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<p class="title is-5 mathjax"> The CONUS+ experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Collaboration%2C+T+C">The CONUS+ Collaboration</a>, <a href="/search/hep-ex?searchtype=author&query=%3A"> :</a>, <a href="/search/hep-ex?searchtype=author&query=Ackermann%2C+N">N. Ackermann</a>, <a href="/search/hep-ex?searchtype=author&query=Armbruster%2C+S">S. Armbruster</a>, <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=Fulber%2C+K">K. Fulber</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenmuller%2C+J">J. Hakenmuller</a>, <a href="/search/hep-ex?searchtype=author&query=Hempfling%2C+J">J. Hempfling</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Ni%2C+K">K. Ni</a>, <a href="/search/hep-ex?searchtype=author&query=Rank%2C+M">M. Rank</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Garcia%2C+E+S">E. Sanchez Garcia</a>, <a href="/search/hep-ex?searchtype=author&query=Stalder%2C+I">I. Stalder</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</a>, <a href="/search/hep-ex?searchtype=author&query=Wink%2C+R">R. Wink</a>, <a href="/search/hep-ex?searchtype=author&query=Woenckhaus%2C+J">J. Woenckhaus</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="2407.11912v1-abstract-short" style="display: inline;"> The CONUS+ experiment aims to detect coherent elastic neutrino-nucleus scattering (CEvNS) of reactor antineutrinos on germanium nuclei in the fully coherent regime, continuing on this way the CONUS physics program started at the Brokdorf nuclear power plant, Germany. The CONUS+ setup is installed in the nuclear power plant in Leibstadt, Switzerland, at a distance of 20.7 m from the 3.6 GW thermal… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2407.11912v1-abstract-full').style.display = 'inline'; document.getElementById('2407.11912v1-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2407.11912v1-abstract-full" style="display: none;"> The CONUS+ experiment aims to detect coherent elastic neutrino-nucleus scattering (CEvNS) of reactor antineutrinos on germanium nuclei in the fully coherent regime, continuing on this way the CONUS physics program started at the Brokdorf nuclear power plant, Germany. The CONUS+ setup is installed in the nuclear power plant in Leibstadt, Switzerland, at a distance of 20.7 m from the 3.6 GW thermal power reactor core. The CEvNS signature will be measured with the same four point-contact high-purity germanium (HPGe) detectors produced for the former experiment, however refurbished and with optimized low energy thresholds. To suppress the background in the CONUS+ detectors, the passive and active layers of the original CONUS shield were modified such to fit better to the significantly changed background conditions at the new experimental location. New data acquisition and monitoring systems were developed. A direct network connection between the experiment and the Max-Planck-Institut fur Kernphysik (MPIK) makes it possible to control and monitor data acquisition in real time. The impact of all these modifications is discussed with particular emphasis on the resulting CEvNS signal prediction for the first data collection phase of CONUS+. Prospects of the planned upgrade in a second phase integrating new larger HPGe detectors are also discussed. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2407.11912v1-abstract-full').style.display = 'none'; document.getElementById('2407.11912v1-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 16 July, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 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">14 pages. 12 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2401.13025">arXiv:2401.13025</a> <span> [<a href="https://arxiv.org/pdf/2401.13025">pdf</a>, <a href="https://arxiv.org/format/2401.13025">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy 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/10.1007/JHEP08(2024)171">10.1007/JHEP08(2024)171 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Light vector bosons and the weak mixing angle in the light of future germanium-based reactor CE$谓$NS experiments </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">Manfred Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">Thomas Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Sen%2C+M">Manibrata Sen</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="2401.13025v2-abstract-short" style="display: inline;"> In this work, the sensitivity of future germanium-based reactor neutrino experiments to the weak mixing angle $\sin^{2}胃_{W}$, and to the presence of new light vector bosons is investigated. By taking into account key experimental features with their uncertainties and the application of a data-driven and state-of-the-art reactor antineutrino spectrum, the impact of detection threshold and experime… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2401.13025v2-abstract-full').style.display = 'inline'; document.getElementById('2401.13025v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2401.13025v2-abstract-full" style="display: none;"> In this work, the sensitivity of future germanium-based reactor neutrino experiments to the weak mixing angle $\sin^{2}胃_{W}$, and to the presence of new light vector bosons is investigated. By taking into account key experimental features with their uncertainties and the application of a data-driven and state-of-the-art reactor antineutrino spectrum, the impact of detection threshold and experimental exposure is assessed in detail for an experiment relying on germanium semiconductor detectors. With the established analysis framework, the precision on the Weinberg angle, and capability of probing the parameter space of a universally coupled mediator model, as well as a U(1)$_{\rm B-L}$-symmetric model are quantified. Our investigation finds the next-generation of germanium-based reactor neutrino experiments in good shape to determine the Weinberg angle $\sin^{2}胃_{W}$ with $<10$ % precision using the low-energetic neutrino channel of CE$谓$NS. In addition, the current limits on new light vector bosons determined by reactor experiments can be lowered by about an order of magnitude via the combination of both CE$谓$NS and E$谓$eS. Consequently, our findings provide strong phenomenological support for future experimental endeavours close to a reactor site. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2401.13025v2-abstract-full').style.display = 'none'; document.getElementById('2401.13025v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 23 August, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 23 January, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 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">25 pages, 8 figures; minor title change, figure 6 adapted (improved readability, additional limits), references and discussions added; matches published version</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JHEP08 (2024) 171 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2401.07684">arXiv:2401.07684</a> <span> [<a href="https://arxiv.org/pdf/2401.07684">pdf</a>, <a href="https://arxiv.org/format/2401.07684">other</a>] </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> </div> </div> <p class="title is-5 mathjax"> Final CONUS results on coherent elastic neutrino nucleus scattering at the Brokdorf reactor </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Ackermann%2C+N">N. Ackermann</a>, <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=F%C3%BClber%2C+K">K. F眉lber</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenm%C3%BCller%2C+J">J. Hakenm眉ller</a>, <a href="/search/hep-ex?searchtype=author&query=Hempfling%2C+J">J. Hempfling</a>, <a href="/search/hep-ex?searchtype=author&query=Henrichs%2C+J">J. Henrichs</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Garcia%2C+E+S">E. Sanchez Garcia</a>, <a href="/search/hep-ex?searchtype=author&query=Stauber%2C+J">J. Stauber</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</a>, <a href="/search/hep-ex?searchtype=author&query=Wink%2C+R">R. Wink</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="2401.07684v2-abstract-short" style="display: inline;"> The CONUS experiment studies coherent elastic neutrino nucleus scattering in four 1 kg germanium spectrometers. Low ionization energy thresholds of 210 eV were achieved. The detectors were operated inside an optimized shield at the Brokdorf nuclear power plant which provided a reactor antineutrino flux of up to $2.3\cdot10^{13}$ cm$^{-2}$s$^{-1}$. In the final phase of data collection at this site… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2401.07684v2-abstract-full').style.display = 'inline'; document.getElementById('2401.07684v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2401.07684v2-abstract-full" style="display: none;"> The CONUS experiment studies coherent elastic neutrino nucleus scattering in four 1 kg germanium spectrometers. Low ionization energy thresholds of 210 eV were achieved. The detectors were operated inside an optimized shield at the Brokdorf nuclear power plant which provided a reactor antineutrino flux of up to $2.3\cdot10^{13}$ cm$^{-2}$s$^{-1}$. In the final phase of data collection at this site, the constraints on the neutrino interaction rate were improved by an order of magnitude as compared to the previous CONUS analysis. The new limit of less than 0.34 signal events kg$^{-1}$d$^{-1}$ is within a factor 2 of the rate predicted by the Standard Model. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2401.07684v2-abstract-full').style.display = 'none'; document.getElementById('2401.07684v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 April, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 15 January, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 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">8 figures, 4 tables</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2308.12105">arXiv:2308.12105</a> <span> [<a href="https://arxiv.org/pdf/2308.12105">pdf</a>, <a href="https://arxiv.org/format/2308.12105">other</a>] </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/s10052-024-12470-w">10.1140/epjc/s10052-024-12470-w <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Pulse shape discrimination for the CONUS experiment in the keV and sub-keV regime </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=F%C3%BClber%2C+K">K. F眉lber</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenm%C3%BCller%2C+J">J. Hakenm眉ller</a>, <a href="/search/hep-ex?searchtype=author&query=Hempfling%2C+J">J. Hempfling</a>, <a href="/search/hep-ex?searchtype=author&query=Henrichs%2C+J">J. Henrichs</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Garcia%2C+E+S">E. Sanchez Garcia</a>, <a href="/search/hep-ex?searchtype=author&query=Stauber%2C+J">J. Stauber</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</a>, <a href="/search/hep-ex?searchtype=author&query=Wink%2C+R">R. Wink</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="2308.12105v2-abstract-short" style="display: inline;"> Point-contact p-type high-purity germanium detectors (PPC HPGe) are particularly suited for detection of sub-keV nuclear recoils from coherent elastic scattering of neutrinos or light dark matter particles. While these particles are expected to interact homogeneously in the entire detector volume, specific classes of external background radiation preferably deposit their energy close to the semi-a… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2308.12105v2-abstract-full').style.display = 'inline'; document.getElementById('2308.12105v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2308.12105v2-abstract-full" style="display: none;"> Point-contact p-type high-purity germanium detectors (PPC HPGe) are particularly suited for detection of sub-keV nuclear recoils from coherent elastic scattering of neutrinos or light dark matter particles. While these particles are expected to interact homogeneously in the entire detector volume, specific classes of external background radiation preferably deposit their energy close to the semi-active detector surface, in which diffusion processes dominate that subsequently lead to slower rising pulses compared to the ones from the fully active bulk volume. Dedicated studies of their shape are therefore highly beneficial for the understanding and the rejection of these unwanted events. This article reports about the development of a data-driven pulse shape discrimination (PSD) method for the four 1 kg size PPC HPGe detectors of the CONUS experiment in the keV and sub-keV regime down to 210 eV$_{\text{ee}}$. The impact of the electronic noise at such low energies is carefully examined. It is shown that for an acceptance of 90% of the faster signal-like pulses from the bulk volume, approx. 50% of the surface events can be rejected at the energy threshold and that their contribution is fully suppressed above 800 eV$_{\text{ee}}$. Applied to the CONUS background data, such a PSD rejection cut allows to achieve an overall (15-25)% reduction of the total background budget. The new method allows to improve the sensitivity of future CONUS analyses and to refine the corresponding background model in the sub-keV energy region. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2308.12105v2-abstract-full').style.display = 'none'; document.getElementById('2308.12105v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 February, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 23 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">Journal ref:</span> Eur. Phys. J. C 84, 139 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2205.06712">arXiv:2205.06712</a> <span> [<a href="https://arxiv.org/pdf/2205.06712">pdf</a>, <a href="https://arxiv.org/format/2205.06712">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Coherent elastic neutrino-nucleus scattering -- First constraints/observations and future potential </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">Thomas Rink</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="2205.06712v2-abstract-short" style="display: inline;"> The detection of coherent elastic neutrino-nucleus scattering (CE$谓$NS) opens new possibilities for neutrino physics within and beyond the Standard Model. Following the initial discovery in 2017, several experimental attempts have emerged allowing this reaction channel to be studied with the full repertoire of modern detection technologies. As one of several reactor experiments, CONUS aims for an… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.06712v2-abstract-full').style.display = 'inline'; document.getElementById('2205.06712v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2205.06712v2-abstract-full" style="display: none;"> The detection of coherent elastic neutrino-nucleus scattering (CE$谓$NS) opens new possibilities for neutrino physics within and beyond the Standard Model. Following the initial discovery in 2017, several experimental attempts have emerged allowing this reaction channel to be studied with the full repertoire of modern detection technologies. As one of several reactor experiments, CONUS aims for an observation with antineutrinos emitted from the powerful $3.9$ GW$_{th}$ reactor of the nuclear power plant in Brokdorf (Germany). In particular, the application of ultra-low threshold, high-purity germanium detectors within a sophisticated shield design in close proximity to a nuclear reactor core represents an important step towards high-statistics neutrino detection with small-scale detectors. In addition to the conventional interaction, typical extensions of the Standard Model neutrino sector can be investigated with data provided from different neutrino sources and several target materials. Among these, new neutrino interactions as well as electromagnetic neutrino properties are of particular interest. This talk gives an overview of existing CE$谓$NS results and highlights the advantage of using different neutrino sources and target materials. The example of CONUS is used to demonstrate the various capabilities of recent and future CE$谓$NS measurements. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.06712v2-abstract-full').style.display = 'none'; document.getElementById('2205.06712v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 January, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 13 May, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Contribution to the 2022 Electroweak session of the 56th Rencontres de Moriond; v2: footnote added, references updated</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.07361">arXiv:2203.07361</a> <span> [<a href="https://arxiv.org/pdf/2203.07361">pdf</a>, <a href="https://arxiv.org/format/2203.07361">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Astrophysical Phenomena">astro-ph.HE</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> </div> <p class="title is-5 mathjax"> Coherent elastic neutrino-nucleus scattering: Terrestrial and astrophysical applications </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Abdullah%2C+M">M. Abdullah</a>, <a href="/search/hep-ex?searchtype=author&query=Abele%2C+H">H. Abele</a>, <a href="/search/hep-ex?searchtype=author&query=Akimov%2C+D">D. Akimov</a>, <a href="/search/hep-ex?searchtype=author&query=Angloher%2C+G">G. Angloher</a>, <a href="/search/hep-ex?searchtype=author&query=Aristizabal-Sierra%2C+D">D. Aristizabal-Sierra</a>, <a href="/search/hep-ex?searchtype=author&query=Augier%2C+C">C. Augier</a>, <a href="/search/hep-ex?searchtype=author&query=Balantekin%2C+A+B">A. B. Balantekin</a>, <a href="/search/hep-ex?searchtype=author&query=Balogh%2C+L">L. Balogh</a>, <a href="/search/hep-ex?searchtype=author&query=Barbeau%2C+P+S">P. S. Barbeau</a>, <a href="/search/hep-ex?searchtype=author&query=Baudis%2C+L">L. Baudis</a>, <a href="/search/hep-ex?searchtype=author&query=Baxter%2C+A+L">A. L. Baxter</a>, <a href="/search/hep-ex?searchtype=author&query=Beaufort%2C+C">C. Beaufort</a>, <a href="/search/hep-ex?searchtype=author&query=Beaulieu%2C+G">G. Beaulieu</a>, <a href="/search/hep-ex?searchtype=author&query=Belov%2C+V">V. Belov</a>, <a href="/search/hep-ex?searchtype=author&query=Bento%2C+A">A. Bento</a>, <a href="/search/hep-ex?searchtype=author&query=Berge%2C+L">L. Berge</a>, <a href="/search/hep-ex?searchtype=author&query=Bernardi%2C+I+A">I. A. Bernardi</a>, <a href="/search/hep-ex?searchtype=author&query=Billard%2C+J">J. Billard</a>, <a href="/search/hep-ex?searchtype=author&query=Bolozdynya%2C+A">A. Bolozdynya</a>, <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Bres%2C+G">G. Bres</a>, <a href="/search/hep-ex?searchtype=author&query=Bret%2C+J+L">J-. L. Bret</a>, <a href="/search/hep-ex?searchtype=author&query=Broniatowski%2C+A">A. Broniatowski</a>, <a href="/search/hep-ex?searchtype=author&query=Brossard%2C+A">A. Brossard</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a> , et al. (250 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2203.07361v1-abstract-short" style="display: inline;"> Coherent elastic neutrino-nucleus scattering (CE$谓$NS) is a process in which neutrinos scatter on a nucleus which acts as a single particle. Though the total cross section is large by neutrino standards, CE$谓$NS has long proven difficult to detect, since the deposited energy into the nucleus is $\sim$ keV. In 2017, the COHERENT collaboration announced the detection of CE$谓$NS using a stopped-pion… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.07361v1-abstract-full').style.display = 'inline'; document.getElementById('2203.07361v1-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.07361v1-abstract-full" style="display: none;"> Coherent elastic neutrino-nucleus scattering (CE$谓$NS) is a process in which neutrinos scatter on a nucleus which acts as a single particle. Though the total cross section is large by neutrino standards, CE$谓$NS has long proven difficult to detect, since the deposited energy into the nucleus is $\sim$ keV. In 2017, the COHERENT collaboration announced the detection of CE$谓$NS using a stopped-pion source with CsI detectors, followed up the detection of CE$谓$NS using an Ar target. The detection of CE$谓$NS has spawned a flurry of activities in high-energy physics, inspiring new constraints on beyond the Standard Model (BSM) physics, and new experimental methods. The CE$谓$NS process has important implications for not only high-energy physics, but also astrophysics, nuclear physics, and beyond. This whitepaper discusses the scientific importance of CE$谓$NS, highlighting how present experiments such as COHERENT are informing theory, and also how future experiments will provide a wealth of information across the aforementioned fields of physics. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.07361v1-abstract-full').style.display = 'none'; document.getElementById('2203.07361v1-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 March, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">contribution to Snowmasss 2021. Contact authors: P. S. Barbeau, R. Strauss, L. E. Strigari</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.03754">arXiv:2202.03754</a> <span> [<a href="https://arxiv.org/pdf/2202.03754">pdf</a>, <a href="https://arxiv.org/format/2202.03754">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-022-10768-1">10.1140/epjc/s10052-022-10768-1 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Direct measurement of the ionization quenching factor of nuclear recoils in germanium in the keV energy range </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenm%C3%BCller%2C+J">J. Hakenm眉ller</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Hugle%2C+T">T. Hugle</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Nolte%2C+R">R. Nolte</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Pirovano%2C+E">E. Pirovano</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</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="2202.03754v2-abstract-short" style="display: inline;"> This article reports the measurement of the ionization quenching factor in germanium for nuclear recoil energies between 0.4 and 6.3 keV$_{nr}$. Precise knowledge of this factor in this energy range is relevant for coherent elastic neutrino-nucleus scattering and low mass dark matter searches with germanium-based detectors. Nuclear recoils were produced in a thin high-purity germanium target with… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.03754v2-abstract-full').style.display = 'inline'; document.getElementById('2202.03754v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.03754v2-abstract-full" style="display: none;"> This article reports the measurement of the ionization quenching factor in germanium for nuclear recoil energies between 0.4 and 6.3 keV$_{nr}$. Precise knowledge of this factor in this energy range is relevant for coherent elastic neutrino-nucleus scattering and low mass dark matter searches with germanium-based detectors. Nuclear recoils were produced in a thin high-purity germanium target with a very low energy threshold via irradiation with monoenergetic neutron beams. The energy dependence of the ionization quenching factor was directly measured via kinematically constrained coincidences with surrounding liquid scintillator based neutron detectors. The systematic uncertainties of the measurements are discussed in detail. With measured quenching factors between 0.16 and 0.23 in the [0.4, 6.3] keV$_{nr}$ energy range, the data are compatible with the Lindhard theory with a parameter $k$ of 0.162 $\pm$ 0.004 (stat+sys). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.03754v2-abstract-full').style.display = 'none'; document.getElementById('2202.03754v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 September, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 8 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur. Phys. J. C 82, 815 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2201.12257">arXiv:2201.12257</a> <span> [<a href="https://arxiv.org/pdf/2201.12257">pdf</a>, <a href="https://arxiv.org/format/2201.12257">other</a>] </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> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-022-10722-1">10.1140/epjc/s10052-022-10722-1 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> First upper limits on neutrino electromagnetic properties from the CONUS experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=F%C3%BClber%2C+K">K. F眉lber</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenm%C3%BCller%2C+J">J. Hakenm眉ller</a>, <a href="/search/hep-ex?searchtype=author&query=Hempfling%2C+J">J. Hempfling</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Hugle%2C+T">T. Hugle</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</a>, <a href="/search/hep-ex?searchtype=author&query=Wink%2C+R">R. Wink</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="2201.12257v2-abstract-short" style="display: inline;"> We report first constraints on neutrino electromagnetic properties from neutrino-electron scattering using data obtained from the CONUS germanium detectors, i.e. an upper limit on the effective neutrino magnetic moment and an upper limit on the effective neutrino millicharge. The electron antineutrinos are emitted from the 3.9 GW$_\mathrm{th}$ reactor core of the Brokdorf nuclear power plant in Ge… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2201.12257v2-abstract-full').style.display = 'inline'; document.getElementById('2201.12257v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2201.12257v2-abstract-full" style="display: none;"> We report first constraints on neutrino electromagnetic properties from neutrino-electron scattering using data obtained from the CONUS germanium detectors, i.e. an upper limit on the effective neutrino magnetic moment and an upper limit on the effective neutrino millicharge. The electron antineutrinos are emitted from the 3.9 GW$_\mathrm{th}$ reactor core of the Brokdorf nuclear power plant in Germany. The CONUS low background detectors are positioned at 17.1 m distance from the reactor core center. The analyzed data set includes 689.1 kg$\cdot$d collected during reactor ON periods and 131.0 kg$\cdot$d collected during reactor OFF periods in the energy range of 2 to 8 keV$_{ee}$. With the current statistics, we are able to determine an upper limit on the effective neutrino magnetic moment $渭_谓< 7.5\cdot10^{-11}\,渭_B$ at 90% confidence level. From this first magnetic moment limit we can derive an upper bound on the neutrino millicharge of $\vert q_谓\vert < 3.3\cdot10^{-12}\,e_0$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2201.12257v2-abstract-full').style.display = 'none'; document.getElementById('2201.12257v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 29 January, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">6 pages, 3 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> The European Physical Journal C 82.9 (2022): 813 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2110.02174">arXiv:2110.02174</a> <span> [<a href="https://arxiv.org/pdf/2110.02174">pdf</a>, <a href="https://arxiv.org/format/2110.02174">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy 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/10.1007/JHEP05(2022)085">10.1007/JHEP05(2022)085 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Novel constraints on neutrino physics beyond the standard model from the CONUS experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=CONUS+Collaboration"> CONUS Collaboration</a>, <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=F%C3%BClber%2C+K">K. F眉lber</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenm%C3%BCller%2C+J">J. Hakenm眉ller</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Hugle%2C+T">T. Hugle</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</a>, <a href="/search/hep-ex?searchtype=author&query=Wink%2C+R">R. Wink</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="2110.02174v2-abstract-short" style="display: inline;"> The measurements of coherent elastic neutrino-nucleus scattering (CE$谓$NS) experiments have opened up the possibility to constrain neutrino physics beyond the standard model of elementary particle physics. Furthermore, by considering neutrino-electron scattering in the keV-energy region, it is possible to set additional limits on new physics processes. Here, we present constraints that are derived… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2110.02174v2-abstract-full').style.display = 'inline'; document.getElementById('2110.02174v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2110.02174v2-abstract-full" style="display: none;"> The measurements of coherent elastic neutrino-nucleus scattering (CE$谓$NS) experiments have opened up the possibility to constrain neutrino physics beyond the standard model of elementary particle physics. Furthermore, by considering neutrino-electron scattering in the keV-energy region, it is possible to set additional limits on new physics processes. Here, we present constraints that are derived from CONUS germanium data on beyond the standard model (BSM) processes like tensor and vector non-standard interactions (NSIs) in the neutrino-quark sector, as well as light vector and scalar mediators. Thanks to the realized low background levels in the CONUS experiment at ionization energies below 1 keV, we are able to set the world's best limits on tensor NSIs from CE$谓$NS and constrain the scale of corresponding new physics to lie above 360 GeV. For vector NSIs, the derived limits strongly depend on the assumed ionization quenching factor within the detector material, since small quenching factors largely suppress potential signals for both, the expected standard model CE$谓$NS process and the vector NSIs. Furthermore, competitive limits on scalar and vector mediators are obtained from the CE$谓$NS channel at reactor-site which allow to probe coupling constants as low as $5\cdot10^{-5}$ of low mediator masses, assuming the currently favored quenching factor regime. The consideration of neutrino-electron scatterings allows to set even stronger constraints for mediator masses below $\sim1$ MeV and $\sim 10$ MeV for scalar and vector mediators, respectively. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2110.02174v2-abstract-full').style.display = 'none'; document.getElementById('2110.02174v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 23 May, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 5 October, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 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">35 pages, 6 figures, 3 tables; v2: Figure 2 and further references added, other CE$谓$NS limits included in result plots, matches published version in JHEP</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JHEP 05 (2022) 085 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.00210">arXiv:2011.00210</a> <span> [<a href="https://arxiv.org/pdf/2011.00210">pdf</a>, <a href="https://arxiv.org/format/2011.00210">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevLett.126.041804">10.1103/PhysRevLett.126.041804 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Constraints on elastic neutrino nucleus scattering in the fully coherent regime from the CONUS experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&query=Bonet%2C+H">H. Bonet</a>, <a href="/search/hep-ex?searchtype=author&query=Bonhomme%2C+A">A. Bonhomme</a>, <a href="/search/hep-ex?searchtype=author&query=Buck%2C+C">C. Buck</a>, <a href="/search/hep-ex?searchtype=author&query=F%C3%BClber%2C+K">K. F眉lber</a>, <a href="/search/hep-ex?searchtype=author&query=Hakenm%C3%BCller%2C+J">J. Hakenm眉ller</a>, <a href="/search/hep-ex?searchtype=author&query=Heusser%2C+G">G. Heusser</a>, <a href="/search/hep-ex?searchtype=author&query=Hugle%2C+T">T. Hugle</a>, <a href="/search/hep-ex?searchtype=author&query=Lindner%2C+M">M. Lindner</a>, <a href="/search/hep-ex?searchtype=author&query=Maneschg%2C+W">W. Maneschg</a>, <a href="/search/hep-ex?searchtype=author&query=Rink%2C+T">T. Rink</a>, <a href="/search/hep-ex?searchtype=author&query=Strecker%2C+H">H. Strecker</a>, <a href="/search/hep-ex?searchtype=author&query=Wink%2C+R">R. Wink</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="2011.00210v2-abstract-short" style="display: inline;"> We report the best limit on coherent elastic scattering of electron antineutrinos emitted from a nuclear reactor off germanium nuclei. The measurement was performed with the CONUS detectors positioned at 17.1m from the 3.9GWth reactor core of the nuclear power plant in Brokdorf, Germany. The antineutrino energies of less than 10 MeV assure interactions in the fully coherent regime. The analyzed da… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.00210v2-abstract-full').style.display = 'inline'; document.getElementById('2011.00210v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.00210v2-abstract-full" style="display: none;"> We report the best limit on coherent elastic scattering of electron antineutrinos emitted from a nuclear reactor off germanium nuclei. The measurement was performed with the CONUS detectors positioned at 17.1m from the 3.9GWth reactor core of the nuclear power plant in Brokdorf, Germany. The antineutrino energies of less than 10 MeV assure interactions in the fully coherent regime. The analyzed dataset includes 248.7 kgd with the reactor turned on and background data of 58.8 kgd with the reactor off. With a quenching parameter of k = 0.18 for germanium, we determined an upper limit on the number of neutrino events of 85 in the region of interest at 90% confidence level. This new CONUS dataset disfavors quenching parameters above k = 0.27, under the assumption of standard-model-like coherent scattering of the reactor antineutrinos. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.00210v2-abstract-full').style.display = 'none'; document.getElementById('2011.00210v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 February, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 31 October, 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">6 pages, 4 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. Lett. 126, 041804 (2021) </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> </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="M502.3 190.8c3.9-3.1 9.7-.2 9.7 4.7V400c0 26.5-21.5 48-48 48H48c-26.5 0-48-21.5-48-48V195.6c0-5 5.7-7.8 9.7-4.7 22.4 17.4 52.1 39.5 154.1 113.6 21.1 15.4 56.7 47.8 92.2 47.6 35.7.3 72-32.8 92.3-47.6 102-74.1 131.6-96.3 154-113.7zM256 320c23.2.4 56.6-29.2 73.4-41.4 132.7-96.3 142.8-104.7 173.4-128.7 5.8-4.5 9.2-11.5 9.2-18.9v-19c0-26.5-21.5-48-48-48H48C21.5 64 0 85.5 0 112v19c0 7.4 3.4 14.3 9.2 18.9 30.6 23.9 40.7 32.4 173.4 128.7 16.8 12.2 50.2 41.8 73.4 41.4z"/></svg> <a href="https://info.arxiv.org/help/contact.html"> Contact</a> </li> <li> <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><title>subscribe to arXiv mailings</title><desc>Click here to subscribe</desc><path d="M476 3.2L12.5 270.6c-18.1 10.4-15.8 35.6 2.2 43.2L121 358.4l287.3-253.2c5.5-4.9 13.3 2.6 8.6 8.3L176 407v80.5c0 23.6 28.5 32.9 42.5 15.8L282 426l124.6 52.2c14.2 6 30.4-2.9 33-18.2l72-432C515 7.8 493.3-6.8 476 3.2z"/></svg> <a href="https://info.arxiv.org/help/subscribe"> Subscribe</a> </li> </ul> </div> </div> </div> <!-- end MetaColumn 1 --> <!-- MetaColumn 2 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/help/license/index.html">Copyright</a></li> <li><a href="https://info.arxiv.org/help/policies/privacy_policy.html">Privacy Policy</a></li> </ul> </div> <div class="column sorry-app-links"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/help/web_accessibility.html">Web Accessibility Assistance</a></li> <li> <p class="help"> <a class="a11y-main-link" href="https://status.arxiv.org" target="_blank">arXiv Operational Status <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 256 512" class="icon filter-dark_grey" role="presentation"><path d="M224.3 273l-136 136c-9.4 9.4-24.6 9.4-33.9 0l-22.6-22.6c-9.4-9.4-9.4-24.6 0-33.9l96.4-96.4-96.4-96.4c-9.4-9.4-9.4-24.6 0-33.9L54.3 103c9.4-9.4 24.6-9.4 33.9 0l136 136c9.5 9.4 9.5 24.6.1 34z"/></svg></a><br> Get status notifications via <a class="is-link" href="https://subscribe.sorryapp.com/24846f03/email/new" target="_blank"><svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><path d="M502.3 190.8c3.9-3.1 9.7-.2 9.7 4.7V400c0 26.5-21.5 48-48 48H48c-26.5 0-48-21.5-48-48V195.6c0-5 5.7-7.8 9.7-4.7 22.4 17.4 52.1 39.5 154.1 113.6 21.1 15.4 56.7 47.8 92.2 47.6 35.7.3 72-32.8 92.3-47.6 102-74.1 131.6-96.3 154-113.7zM256 320c23.2.4 56.6-29.2 73.4-41.4 132.7-96.3 142.8-104.7 173.4-128.7 5.8-4.5 9.2-11.5 9.2-18.9v-19c0-26.5-21.5-48-48-48H48C21.5 64 0 85.5 0 112v19c0 7.4 3.4 14.3 9.2 18.9 30.6 23.9 40.7 32.4 173.4 128.7 16.8 12.2 50.2 41.8 73.4 41.4z"/></svg>email</a> or <a class="is-link" href="https://subscribe.sorryapp.com/24846f03/slack/new" target="_blank"><svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 448 512" class="icon filter-black" role="presentation"><path d="M94.12 315.1c0 25.9-21.16 47.06-47.06 47.06S0 341 0 315.1c0-25.9 21.16-47.06 47.06-47.06h47.06v47.06zm23.72 0c0-25.9 21.16-47.06 47.06-47.06s47.06 21.16 47.06 47.06v117.84c0 25.9-21.16 47.06-47.06 47.06s-47.06-21.16-47.06-47.06V315.1zm47.06-188.98c-25.9 0-47.06-21.16-47.06-47.06S139 32 164.9 32s47.06 21.16 47.06 47.06v47.06H164.9zm0 23.72c25.9 0 47.06 21.16 47.06 47.06s-21.16 47.06-47.06 47.06H47.06C21.16 243.96 0 222.8 0 196.9s21.16-47.06 47.06-47.06H164.9zm188.98 47.06c0-25.9 21.16-47.06 47.06-47.06 25.9 0 47.06 21.16 47.06 47.06s-21.16 47.06-47.06 47.06h-47.06V196.9zm-23.72 0c0 25.9-21.16 47.06-47.06 47.06-25.9 0-47.06-21.16-47.06-47.06V79.06c0-25.9 21.16-47.06 47.06-47.06 25.9 0 47.06 21.16 47.06 47.06V196.9zM283.1 385.88c25.9 0 47.06 21.16 47.06 47.06 0 25.9-21.16 47.06-47.06 47.06-25.9 0-47.06-21.16-47.06-47.06v-47.06h47.06zm0-23.72c-25.9 0-47.06-21.16-47.06-47.06 0-25.9 21.16-47.06 47.06-47.06h117.84c25.9 0 47.06 21.16 47.06 47.06 0 25.9-21.16 47.06-47.06 47.06H283.1z"/></svg>slack</a> </p> </li> </ul> </div> </div> </div> <!-- end MetaColumn 2 --> </div> </footer> <script src="https://static.arxiv.org/static/base/1.0.0a5/js/member_acknowledgement.js"></script> </body> </html>