;</span> </div> </div> </main> <footer> <div class="columns is-desktop" role="navigation" aria-label="Secondary"> <!-- MetaColumn 1 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/about">About</a></li> <li><a href="https://info.arxiv.org/help">Help</a></li> </ul> </div> <div class="column"> <ul class="nav-spaced"> <li> <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><title>contact arXiv</title><desc>Click here to contact arXiv</desc><path d="M502.3 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