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aria-label="Page 3" aria-current="page">3 </a> </li> </ul> </nav> <ol class="breathe-horizontal" start="1"> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.01996">arXiv:2410.01996</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.01996">pdf</a>, <a href="https://arxiv.org/format/2410.01996">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> </div> </div> <p class="title is-5 mathjax"> Limits on the Low-Energy Electron Antineutrino Flux from the Brightest GRB of All Time </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Araki%2C+T">T. Araki</a>, <a href="/search/?searchtype=author&amp;query=Chauhan%2C+S">S. Chauhan</a>, <a href="/search/?searchtype=author&amp;query=Chiba%2C+K">K. Chiba</a>, <a href="/search/?searchtype=author&amp;query=Eda%2C+T">T. Eda</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Funahashi%2C+Y">Y. Funahashi</a>, <a href="/search/?searchtype=author&amp;query=Furuto%2C+A">A. Furuto</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+S">S. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Marthe%2C+A">A. Marthe</a>, <a href="/search/?searchtype=author&amp;query=Matsumoto%2C+Y">Y. Matsumoto</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Morita%2C+D">D. Morita</a> , et al. (48 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="2410.01996v2-abstract-short" style="display: inline;"> The electron antinuetrino flux limits are presented for the brightest gamma-ray burst (GRB) of all time, GRB221009A, over a range of 1.8-200 MeV using the Kamioka Liquid Scintillator Anti Neutrino Detector (KamLAND). Using a variety of time windows to search for electron antineutrinos coincident with the GRB, we set an upper limit on the flux under the assumption of various neutrino source spectra&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.01996v2-abstract-full').style.display = 'inline'; document.getElementById('2410.01996v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.01996v2-abstract-full" style="display: none;"> The electron antinuetrino flux limits are presented for the brightest gamma-ray burst (GRB) of all time, GRB221009A, over a range of 1.8-200 MeV using the Kamioka Liquid Scintillator Anti Neutrino Detector (KamLAND). Using a variety of time windows to search for electron antineutrinos coincident with the GRB, we set an upper limit on the flux under the assumption of various neutrino source spectra. No excess was observed in any time windows ranging from seconds to days around the event trigger time. The limits are compared to the results presented by IceCube. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.01996v2-abstract-full').style.display = 'none'; document.getElementById('2410.01996v2-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> 21 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 2 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 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 pages, 3 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/2409.12756">arXiv:2409.12756</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.12756">pdf</a>, <a href="https://arxiv.org/format/2409.12756">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurement of elliptic flow of J$/蠄$ in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions at forward rapidity </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Antsupov%2C+S">S. Antsupov</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Ayuso%2C+C">C. Ayuso</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Bannikov%2C+E">E. Bannikov</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a> , et al. (344 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="2409.12756v1-abstract-short" style="display: inline;"> We report the first measurement of the azimuthal anisotropy of J$/蠄$ at forward rapidity ($1.2&lt;|畏|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV at the Relativistic Heavy Ion Collider. The data were collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The second Fourier coefficient ($v_2$) of the azimuthal distribution of $J/蠄$ is determined&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.12756v1-abstract-full').style.display = 'inline'; document.getElementById('2409.12756v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.12756v1-abstract-full" style="display: none;"> We report the first measurement of the azimuthal anisotropy of J$/蠄$ at forward rapidity ($1.2&lt;|畏|&lt;2.2$) in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV at the Relativistic Heavy Ion Collider. The data were collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The second Fourier coefficient ($v_2$) of the azimuthal distribution of $J/蠄$ is determined as a function of the transverse momentum ($p_T$) using the event-plane method. The measurements were performed for several selections of collision centrality: 0\%--50\%, 10\%--60\%, and 10\%-40\%. We find that in all cases the values of $v_2(p_T)$, which quantify the elliptic flow of J$/蠄$, are consistent with zero. The results are consistent with measurements at midrapidity, indicating no significant elliptic flow of the J$/蠄$ within the quark-gluon-plasma medium at collision energies of $\sqrt{s_{_{NN}}}=200$ GeV. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.12756v1-abstract-full').style.display = 'none'; document.getElementById('2409.12756v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 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">369 authors from 72 institutions, 12 pages, 7 figures, 5 tables. v1 is version submitted to Physical Review C. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.12715">arXiv:2409.12715</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.12715">pdf</a>, <a href="https://arxiv.org/format/2409.12715">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurements at forward rapidity of elliptic flow of charged hadrons and open-heavy-flavor muons in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Antsupov%2C+S">S. Antsupov</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Ayuso%2C+C">C. Ayuso</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Bannikov%2C+E">E. Bannikov</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a> , et al. (344 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="2409.12715v1-abstract-short" style="display: inline;"> We present the first forward-rapidity measurements of elliptic anisotropy of open-heavy-flavor muons at the BNL Relativistic Heavy Ion Collider. The measurements are based on data samples of Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The measurements are performed in the pseudorapidity range&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.12715v1-abstract-full').style.display = 'inline'; document.getElementById('2409.12715v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.12715v1-abstract-full" style="display: none;"> We present the first forward-rapidity measurements of elliptic anisotropy of open-heavy-flavor muons at the BNL Relativistic Heavy Ion Collider. The measurements are based on data samples of Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV collected by the PHENIX experiment in 2014 and 2016 with integrated luminosity of 14.5~nb$^{-1}$. The measurements are performed in the pseudorapidity range $1.2&lt;|畏|&lt;2$ and cover transverse momenta $1&lt;p_T&lt;4$~GeV/$c$. The elliptic flow of charged hadrons as a function of transverse momentum is also measured in the same kinematic range. We observe significant elliptic flow for both charged hadrons and heavy-flavor muons. The results show clear mass ordering of elliptic flow of light- and heavy-flavor particles. The magnitude of the measured $v_2$ is comparable to that in the midrapidity region. This indicates that there is no strong longitudinal dependence in the quark-gluon-plasma evolution between midrapidity and the rapidity range of this measurement at $\sqrt{s_{_{NN}}}=200$~GeV. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.12715v1-abstract-full').style.display = 'none'; document.getElementById('2409.12715v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 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">369 authors from 72 institutions, 12 pages, 7 figures, 2 tables. v1 is version submitted to Physical Review C. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.03728">arXiv:2409.03728</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.03728">pdf</a>, <a href="https://arxiv.org/format/2409.03728">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> </div> </div> <p class="title is-5 mathjax"> Multiplicity dependent $J/蠄$ and $蠄(2S)$ production at forward and backward rapidity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Antsupov%2C+S">S. Antsupov</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannikov%2C+E">E. Bannikov</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a> , et al. (276 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="2409.03728v1-abstract-short" style="display: inline;"> The $J/蠄$ and $蠄(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics in high-energy hadronic interactions. However, there is not yet a complete understanding of the charmonium-production mechanism. Recent measurements of $J/蠄$ production as a function of event charged-particle multiplicity&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.03728v1-abstract-full').style.display = 'inline'; document.getElementById('2409.03728v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.03728v1-abstract-full" style="display: none;"> The $J/蠄$ and $蠄(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics in high-energy hadronic interactions. However, there is not yet a complete understanding of the charmonium-production mechanism. Recent measurements of $J/蠄$ production as a function of event charged-particle multiplicity at the collision energies of both the Large Hadron Collider (LHC) and the Relativistic Heavy Ion Collider (RHIC) show enhanced $J/蠄$ production yields with increasing multiplicity. One potential explanation for this type of dependence is multiparton interactions (MPI). We carry out the first measurements of self-normalized $J/蠄$ yields and the $蠄(2S)$ to $J/蠄$ ratio at both forward and backward rapidities as a function of self-normalized charged-particle multiplicity in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV. In addition, detailed {\sc pythia} studies tuned to RHIC energies were performed to investigate the MPI impacts. We find that the PHENIX data at RHIC are consistent with recent LHC measurements and can only be described by {\sc pythia} calculations that include MPI effects. The forward and backward $蠄(2S)$ to $J/蠄$ ratio, which serves as a unique and powerful approach to study final-state effects on charmonium production, is found to be less dependent on the charged-particle multiplicity. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.03728v1-abstract-full').style.display = 'none'; document.getElementById('2409.03728v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 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">301 authors from 69 institutions, 8 pages, 3 figures. v1 is version submitted to Physical Review D Letters. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2408.11144">arXiv:2408.11144</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2408.11144">pdf</a>, <a href="https://arxiv.org/format/2408.11144">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Measurement of inclusive jet cross section and substructure in $p$$+$$p$ collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Antsupov%2C+S">S. Antsupov</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+X">X. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Bannikov%2C+E">E. Bannikov</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a> , et al. (422 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="2408.11144v1-abstract-short" style="display: inline;"> The jet cross-section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0&lt;p_T&lt;40.0$ Ge&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.11144v1-abstract-full').style.display = 'inline'; document.getElementById('2408.11144v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2408.11144v1-abstract-full" style="display: none;"> The jet cross-section and jet-substructure observables in $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV were measured by the PHENIX Collaboration at the Relativistic Heavy Ion Collider (RHIC). Jets are reconstructed from charged-particle tracks and electromagnetic-calorimeter clusters using the anti-$k_{t}$ algorithm with a jet radius $R=0.3$ for jets with transverse momentum within $8.0&lt;p_T&lt;40.0$ GeV/$c$ and pseudorapidity $|畏|&lt;0.15$. Measurements include the jet cross section, as well as distributions of SoftDrop-groomed momentum fraction ($z_g$), charged-particle transverse momentum with respect to jet axis ($j_T$), and radial distributions of charged particles within jets ($r$). Also meaureed was the distribution of $尉=-ln(z)$, where $z$ is the fraction of the jet momentum carried by the charged particle. The measurements are compared to theoretical next-to and next-to-next-to-leading-order calculatios, PYTHIA event generator, and to other existing experimental results. Indicated from these meaurements is a lower particle multiplicity in jets at RHIC energies when compared to models. Also noted are implications for future jet measurements with sPHENIX at RHIC as well as at the future Election-Ion Collider. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.11144v1-abstract-full').style.display = 'none'; document.getElementById('2408.11144v1-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 August, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 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">446 authors from 77 institutions, 11 pages, 8 figures. v1 is version submitted to Physical Review D. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2407.08586">arXiv:2407.08586</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2407.08586">pdf</a>, <a href="https://arxiv.org/format/2407.08586">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Centrality dependence of L茅vy-stable two-pion Bose-Einstein correlations in $\sqrt{s_{_{NN}}}=200$ GeV Au$+$Au collisions </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Al-Ta%27ani%2C+H">H. Al-Ta&#39;ani</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Angerami%2C+A">A. Angerami</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Aschenauer%2C+E+C">E. C. Aschenauer</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bassalleck%2C+B">B. Bassalleck</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a> , et al. (377 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="2407.08586v2-abstract-short" style="display: inline;"> The PHENIX experiment measured the centrality dependence of two-pion Bose-Einstein correlation functions in $\sqrt{s_{_{NN}}}=200$~GeV Au$+$Au collisions at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory. The data are well represented by L茅vy-stable source distributions. The extracted source parameters are the correlation-strength parameter $位$, the L茅vy index of stability&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2407.08586v2-abstract-full').style.display = 'inline'; document.getElementById('2407.08586v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2407.08586v2-abstract-full" style="display: none;"> The PHENIX experiment measured the centrality dependence of two-pion Bose-Einstein correlation functions in $\sqrt{s_{_{NN}}}=200$~GeV Au$+$Au collisions at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory. The data are well represented by L茅vy-stable source distributions. The extracted source parameters are the correlation-strength parameter $位$, the L茅vy index of stability $伪$, and the L茅vy-scale parameter $R$ as a function of transverse mass $m_T$ and centrality. The $位(m_T)$ parameter is constant at larger values of $m_T$, but decreases as $m_T$ decreases. The L茅vy scale parameter $R(m_T)$ decreases with $m_T$ and exhibits proportionality to the length scale of the nuclear overlap region. The L茅vy exponent $伪(m_T)$ is independent of $m_T$ within uncertainties in each investigated centrality bin, but shows a clear centrality dependence. At all centralities, the L茅vy exponent $伪$ is significantly different from that of Gaussian ($伪=2$) or Cauchy ($伪=1$) source distributions. Comparisons to the predictions of Monte-Carlo simulations of resonance-decay chains show that in all but the most peripheral centrality class (50%-60%), the obtained results are inconsistent with the measurements, unless a significant reduction of the in-medium mass of the $畏&#39;$ meson is included. In each centrality class, the best value of the in-medium $畏&#39;$ mass is compared to the mass of the $畏$ meson, as well as to several theoretical predictions that consider restoration of $U_A(1)$ symmetry in hot hadronic matter. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2407.08586v2-abstract-full').style.display = 'none'; document.getElementById('2407.08586v2-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 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 11 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">401 authors from 75 institutions, 23 pages, 15 figures, 2 tables. v2 is version accepted for publication by Physical Review C. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2406.11438">arXiv:2406.11438</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2406.11438">pdf</a>, <a href="https://arxiv.org/format/2406.11438">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> </div> </div> <p class="title is-5 mathjax"> Search for Majorana Neutrinos with the Complete KamLAND-Zen Dataset </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Araki%2C+T">T. Araki</a>, <a href="/search/?searchtype=author&amp;query=Chiba%2C+K">K. Chiba</a>, <a href="/search/?searchtype=author&amp;query=Eda%2C+T">T. Eda</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Funahashi%2C+Y">Y. Funahashi</a>, <a href="/search/?searchtype=author&amp;query=Furuto%2C+A">A. Furuto</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+S">S. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Marthe%2C+A">A. Marthe</a>, <a href="/search/?searchtype=author&amp;query=Matsumoto%2C+Y">Y. Matsumoto</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a> , et al. (48 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="2406.11438v1-abstract-short" style="display: inline;"> We present a search for neutrinoless double-beta ($0谓尾尾$) decay of $^{136}$Xe using the full KamLAND-Zen 800 dataset with 745 kg of enriched xenon, corresponding to an exposure of $2.097$ ton yr of $^{136}$Xe. This updated search benefits from a more than twofold increase in exposure, recovery of photo-sensor gain, and reduced background from muon-induced spallation of xenon. Combining with the se&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2406.11438v1-abstract-full').style.display = 'inline'; document.getElementById('2406.11438v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2406.11438v1-abstract-full" style="display: none;"> We present a search for neutrinoless double-beta ($0谓尾尾$) decay of $^{136}$Xe using the full KamLAND-Zen 800 dataset with 745 kg of enriched xenon, corresponding to an exposure of $2.097$ ton yr of $^{136}$Xe. This updated search benefits from a more than twofold increase in exposure, recovery of photo-sensor gain, and reduced background from muon-induced spallation of xenon. Combining with the search in the previous KamLAND-Zen phase, we obtain a lower limit for the $0谓尾尾$ decay half-life of $T_{1/2}^{0谓} &gt; 3.8 \times 10^{26}$ yr at 90% C.L., a factor of 1.7 improvement over the previous limit. The corresponding upper limits on the effective Majorana neutrino mass are in the range 28-122 meV using phenomenological nuclear matrix element calculations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2406.11438v1-abstract-full').style.display = 'none'; document.getElementById('2406.11438v1-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> 17 June, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 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">arXiv admin note: text overlap with arXiv:2203.02139</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2406.08301">arXiv:2406.08301</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2406.08301">pdf</a>, <a href="https://arxiv.org/format/2406.08301">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.110.044901">10.1103/PhysRevC.110.044901 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Jet modification via $蟺^0$-hadron correlations in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Afanasiev%2C+S">S. Afanasiev</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Al-Bataineh%2C+H">H. Al-Bataineh</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aphecetche%2C+L">L. Aphecetche</a>, <a href="/search/?searchtype=author&amp;query=Asai%2C+J">J. Asai</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Averbeck%2C+R">R. Averbeck</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Baksay%2C+G">G. Baksay</a>, <a href="/search/?searchtype=author&amp;query=Baksay%2C+L">L. Baksay</a>, <a href="/search/?searchtype=author&amp;query=Baldisseri%2C+A">A. Baldisseri</a> , et al. (511 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="2406.08301v2-abstract-short" style="display: inline;"> High-momentum two-particle correlations are a useful tool for studying jet-quenching effects in the quark-gluon plasma. Angular correlations between neutral-pion triggers and charged hadrons with transverse momenta in the range 4--12~GeV/$c$ and 0.5--7~GeV/$c$, respectively, have been measured by the PHENIX experiment in 2014 for Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$~GeV. Suppression is obs&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2406.08301v2-abstract-full').style.display = 'inline'; document.getElementById('2406.08301v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2406.08301v2-abstract-full" style="display: none;"> High-momentum two-particle correlations are a useful tool for studying jet-quenching effects in the quark-gluon plasma. Angular correlations between neutral-pion triggers and charged hadrons with transverse momenta in the range 4--12~GeV/$c$ and 0.5--7~GeV/$c$, respectively, have been measured by the PHENIX experiment in 2014 for Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$~GeV. Suppression is observed in the yield of high-momentum jet fragments opposite the trigger particle, which indicates jet suppression stemming from in-medium partonic energy loss, while enhancement is observed for low-momentum particles. The ratio and differences between the yield in Au$+$Au collisions and $p$$+$$p$ collisions, $I_{AA}$ and $螖_{AA}$, as a function of the trigger-hadron azimuthal separation, $螖蠁$, are measured for the first time at the Relativistic Heavy Ion Collider. These results better quantify how the yield of low-$p_T$ associated hadrons is enhanced at wide angle, which is crucial for studying energy loss as well as medium-response effects. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2406.08301v2-abstract-full').style.display = 'none'; document.getElementById('2406.08301v2-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> 1 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 12 June, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 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">535 authors from 84 institutions, 12 pages, 8 figures. v2 is version accepted for publication in Physical Review C. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 110, 044901 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2404.09920">arXiv:2404.09920</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2404.09920">pdf</a>, <a href="https://arxiv.org/format/2404.09920">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 Astrophysical Phenomena">astro-ph.HE</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/10.3847/1538-4357/ad5fee">10.3847/1538-4357/ad5fee <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Combined Pre-Supernova Alert System with Kamland and Super-Kamiokande </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=KamLAND"> KamLAND</a>, <a href="/search/?searchtype=author&amp;query=Collaborations%2C+S">Super-Kamiokande Collaborations</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Abe%2C+S">Seisho Abe</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">Minori Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">Sawako Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">Azusa Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Yoshihito Gando</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+S">Shun Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">Takahiko Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">Kazumi Hata</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">Koichi Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">Sei Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">Haruo Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">Kunio Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">Koji Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Yuto Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">Nanami Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Yasuhiro Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">Masayuki Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">Maho Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">Tadao Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">Haruhiko Miyake</a>, <a href="/search/?searchtype=author&amp;query=Morita%2C+D">Daisuke Morita</a>, <a href="/search/?searchtype=author&amp;query=Nakahata%2C+T">Takeshi Nakahata</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="2404.09920v3-abstract-short" style="display: inline;"> Preceding a core-collapse supernova, various processes produce an increasing amount of neutrinos of all flavors characterized by mounting energies from the interior of massive stars. Among them, the electron antineutrinos are potentially detectable by terrestrial neutrino experiments such as KamLAND and Super-Kamiokande via inverse beta decay interactions. Once these pre-supernova neutrinos are ob&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2404.09920v3-abstract-full').style.display = 'inline'; document.getElementById('2404.09920v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2404.09920v3-abstract-full" style="display: none;"> Preceding a core-collapse supernova, various processes produce an increasing amount of neutrinos of all flavors characterized by mounting energies from the interior of massive stars. Among them, the electron antineutrinos are potentially detectable by terrestrial neutrino experiments such as KamLAND and Super-Kamiokande via inverse beta decay interactions. Once these pre-supernova neutrinos are observed, an early warning of the upcoming core-collapse supernova can be provided. In light of this, KamLAND and Super-Kamiokande, both located in the Kamioka mine in Japan, have been monitoring pre-supernova neutrinos since 2015 and 2021, respectively. Recently, we performed a joint study between KamLAND and Super-Kamiokande on pre-supernova neutrino detection. A pre-supernova alert system combining the KamLAND detector and the Super-Kamiokande detector was developed and put into operation, which can provide a supernova alert to the astrophysics community. Fully leveraging the complementary properties of these two detectors, the combined alert is expected to resolve a pre-supernova neutrino signal from a 15 M$_{\odot}$ star within 510 pc of the Earth, at a significance level corresponding to a false alarm rate of no more than 1 per century. For a Betelgeuse-like model with optimistic parameters, it can provide early warnings up to 12 hours in advance. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2404.09920v3-abstract-full').style.display = 'none'; document.getElementById('2404.09920v3-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> 1 July, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 15 April, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 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">Resubmitted to ApJ. 22 pages, 16 figures, for more information about the combined pre-supernova alert system, see https://www.lowbg.org/presnalarm/</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2312.09827">arXiv:2312.09827</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2312.09827">pdf</a>, <a href="https://arxiv.org/format/2312.09827">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.109.054910">10.1103/PhysRevC.109.054910 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Identified charged-hadron production in $p$$+$Al, $^3$He$+$Au, and Cu$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV and in U$+$U collisions at $\sqrt{s_{_{NN}}}=193$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+X">X. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Baublis%2C+V">V. Baublis</a> , et al. (456 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="2312.09827v2-abstract-short" style="display: inline;"> The PHENIX experiment has performed a systematic study of identified charged-hadron ($蟺^\pm$, $K^\pm$, $p$, $\bar{p}$) production at midrapidity in $p$$+$Al, $^3$He$+$Au, Cu$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV and U$+$U collisions at $\sqrt{s_{_{NN}}}=193$ GeV. Identified charged-hadron invariant transverse-momentum ($p_T$) and transverse-mass ($m_T$) spectra are presented and interprete&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2312.09827v2-abstract-full').style.display = 'inline'; document.getElementById('2312.09827v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2312.09827v2-abstract-full" style="display: none;"> The PHENIX experiment has performed a systematic study of identified charged-hadron ($蟺^\pm$, $K^\pm$, $p$, $\bar{p}$) production at midrapidity in $p$$+$Al, $^3$He$+$Au, Cu$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV and U$+$U collisions at $\sqrt{s_{_{NN}}}=193$ GeV. Identified charged-hadron invariant transverse-momentum ($p_T$) and transverse-mass ($m_T$) spectra are presented and interpreted in terms of radially expanding thermalized systems. The particle ratios of $K/蟺$ and $p/蟺$ have been measured in different centrality ranges of large (Cu$+$Au, U$+$U) and small ($p$$+$Al, $^3$He$+$Au) collision systems. The values of $K/蟺$ ratios measured in all considered collision systems were found to be consistent with those measured in $p$$+$$p$ collisions. However the values of $p/蟺$ ratios measured in large collision systems reach the values of $\approx0.6$, which is $\approx2$ times larger than in $p$$+$$p$ collisions. These results can be qualitatively understood in terms of the baryon enhancement expected from hadronization by recombination. Identified charged-hadron nuclear-modification factors ($R_{AB}$) are also presented. Enhancement of proton $R_{AB}$ values over meson $R_{AB}$ values was observed in central $^3$He$+$Au, Cu$+$Au, and U$+$U collisions. The proton $R_{AB}$ values measured in $p$$+$Al collision system were found to be consistent with $R_{AB}$ values of $蠁$, $蟺^\pm$, $K^\pm$, and $蟺^0$ mesons, which may indicate that the size of the system produced in $p$$+$Al collisions is too small for recombination to cause a noticeable increase in proton production. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2312.09827v2-abstract-full').style.display = 'none'; document.getElementById('2312.09827v2-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 14 December, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">480 authors from 78 institutions, 18 pages, 6 tables, 16 figures. v2 is version accepted for publication in Physical Review C. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 109, 054910 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2311.09676">arXiv:2311.09676</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2311.09676">pdf</a>, <a href="https://arxiv.org/format/2311.09676">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1016/j.physletb.2024.138846">10.1016/j.physletb.2024.138846 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for Charged Excited States of Dark Matter with KamLAND-Zen </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=collaboration%2C+K">KamLAND-Zen collaboration</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+S">S. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Morita%2C+D">D. Morita</a>, <a href="/search/?searchtype=author&amp;query=Nakahata%2C+T">T. Nakahata</a> , et al. (44 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="2311.09676v2-abstract-short" style="display: inline;"> Particle dark matter could belong to a multiplet that includes an electrically charged state. WIMP dark matter ($蠂^{0}$) accompanied by a negatively charged excited state ($蠂^{-}$) with a small mass difference (e.g. $&lt;$ 20 MeV) can form a bound-state with a nucleus such as xenon. This bound-state formation is rare and the released energy is $\mathcal{O}(1-10$) MeV depending on the nucleus, making&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.09676v2-abstract-full').style.display = 'inline'; document.getElementById('2311.09676v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2311.09676v2-abstract-full" style="display: none;"> Particle dark matter could belong to a multiplet that includes an electrically charged state. WIMP dark matter ($蠂^{0}$) accompanied by a negatively charged excited state ($蠂^{-}$) with a small mass difference (e.g. $&lt;$ 20 MeV) can form a bound-state with a nucleus such as xenon. This bound-state formation is rare and the released energy is $\mathcal{O}(1-10$) MeV depending on the nucleus, making large liquid scintillator detectors suitable for detection. We searched for bound-state formation events with xenon in two experimental phases of the KamLAND-Zen experiment, a xenon-doped liquid scintillator detector. No statistically significant events were observed. For a benchmark parameter set of WIMP mass $m_{蠂^{0}} = 1$ TeV and mass difference $螖m = 17$ MeV, we set the most stringent upper limits on the recombination cross section times velocity $\langle蟽v\rangle$ and the decay-width of $蠂^{-}$ to $9.2 \times 10^{-30}$ ${\rm cm^3/s}$ and $8.7 \times 10^{-14}$ GeV, respectively at 90% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.09676v2-abstract-full').style.display = 'none'; document.getElementById('2311.09676v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 July, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 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">Journal ref:</span> Phys. Lett. B 855 (2024) 138846 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2311.07413">arXiv:2311.07413</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2311.07413">pdf</a>, <a href="https://arxiv.org/format/2311.07413">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/19/07/P07006">10.1088/1748-0221/19/07/P07006 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Performance of the electromagnetic and hadronic prototype segments of the ALICE Forward Calorimeter </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Aehle%2C+M">M. Aehle</a>, <a href="/search/?searchtype=author&amp;query=Alme%2C+J">J. Alme</a>, <a href="/search/?searchtype=author&amp;query=Arata%2C+C">C. Arata</a>, <a href="/search/?searchtype=author&amp;query=Arsene%2C+I">I. Arsene</a>, <a href="/search/?searchtype=author&amp;query=Bearden%2C+I">I. Bearden</a>, <a href="/search/?searchtype=author&amp;query=Bodova%2C+T">T. Bodova</a>, <a href="/search/?searchtype=author&amp;query=Borshchov%2C+V">V. Borshchov</a>, <a href="/search/?searchtype=author&amp;query=Bourrion%2C+O">O. Bourrion</a>, <a href="/search/?searchtype=author&amp;query=Bregant%2C+M">M. Bregant</a>, <a href="/search/?searchtype=author&amp;query=Brink%2C+A+v+d">A. van den Brink</a>, <a href="/search/?searchtype=author&amp;query=Buchakchiev%2C+V">V. Buchakchiev</a>, <a href="/search/?searchtype=author&amp;query=Buhl%2C+A">A. Buhl</a>, <a href="/search/?searchtype=author&amp;query=Chujo%2C+T">T. Chujo</a>, <a href="/search/?searchtype=author&amp;query=Dufke%2C+L">L. Dufke</a>, <a href="/search/?searchtype=author&amp;query=Eikeland%2C+V">V. Eikeland</a>, <a href="/search/?searchtype=author&amp;query=Fasel%2C+M">M. Fasel</a>, <a href="/search/?searchtype=author&amp;query=Gauger%2C+N">N. Gauger</a>, <a href="/search/?searchtype=author&amp;query=Gautam%2C+A">A. Gautam</a>, <a href="/search/?searchtype=author&amp;query=Ghimouz%2C+A">A. Ghimouz</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+Y">Y. Goto</a>, <a href="/search/?searchtype=author&amp;query=Guernane%2C+R">R. Guernane</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hassan%2C+H">H. Hassan</a>, <a href="/search/?searchtype=author&amp;query=He%2C+L">L. He</a>, <a href="/search/?searchtype=author&amp;query=Helstrup%2C+H">H. Helstrup</a> , et al. (52 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="2311.07413v2-abstract-short" style="display: inline;"> We present the performance of a full-length prototype of the ALICE Forward Calorimeter (FoCal). The detector is composed of a silicon-tungsten electromagnetic sampling calorimeter with longitudinal and transverse segmentation (FoCal-E) of about 20$X_0$ and a hadronic copper-scintillating-fiber calorimeter (FoCal-H) of about 5$位_{\rm int}$. The data were taken between 2021 and 2023 at the CERN PS a&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.07413v2-abstract-full').style.display = 'inline'; document.getElementById('2311.07413v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2311.07413v2-abstract-full" style="display: none;"> We present the performance of a full-length prototype of the ALICE Forward Calorimeter (FoCal). The detector is composed of a silicon-tungsten electromagnetic sampling calorimeter with longitudinal and transverse segmentation (FoCal-E) of about 20$X_0$ and a hadronic copper-scintillating-fiber calorimeter (FoCal-H) of about 5$位_{\rm int}$. The data were taken between 2021 and 2023 at the CERN PS and SPS beam lines with hadron (electron) beams up to energies of 350 (300) GeV. Regarding FoCal-E, we report a comprehensive analysis of its response to minimum ionizing particles across all pad layers. The longitudinal shower profile of electromagnetic showers is measured with a layer-wise segmentation of 1$X_0$. As a projection to the performance of the final detector in electromagnetic showers, we demonstrate linearity in the full energy range, and show that the energy resolution fulfills the requirements for the physics needs. Additionally, the performance to separate two-showers events was studied by quantifying the transverse shower width. Regarding FoCal-H, we report a detailed analysis of the response to hadron beams between 60 and 350 GeV. The results are compared to simulations obtained with a Geant4 model of the test beam setup, which in particular for FoCal-E are in good agreement with the data. The energy resolution of FoCal-E was found to be lower than 3% at energies larger than 100 GeV. The response of FoCal-H to hadron beams was found to be linear, albeit with a significant intercept that is about factor 2 larger than in simulations. Its resolution, which is non-Gaussian and generally larger than in simulations, was quantified using the FWHM, and decreases from about 16% at 100 GeV to about 11% at 350 GeV. The discrepancy to simulations, which is particularly evident at low hadron energies, needs to be further investigated. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2311.07413v2-abstract-full').style.display = 'none'; document.getElementById('2311.07413v2-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 July, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 13 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">57 pages (without acronyms), 45 captioned figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JINST 19 P07006 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2306.06153">arXiv:2306.06153</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2306.06153">pdf</a>, <a href="https://arxiv.org/format/2306.06153">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"> A Large-Scale Pad-Sensor Based Prototype of the Silicon Tungsten Electromagnetic Calorimeter for the Forward Direction in ALICE at LHC </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Barthel%2C+R+G+E">R. G. E. Barthel</a>, <a href="/search/?searchtype=author&amp;query=Chujo%2C+T">T. Chujo</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hatakeyama%2C+M">M. Hatakeyama</a>, <a href="/search/?searchtype=author&amp;query=Hoshi%2C+Y">Y. Hoshi</a>, <a href="/search/?searchtype=author&amp;query=Inaba%2C+M">M. Inaba</a>, <a href="/search/?searchtype=author&amp;query=Y."> Y.</a>, <a href="/search/?searchtype=author&amp;query=Kawamura"> Kawamura</a>, <a href="/search/?searchtype=author&amp;query=Kawana%2C+D">D. Kawana</a>, <a href="/search/?searchtype=author&amp;query=Loizides%2C+C">C. Loizides</a>, <a href="/search/?searchtype=author&amp;query=Miake%2C+Y">Y. Miake</a>, <a href="/search/?searchtype=author&amp;query=Minato%2C+Y">Y. Minato</a>, <a href="/search/?searchtype=author&amp;query=Nakagawa%2C+K">K. Nakagawa</a>, <a href="/search/?searchtype=author&amp;query=Novitzky%2C+N">N. Novitzky</a>, <a href="/search/?searchtype=author&amp;query=Peitzmann%2C+T">T. Peitzmann</a>, <a href="/search/?searchtype=author&amp;query=Rossewij%2C+M">M. Rossewij</a>, <a href="/search/?searchtype=author&amp;query=Shimomura%2C+M">M. Shimomura</a>, <a href="/search/?searchtype=author&amp;query=Sugitate%2C+T">T. Sugitate</a>, <a href="/search/?searchtype=author&amp;query=Suzuki%2C+T">T. Suzuki</a>, <a href="/search/?searchtype=author&amp;query=Tadokoro%2C+K">K. Tadokoro</a>, <a href="/search/?searchtype=author&amp;query=Takamura%2C+M">M. Takamura</a>, <a href="/search/?searchtype=author&amp;query=Takasu%2C+S">S. Takasu</a>, <a href="/search/?searchtype=author&amp;query=Brink%2C+A+v+d">A. van den Brink</a>, <a href="/search/?searchtype=author&amp;query=van+Leeuwen%2C+M">M. van Leeuwen</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="2306.06153v2-abstract-short" style="display: inline;"> We constructed a large-scale electromagnetic calorimeter prototype as a part of the Forward Calorimeter upgrade project (FoCal) for the ALICE experiment at the Large Hadron Collider (LHC). The prototype, also known as ``Mini FoCal&#39;&#39;, consists of 20 layers of silicon pad sensors and tungsten alloy plates with printed circuit boards and readout electronics. The constructed detector was tested at the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.06153v2-abstract-full').style.display = 'inline'; document.getElementById('2306.06153v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2306.06153v2-abstract-full" style="display: none;"> We constructed a large-scale electromagnetic calorimeter prototype as a part of the Forward Calorimeter upgrade project (FoCal) for the ALICE experiment at the Large Hadron Collider (LHC). The prototype, also known as ``Mini FoCal&#39;&#39;, consists of 20 layers of silicon pad sensors and tungsten alloy plates with printed circuit boards and readout electronics. The constructed detector was tested at the test beam facility of the Super Proton Synchrotron (SPS) at CERN. We obtain an energy resolution of about 4.3% for electron beams at both 150 and 250 GeV/$c$, which is consistent with realistic detector response simulations. Longitudinal profiles of electromagnetic shower were also measured and found to agree with the simulations. The same prototype detector was installed in the ALICE experimental area about 7.5m away from the interaction point. It was used to measure inclusive electromagnetic cluster energy distributions and neutral-pion candidate invariant mass distributions for pseudo-rapidity of $畏$=3.7-4.5 in proton-proton collisions at $\sqrt{s}$ = 13 TeV at LHC. The measured distributions in different $畏$ regions are similar to those obtained from PYTHIA simulations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2306.06153v2-abstract-full').style.display = 'none'; document.getElementById('2306.06153v2-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 March, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 9 June, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> June 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">30 pages, 27 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/2303.17254">arXiv:2303.17254</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.17254">pdf</a>, <a href="https://arxiv.org/format/2303.17254">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <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="Nuclear Theory">nucl-th</span> </div> </div> <p class="title is-5 mathjax"> Hot QCD White Paper </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Arslandok%2C+M">M. Arslandok</a>, <a href="/search/?searchtype=author&amp;query=Bass%2C+S+A">S. A. Bass</a>, <a href="/search/?searchtype=author&amp;query=Baty%2C+A+A">A. A. Baty</a>, <a href="/search/?searchtype=author&amp;query=Bautista%2C+I">I. Bautista</a>, <a href="/search/?searchtype=author&amp;query=Beattie%2C+C">C. Beattie</a>, <a href="/search/?searchtype=author&amp;query=Becattini%2C+F">F. Becattini</a>, <a href="/search/?searchtype=author&amp;query=Bellwied%2C+R">R. Bellwied</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bielcik%2C+J">J. Bielcik</a>, <a href="/search/?searchtype=author&amp;query=Blair%2C+J+T">J. T. Blair</a>, <a href="/search/?searchtype=author&amp;query=Bock%2C+F">F. Bock</a>, <a href="/search/?searchtype=author&amp;query=Boimska%2C+B">B. Boimska</a>, <a href="/search/?searchtype=author&amp;query=Bossi%2C+H">H. Bossi</a>, <a href="/search/?searchtype=author&amp;query=Caines%2C+H">H. Caines</a>, <a href="/search/?searchtype=author&amp;query=Chen%2C+Y">Y. Chen</a>, <a href="/search/?searchtype=author&amp;query=Chien%2C+Y+-">Y. -T. Chien</a>, <a href="/search/?searchtype=author&amp;query=Chiu%2C+M">M. Chiu</a>, <a href="/search/?searchtype=author&amp;query=Connors%2C+M+E">M. E. Connors</a>, <a href="/search/?searchtype=author&amp;query=Csan%C3%A1d%2C+M">M. Csan谩d</a>, <a href="/search/?searchtype=author&amp;query=da+Silva%2C+C+L">C. L. da Silva</a>, <a href="/search/?searchtype=author&amp;query=Dash%2C+A+P">A. P. Dash</a>, <a href="/search/?searchtype=author&amp;query=David%2C+G">G. David</a>, <a href="/search/?searchtype=author&amp;query=Dehmelt%2C+K">K. Dehmelt</a>, <a href="/search/?searchtype=author&amp;query=Dexheimer%2C+V">V. Dexheimer</a> , et al. (149 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2303.17254v1-abstract-short" style="display: inline;"> Hot QCD physics studies the nuclear strong force under extreme temperature and densities. Experimentally these conditions are achieved via high-energy collisions of heavy ions at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC). In the past decade, a unique and substantial suite of data was collected at RHIC and the LHC, probing hydrodynamics at the nucleon scale, the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.17254v1-abstract-full').style.display = 'inline'; document.getElementById('2303.17254v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.17254v1-abstract-full" style="display: none;"> Hot QCD physics studies the nuclear strong force under extreme temperature and densities. Experimentally these conditions are achieved via high-energy collisions of heavy ions at the Relativistic Heavy Ion Collider (RHIC) and the Large Hadron Collider (LHC). In the past decade, a unique and substantial suite of data was collected at RHIC and the LHC, probing hydrodynamics at the nucleon scale, the temperature dependence of the transport properties of quark-gluon plasma, the phase diagram of nuclear matter, the interaction of quarks and gluons at different scales and much more. This document, as part of the 2023 nuclear science long range planning process, was written to review the progress in hot QCD since the 2015 Long Range Plan for Nuclear Science, as well as highlight the realization of previous recommendations, and present opportunities for the next decade, building on the accomplishments and investments made in theoretical developments and the construction of new detectors. Furthermore, this document provides additional context to support the recommendations voted on at the Joint Hot and Cold QCD Town Hall Meeting, which are reported in a separate document. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.17254v1-abstract-full').style.display = 'none'; document.getElementById('2303.17254v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 30 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">190 pages, 69 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/2303.12899">arXiv:2303.12899</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.12899">pdf</a>, <a href="https://arxiv.org/format/2303.12899">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevLett.134.022302">10.1103/PhysRevLett.134.022302 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Disentangling centrality bias and final-state effects in the production of high-$p_T$ $蟺^0$ using direct $纬$ in $d$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Ayuso%2C+C">C. Ayuso</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Boer%2C+M">M. Boer</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a>, <a href="/search/?searchtype=author&amp;query=Butler%2C+C">C. Butler</a> , et al. (253 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2303.12899v2-abstract-short" style="display: inline;"> PHENIX presents a simultaneous measurement of the production of direct $纬$ and $蟺^0$ in $d$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV over a $p_T$ range of 7.5 to 18 GeV/$c$ for different event samples selected by event activity, i.e. charged-particle multiplicity detected at forward rapidity. Direct-photon yields are used to empirically estimate the contribution of hard-scattering processes i&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.12899v2-abstract-full').style.display = 'inline'; document.getElementById('2303.12899v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.12899v2-abstract-full" style="display: none;"> PHENIX presents a simultaneous measurement of the production of direct $纬$ and $蟺^0$ in $d$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV over a $p_T$ range of 7.5 to 18 GeV/$c$ for different event samples selected by event activity, i.e. charged-particle multiplicity detected at forward rapidity. Direct-photon yields are used to empirically estimate the contribution of hard-scattering processes in the different event samples. Using this estimate, the average nuclear-modification factor $R_{d\rm Au,EXP}^{纬^{\rm dir}}$ is $0.925{\pm}0.023({\rm stat}){\pm}0.15^{\rm (scale)}$, consistent with unity for minimum-bias (MB) $d$$+$Au events. For event classes with moderate event activity, $R_{d\rm Au,EXP}^{纬^{\rm dir}}$ is consistent with the MB value within 5\% uncertainty. These results confirm that the previously observed enhancement of high-$p_T$ $蟺^0$ production found in small-system collisions with low event activity is a result of a bias in interpreting event activity within the Glauber framework. In contrast, for the top 5\% of events with the highest event activity, $R_{d\rm Au,EXP}^{纬^{\rm dir}}$ is suppressed by 20\% relative to the MB value with a significance of $4.5蟽$, which may be due to final-state effects. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.12899v2-abstract-full').style.display = 'none'; document.getElementById('2303.12899v2-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, 2025; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 22 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">279 authors from 69 institutions, 8 pages, 3 figures, v2 is version accepted for publication in Physical Review Letters. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 134, 022302 (2025) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2303.07191">arXiv:2303.07191</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.07191">pdf</a>, <a href="https://arxiv.org/format/2303.07191">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> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.108.072016">10.1103/PhysRevD.108.072016 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Transverse single-spin asymmetry of charged hadrons at forward and backward rapidity in polarized $p$+$p$, $p$+Al, and $p$+Au collisions at $\sqrt{s_{NN}}=200$ GeV} </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a> , et al. (297 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2303.07191v2-abstract-short" style="display: inline;"> Reported here are transverse single-spin asymmetries ($A_{N}$) in the production of charged hadrons as a function of transverse momentum ($p_T$) and Feynman-$x$ ($x_F$) in polarized $p^{\uparrow}$+$p$, $p^{\uparrow}$+Al, and $p^{\uparrow}$+Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. The measurements have been performed at forward and backward rapidity ($1.4&lt;|畏|&lt;2.4$) over the range of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.07191v2-abstract-full').style.display = 'inline'; document.getElementById('2303.07191v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.07191v2-abstract-full" style="display: none;"> Reported here are transverse single-spin asymmetries ($A_{N}$) in the production of charged hadrons as a function of transverse momentum ($p_T$) and Feynman-$x$ ($x_F$) in polarized $p^{\uparrow}$+$p$, $p^{\uparrow}$+Al, and $p^{\uparrow}$+Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. The measurements have been performed at forward and backward rapidity ($1.4&lt;|畏|&lt;2.4$) over the range of $1.5&lt;p_{T}&lt;7.0~{\rm GeV}/c$ and $0.04&lt;|x_{F}|&lt;0.2$. A nonzero asymmetry is observed for positively charged hadrons at forward rapidity ($x_F&gt;0$) in $p^{\uparrow}$+$p$ collisions, whereas the $p^{\uparrow}$+Al and $p^{\uparrow}$+Au results show smaller asymmetries. This finding provides new opportunities to investigate the origin of transverse single-spin asymmetries and a tool to study nuclear effects in $p$+$A$ collisions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.07191v2-abstract-full').style.display = 'none'; document.getElementById('2303.07191v2-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 October, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 13 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">322 authors from 70 institutions, 13 pages, 9 figures, 13 tables, one appendix, 2015 data. v2 is version accepted for publication in Phys. Rev. D. HEPData tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 108, 072016 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2303.07190">arXiv:2303.07190</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2303.07190">pdf</a>, <a href="https://arxiv.org/format/2303.07190">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> </div> </div> <p class="title is-5 mathjax"> Transverse single-spin asymmetry of midrapidity $蟺^{0}$ and $畏$ mesons in $p$+Au and $p$+Al collisions at $\sqrt{s_{_{NN}}}=$ 200 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a> , et al. (297 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2303.07190v2-abstract-short" style="display: inline;"> Presented are the first measurements of the transverse single-spin asymmetries ($A_N$) for neutral pions and eta mesons in $p$+Au and $p$+Al collisions at $\sqrt{s_{_{NN}}}=200$ GeV in the pseudorapidity range $|畏|&lt;$0.35 with the PHENIX detector at the Relativistic Heavy Ion Collider. The asymmetries are consistent with zero, similar to those for midrapidity neutral pions and eta mesons produced i&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.07190v2-abstract-full').style.display = 'inline'; document.getElementById('2303.07190v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2303.07190v2-abstract-full" style="display: none;"> Presented are the first measurements of the transverse single-spin asymmetries ($A_N$) for neutral pions and eta mesons in $p$+Au and $p$+Al collisions at $\sqrt{s_{_{NN}}}=200$ GeV in the pseudorapidity range $|畏|&lt;$0.35 with the PHENIX detector at the Relativistic Heavy Ion Collider. The asymmetries are consistent with zero, similar to those for midrapidity neutral pions and eta mesons produced in $p$+$p$ collisions. These measurements show no evidence of additional effects that could potentially arise from the more complex partonic environment present in proton-nucleus collisions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2303.07190v2-abstract-full').style.display = 'none'; document.getElementById('2303.07190v2-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 June, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 13 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> March 2023. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">322 authors from 70 institutions, 8 pages, 2 figures, 1 table, 2015 data. v2 is version accepted for publication in Phys. Rev. D. HEPData tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2301.09307">arXiv:2301.09307</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2301.09307">pdf</a>, <a href="https://arxiv.org/format/2301.09307">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> </div> <p class="title is-5 mathjax"> Measurement of cosmic-ray muon spallation products in a xenon-loaded liquid scintillator with KamLAND </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Collaboration%2C+K">KamLAND-Zen Collaboration</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a> , et al. (42 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2301.09307v1-abstract-short" style="display: inline;"> Cosmic-ray muons produce various radioisotopes when passing through material. These spallation products can be backgrounds for rare event searches such as in solar neutrino, double-beta decay, and dark matter search experiments. The KamLAND-Zen experiment searches for neutrinoless double-beta decay in 745kg of xenon dissolved in liquid scintillator. The experiment includes dead-time-free electroni&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2301.09307v1-abstract-full').style.display = 'inline'; document.getElementById('2301.09307v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2301.09307v1-abstract-full" style="display: none;"> Cosmic-ray muons produce various radioisotopes when passing through material. These spallation products can be backgrounds for rare event searches such as in solar neutrino, double-beta decay, and dark matter search experiments. The KamLAND-Zen experiment searches for neutrinoless double-beta decay in 745kg of xenon dissolved in liquid scintillator. The experiment includes dead-time-free electronics with a high efficiency for detecting muon-induced neutrons. The production yields of different radioisotopes are measured with a combination of delayed coincidence techniques, newly developed muon reconstruction and xenon spallation identification methods. The observed xenon spallation products are consistent with results from the FLUKA and Geant4 simulation codes. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2301.09307v1-abstract-full').style.display = 'none'; document.getElementById('2301.09307v1-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, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2023. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2211.13911">arXiv:2211.13911</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2211.13911">pdf</a>, <a href="https://arxiv.org/format/2211.13911">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> </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.107.072006">10.1103/PhysRevD.107.072006 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> First measurement of the strange axial coupling constant using neutral-current quasielastic interactions of atmospheric neutrinos at KamLAND </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=KamLAND+Collaboration"> KamLAND Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakahata%2C+T">T. Nakahata</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a> , et al. (39 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="2211.13911v2-abstract-short" style="display: inline;"> We report a measurement of the strange axial coupling constant $g_A^s$ using atmospheric neutrino data at KamLAND. This constant is a component of the axial form factor of the neutral-current quasielastic (NCQE) interaction. The value of $g_A^s$ significantly changes the ratio of proton and neutron NCQE cross sections. KamLAND is suitable for measuring NCQE interactions as it can detect nucleon re&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2211.13911v2-abstract-full').style.display = 'inline'; document.getElementById('2211.13911v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2211.13911v2-abstract-full" style="display: none;"> We report a measurement of the strange axial coupling constant $g_A^s$ using atmospheric neutrino data at KamLAND. This constant is a component of the axial form factor of the neutral-current quasielastic (NCQE) interaction. The value of $g_A^s$ significantly changes the ratio of proton and neutron NCQE cross sections. KamLAND is suitable for measuring NCQE interactions as it can detect nucleon recoils with low-energy thresholds and measure neutron multiplicity with high efficiency. KamLAND data, including the information on neutron multiplicity associated with the NCQE interactions, makes it possible to measure $g_A^s$ with a suppressed dependence on the axial mass $M_A$, which has not yet been determined. For a comprehensive prediction of the neutron emission associated with neutrino interactions, we establish a simulation of particle emission via nuclear deexcitation of $^{12}$C, a process not considered in existing neutrino Monte Carlo event generators. Energy spectrum fitting for each neutron multiplicity gives $g_A^s =-0.14^{+0.25}_{-0.26}$, which is the most stringent limit obtained using NCQE interactions without $M_A$ constraints. The two-body current contribution considered in this analysis relies on a theoretically effective model and electron scattering experiments and requires future verification by direct measurements and future model improvement. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2211.13911v2-abstract-full').style.display = 'none'; document.getElementById('2211.13911v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 April, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 25 November, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 107,072006 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2207.10745">arXiv:2207.10745</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2207.10745">pdf</a>, <a href="https://arxiv.org/format/2207.10745">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.107.014907">10.1103/PhysRevC.107.014907 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of $蠁$-meson production in Cu$+$Au at $\sqrt{s_{_{NN}}}=200$ GeV and U$+$U at $\sqrt{s_{_{NN}}}=193$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Alibordi%2C+M">M. Alibordi</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+X">X. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Baublis%2C+V">V. Baublis</a>, <a href="/search/?searchtype=author&amp;query=Baumann%2C+C">C. Baumann</a>, <a href="/search/?searchtype=author&amp;query=Baumgart%2C+S">S. Baumgart</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a> , et al. (387 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2207.10745v2-abstract-short" style="display: inline;"> The PHENIX experiment reports systematic measurements at the Relativistic Heavy Ion Collider of $蠁$-meson production in asymmetric Cu$+$Au collisions at $\sqrt{s_{_{NN}}}$=200 GeV and in U$+$U collisions at $\sqrt{s_{_{NN}}}$=193 GeV. Measurements were performed via the $蠁\rightarrow K^{+}K^{-}$ decay channel at midrapidity $|畏|&lt;0.35$. Features of $蠁$-meson production measured in Cu$+$Cu, Cu$+$Au,&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.10745v2-abstract-full').style.display = 'inline'; document.getElementById('2207.10745v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2207.10745v2-abstract-full" style="display: none;"> The PHENIX experiment reports systematic measurements at the Relativistic Heavy Ion Collider of $蠁$-meson production in asymmetric Cu$+$Au collisions at $\sqrt{s_{_{NN}}}$=200 GeV and in U$+$U collisions at $\sqrt{s_{_{NN}}}$=193 GeV. Measurements were performed via the $蠁\rightarrow K^{+}K^{-}$ decay channel at midrapidity $|畏|&lt;0.35$. Features of $蠁$-meson production measured in Cu$+$Cu, Cu$+$Au, Au$+$Au, and U$+$U collisions were found to not depend on the collision geometry, which was expected because the yields are averaged over the azimuthal angle and follow the expected scaling with nuclear-overlap size. The elliptic flow of the $蠁$ meson in Cu$+$Au, Au$+$Au, and U$+$U collisions scales with second-order-participant eccentricity and the length scale of the nuclear-overlap region (estimated with the number of participating nucleons). At moderate $p_T$, $蠁$-meson production measured in Cu$+$Au and U$+$U collisions is consistent with coalescence-model predictions, whereas at high $p_T$ the production is in agreement with expectations for in-medium energy loss of parent partons prior to their fragmentation. The elliptic flow for $蠁$ mesons measured in Cu$+$Au and U$+$U collisions is well described by a (2+1)D viscous-hydrodynamic model with specific-shear viscosity $畏/s=1/4蟺$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.10745v2-abstract-full').style.display = 'none'; document.getElementById('2207.10745v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 13 January, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 21 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">412 authors from 76 institutions, 16 pages, 12 figures, 9 tables, 2012 data. v2 is version accepted for publication by Physical Review C. HEPdata for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 107, 014907 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2205.14934">arXiv:2205.14934</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2205.14934">pdf</a>, <a href="https://arxiv.org/format/2205.14934">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Geophysics">physics.geo-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/10.1029/2022GL099566">10.1029/2022GL099566 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Abundances of uranium and thorium elements in Earth estimated by geoneutrino spectroscopy </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakahata%2C+T">T. Nakahata</a> , et al. (43 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="2205.14934v2-abstract-short" style="display: inline;"> The decay of the primordial isotopes $^{238}\mathrm{U}$, $^{235}\mathrm{U}$, $^{232}\mathrm{Th}$, and $^{40}\mathrm{K}$ have contributed to the terrestrial heat budget throughout the Earth&#39;s history. Hence the individual abundance of those isotopes are key parameters in reconstructing contemporary Earth model. The geoneutrinos produced by the radioactive decays of uranium and thorium have been obs&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.14934v2-abstract-full').style.display = 'inline'; document.getElementById('2205.14934v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2205.14934v2-abstract-full" style="display: none;"> The decay of the primordial isotopes $^{238}\mathrm{U}$, $^{235}\mathrm{U}$, $^{232}\mathrm{Th}$, and $^{40}\mathrm{K}$ have contributed to the terrestrial heat budget throughout the Earth&#39;s history. Hence the individual abundance of those isotopes are key parameters in reconstructing contemporary Earth model. The geoneutrinos produced by the radioactive decays of uranium and thorium have been observed with the Kamioka Liquid-Scintillator Antineutrino Detector (KamLAND). Those measurements have been improved with more than 18-year observation time, and improvements in detector background levels mainly by an 8-year almost rector-free period now permit spectroscopy with geoneutrinos. Our results yield the first constraint on both uranium and thorium heat contributions. Herein the KamLAND result is consistent with geochemical estimations based on elemental abundances of chondritic meteorites and mantle peridotites. The High-Q model is disfavored at 99.76% C.L. and a fully radiogenic model is excluded at 5.2$蟽$ assuming a homogeneous heat producing element distribution in the mantle. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2205.14934v2-abstract-full').style.display = 'none'; document.getElementById('2205.14934v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 13 August, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 30 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">13 pages, 2 figures, accepted for publication in Geophysical Research Letters on Aug 4th, 2022</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Geophysical Research Letters, Volume 49, Issue 16, e2022GL099566 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2204.12899">arXiv:2204.12899</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2204.12899">pdf</a>, <a href="https://arxiv.org/format/2204.12899">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> </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.107.052012">10.1103/PhysRevD.107.052012 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Improving constraints on gluon spin-momentum correlations in transversely polarized protons via midrapidity open-heavy-flavor electrons in $p^{\uparrow}+p$ collisions at $\sqrt{s}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a> , et al. (299 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2204.12899v2-abstract-short" style="display: inline;"> Polarized proton-proton collisions provide leading-order access to gluons, presenting an opportunity to constrain gluon spin-momentum correlations within transversely polarized protons and enhance our understanding of the three-dimensional structure of the proton. Midrapidity open-heavy-flavor production at $\sqrt{s}=200$ GeV is dominated by gluon-gluon fusion, providing heightened sensitivity to&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.12899v2-abstract-full').style.display = 'inline'; document.getElementById('2204.12899v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2204.12899v2-abstract-full" style="display: none;"> Polarized proton-proton collisions provide leading-order access to gluons, presenting an opportunity to constrain gluon spin-momentum correlations within transversely polarized protons and enhance our understanding of the three-dimensional structure of the proton. Midrapidity open-heavy-flavor production at $\sqrt{s}=200$ GeV is dominated by gluon-gluon fusion, providing heightened sensitivity to gluon dynamics relative to other production channels. Transverse single-spin asymmetries of positrons and electrons from heavy-flavor hadron decays are measured at midrapidity using the PHENIX detector at the Relativistic Heavy Ion Collider. These charge-separated measurements are sensitive to gluon correlators that can in principle be related to gluon orbital angular momentum via model calculations. Explicit constraints on gluon correlators are extracted for two separate models, one of which had not been constrained previously. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.12899v2-abstract-full').style.display = 'none'; document.getElementById('2204.12899v2-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> 7 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 27 April, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">324 authors from 70 institutions, 11 pages, 5 figures, 3 tables, 2015 data. v2 is version accepted for publication in PRD. HEPData tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2204.12065">arXiv:2204.12065</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2204.12065">pdf</a>, <a href="https://arxiv.org/format/2204.12065">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="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/10.3847/1538-4357/ac7a3f">10.3847/1538-4357/ac7a3f <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for supernova neutrinos and constraint on the galactic star formation rate with the KamLAND data </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakahata%2C+T">T. Nakahata</a> , et al. (42 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2204.12065v3-abstract-short" style="display: inline;"> We present the results of a search for core-collapse supernova neutrinos, using long-term KamLAND data from 2002 March 9 to 2020 April 25. We focus on the electron antineutrinos emitted from supernovae in the energy range of 1.8--111 MeV. Supernovae will make a neutrino event cluster with the duration of $\sim$10 s in the KamLAND data. We find no neutrino clusters and give the upper limit on the s&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.12065v3-abstract-full').style.display = 'inline'; document.getElementById('2204.12065v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2204.12065v3-abstract-full" style="display: none;"> We present the results of a search for core-collapse supernova neutrinos, using long-term KamLAND data from 2002 March 9 to 2020 April 25. We focus on the electron antineutrinos emitted from supernovae in the energy range of 1.8--111 MeV. Supernovae will make a neutrino event cluster with the duration of $\sim$10 s in the KamLAND data. We find no neutrino clusters and give the upper limit on the supernova rate as to be 0.15 yr$^{-1}$ with a 90% confidence level. The detectable range, which corresponds to a &gt;95% detection probability, is 40--59 kpc and 65--81 kpc for core-collapse supernovae and failed core-collapse supernovae, respectively. This paper proposes to convert the supernova rate obtained by the neutrino observation to the Galactic star formation rate. Assuming a modified Salpeter-type initial mass function, the upper limit on the Galactic star formation rate is &lt;(17.5--22.7) $M_{\odot} \mathrm{yr}^{-1}$ with a 90% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2204.12065v3-abstract-full').style.display = 'none'; document.getElementById('2204.12065v3-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 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 April, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">10 pages, 4 figures, accepted for publication in Astrophysical Journal</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> The Astrophysical Journal, Volume 934, Number 1, Page 85 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.17187">arXiv:2203.17187</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.17187">pdf</a>, <a href="https://arxiv.org/format/2203.17187">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.109.044912">10.1103/PhysRevC.109.044912 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Nonprompt direct-photon production in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a> , et al. (311 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="2203.17187v2-abstract-short" style="display: inline;"> The measurement of the direct-photon spectrum from Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV is presented by the PHENIX collaboration using the external-photon-conversion technique for 0\%--93\% central collisions in a transverse-momentum ($p_T$) range of 0.8--10 GeV/$c$. An excess of direct photons, above prompt-photon production from hard-scattering processes, is observed for $p_T&lt;6$ GeV/&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.17187v2-abstract-full').style.display = 'inline'; document.getElementById('2203.17187v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.17187v2-abstract-full" style="display: none;"> The measurement of the direct-photon spectrum from Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV is presented by the PHENIX collaboration using the external-photon-conversion technique for 0\%--93\% central collisions in a transverse-momentum ($p_T$) range of 0.8--10 GeV/$c$. An excess of direct photons, above prompt-photon production from hard-scattering processes, is observed for $p_T&lt;6$ GeV/$c$. Nonprompt direct photons are measured by subtracting the prompt component, which is estimated as $N_{\rm coll}$-scaled direct photons from $p$$+$$p$ collisions at 200 GeV, from the direct-photon spectrum. Results are obtained for $0.8&lt;p_T&lt;6.0$ GeV/$c$ and suggest that the spectrum has an increasing inverse slope from ${\approx}0.2$ to 0.4 GeV/$c$ with increasing $p_T$, which indicates a possible sensitivity of the measurement to photons from earlier stages of the evolution of the collision. In addition, like the direct-photon production, the $p_T$-integrated nonprompt direct-photon yields also follow a power-law scaling behavior as a function of collision-system size. The exponent, $伪$, for the nonprompt component is found to be consistent with 1.1 with no apparent $p_T$ dependence. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.17187v2-abstract-full').style.display = 'none'; document.getElementById('2203.17187v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 April, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 31 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">336 authors from 71 institutions, 26 pages, 30 figures, 4 tabels, 2014 data. v2 is version accepted for publication in Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 109, 044912 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.17058">arXiv:2203.17058</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.17058">pdf</a>, <a href="https://arxiv.org/format/2203.17058">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.109.044907">10.1103/PhysRevC.109.044907 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Charm- and Bottom-Quark Production in Au$+$Au Collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a> , et al. (321 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="2203.17058v2-abstract-short" style="display: inline;"> The invariant yield of electrons from open-heavy-flavor decays for $1&lt;p_T&lt;8$ GeV/$c$ at midrapidity $|y|&lt;0.35$ in Au$+$Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV has been measured by the PHENIX experiment at the Relativistic Heavy Ion Collider. A displaced-vertex analysis with the PHENIX silicon-vertex detector enables extraction of the fraction of charm and bottom hadron decays and unfolding o&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.17058v2-abstract-full').style.display = 'inline'; document.getElementById('2203.17058v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.17058v2-abstract-full" style="display: none;"> The invariant yield of electrons from open-heavy-flavor decays for $1&lt;p_T&lt;8$ GeV/$c$ at midrapidity $|y|&lt;0.35$ in Au$+$Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV has been measured by the PHENIX experiment at the Relativistic Heavy Ion Collider. A displaced-vertex analysis with the PHENIX silicon-vertex detector enables extraction of the fraction of charm and bottom hadron decays and unfolding of the invariant yield of parent charm and bottom hadrons. The nuclear-modification factors $R_{AA}$ for electrons from charm and bottom hadron decays and heavy-flavor hadrons show both a centrality and a quark-mass dependence, indicating suppression in the quark-gluon plasma produced in these collisions that is medium sized and quark-mass dependent. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.17058v2-abstract-full').style.display = 'none'; document.getElementById('2203.17058v2-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 April, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 31 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">345 authors from 72 institutions, 16 pages, 18 figures, 2014 data. v2 is version accepted for publication in Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 109, 044907 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.12354">arXiv:2203.12354</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.12354">pdf</a>, <a href="https://arxiv.org/format/2203.12354">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.107.024914">10.1103/PhysRevC.107.024914 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Low-$p_T$ direct-photon production in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=39$ and 62.4 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Al-Ta%27ani%2C+H">H. Al-Ta&#39;ani</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Angerami%2C+A">A. Angerami</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Aschenauer%2C+E+C">E. C. Aschenauer</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bassalleck%2C+B">B. Bassalleck</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a> , et al. (409 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="2203.12354v2-abstract-short" style="display: inline;"> The measurement of direct photons from Au$+$Au collisions at $\sqrt{s_{_{NN}}}=39$ and 62.4 GeV in the transverse-momentum range $0.4&lt;p_T&lt;3$ Gev/$c$ is presented by the PHENIX collaboration at the Relativistic Heavy Ion Collider. A significant direct-photon yield is observed in both collision systems. A universal scaling is observed when the direct-photon $p_T$ spectra for different center-of-mass&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.12354v2-abstract-full').style.display = 'inline'; document.getElementById('2203.12354v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.12354v2-abstract-full" style="display: none;"> The measurement of direct photons from Au$+$Au collisions at $\sqrt{s_{_{NN}}}=39$ and 62.4 GeV in the transverse-momentum range $0.4&lt;p_T&lt;3$ Gev/$c$ is presented by the PHENIX collaboration at the Relativistic Heavy Ion Collider. A significant direct-photon yield is observed in both collision systems. A universal scaling is observed when the direct-photon $p_T$ spectra for different center-of-mass energies and for different centrality selections at $\sqrt{s_{_{NN}}}=62.4$ GeV is scaled with $(dN_{\rm ch}/d畏)^伪$ for $伪=1.21{\pm}0.04$. This scaling also holds true for direct-photon spectra from Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV measured earlier by PHENIX, as well as the spectra from Pb$+$Pb at $\sqrt{s_{_{NN}}}=2760$ GeV published by ALICE. The scaling power $伪$ seems to be independent of $p_T$, center of mass energy, and collision centrality. The spectra from different collision energies have a similar shape up to $p_T$ of 2 GeV/$c$. The spectra have a local inverse slope $T_{\rm eff}$ increasing with $p_T$ of $0.174\pm0.018$ GeV/$c$ in the range $0.4&lt;p_T&lt;1.3$ GeV/$c$ and increasing to $0.289\pm0.024$ GeV/$c$ for $0.9&lt;p_T&lt;2.1$ GeV/$c$. The observed similarity of low-$p_T$ direct-photon production from $\sqrt{s_{_{NN}}}= 39$ to 2760 GeV suggests a common source of direct photons for the different collision energies and event centrality selections, and suggests a comparable space-time evolution of direct-photon emission. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.12354v2-abstract-full').style.display = 'none'; document.getElementById('2203.12354v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 February, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 23 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">434 authors from 78 institutions, 19 pages, 16 figures, 4 tables. v2 is version accepted for publication in Physical Review C as an Editor&#39;s Suggestion. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 107, 024914 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.09894">arXiv:2203.09894</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.09894">pdf</a>, <a href="https://arxiv.org/format/2203.09894">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.107.024907">10.1103/PhysRevC.107.024907 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurements of second-harmonic Fourier coefficients from azimuthal anisotropies in $p$$+$$p$, $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Ayuso%2C+C">C. Ayuso</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a> , et al. (368 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="2203.09894v2-abstract-short" style="display: inline;"> Recently, the PHENIX Collaboration has published second- and third-harmonic Fourier coefficients $v_2$ and $v_3$ for midrapidity ($|畏|&lt;0.35$) charged hadrons in 0\%--5\% central $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV utilizing three sets of two-particle correlations for two detector combinations with different pseudorapidity acceptance [Phys. Rev. C {\bf 105},&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.09894v2-abstract-full').style.display = 'inline'; document.getElementById('2203.09894v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.09894v2-abstract-full" style="display: none;"> Recently, the PHENIX Collaboration has published second- and third-harmonic Fourier coefficients $v_2$ and $v_3$ for midrapidity ($|畏|&lt;0.35$) charged hadrons in 0\%--5\% central $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV utilizing three sets of two-particle correlations for two detector combinations with different pseudorapidity acceptance [Phys. Rev. C {\bf 105}, 024901 (2022)]. This paper extends these measurements of $v_2$ to all centralities in $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions, as well as $p$$+$$p$ collisions, as a function of transverse momentum ($p_T$) and event multiplicity. The kinematic dependence of $v_2$ is quantified as the ratio $R$ of $v_2$ between the two detector combinations as a function of event multiplicity for $0.5$$&lt;$$p_T$$&lt;$$1$ and $2$$&lt;$$p_T$$&lt;$$2.5$ GeV/$c$. A multiphase-transport (AMPT) model can reproduce the observed $v_2$ in most-central to midcentral $d$$+$Au and $^3$He$+$Au collisions. However, the AMPT model systematically overestimates the measurements in $p$$+$$p$, $p$$+$Au, and peripheral $d$$+$Au and $^3$He$+$Au collisions, indicating a higher nonflow contribution in AMPT than in the experimental data. The AMPT model fails to describe the observed $R$ for $0.5$$&lt;$$p_T$$&lt;$$1$ GeV/$c$, but there is qualitative agreement with the measurements for $2$$&lt;$$p_T$$&lt;$$2.5$ GeV/$c$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.09894v2-abstract-full').style.display = 'none'; document.getElementById('2203.09894v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 March, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 18 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">393 authors from 72 institutions, 14 pages, 10 figures, 2014, 2015, and 2016 data. v2 is version accepted for publication in Physical Review C. HEPdata tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 107, 024907 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.06087">arXiv:2203.06087</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.06087">pdf</a>, <a href="https://arxiv.org/format/2203.06087">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.106.014908">10.1103/PhysRevC.106.014908 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Study of $蠁$-meson production in $p$$+$Al, $p$$+$Au, $d$$+$Au, and $^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a> , et al. (346 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="2203.06087v2-abstract-short" style="display: inline;"> Small nuclear collisions are mainly sensitive to cold-nuclear-matter effects; however, the collective behavior observed in these collisions shows a hint of hot-nuclear-matter effects. The identified-particle spectra, especially the $蠁$ mesons which contain strange and antistrange quarks and have a relatively small hadronic-interaction cross section, are a good tool to study these effects. The PHEN&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.06087v2-abstract-full').style.display = 'inline'; document.getElementById('2203.06087v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.06087v2-abstract-full" style="display: none;"> Small nuclear collisions are mainly sensitive to cold-nuclear-matter effects; however, the collective behavior observed in these collisions shows a hint of hot-nuclear-matter effects. The identified-particle spectra, especially the $蠁$ mesons which contain strange and antistrange quarks and have a relatively small hadronic-interaction cross section, are a good tool to study these effects. The PHENIX experiment has measured $蠁$ mesons in a specific set of small collision systems $p$$+$Al, $p$$+$Au, and $^3$He$+$Au, as well as $d$$+$Au [Phys. Rev. C {\bf 83}, 024909 (2011)], at $\sqrt{s_{_{NN}}}=200$ GeV. The transverse-momentum spectra and nuclear-modification factors are presented and compared to theoretical-model predictions. The comparisons with different calculations suggest that quark-gluon plasma may be formed in these small collision systems at $\sqrt{s_{_{NN}}}=200$ GeV. However, the volume and the lifetime of the produced medium may be insufficient for observing strangeness-enhancement and jet-quenching effects. Comparison with calculations suggests that the main production mechanisms of $蠁$ mesons at midrapidity may be different in $p$$+$Al versus $p/d/$$^3$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. While thermal quark recombination seems to dominate in $p/d/$$^3$He$+$Au collisions, fragmentation seems to be the main production mechanism in $p$$+$Al collisions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.06087v2-abstract-full').style.display = 'none'; document.getElementById('2203.06087v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 26 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 11 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">371 authors from 72 institutions, 13 pages, 7 figures, 7 tables, 2014 and 2015 data. v2 is version accepted for publication Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 106, 014908 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2203.02139">arXiv:2203.02139</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2203.02139">pdf</a>, <a href="https://arxiv.org/format/2203.02139">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevLett.130.051801">10.1103/PhysRevLett.130.051801 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for the Majorana Nature of Neutrinos in the Inverted Mass Ordering Region with KamLAND-Zen </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Collaboration%2C+K">KamLAND-Zen Collaboration</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hayashida%2C+S">S. Hayashida</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a> , et al. (50 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="2203.02139v2-abstract-short" style="display: inline;"> The KamLAND-Zen experiment has provided stringent constraints on the neutrinoless double-beta ($0谓尾尾$) decay half-life in $^{136}$Xe using a xenon-loaded liquid scintillator. We report an improved search using an upgraded detector with almost double the amount of xenon and an ultralow radioactivity container, corresponding to an exposure of 970 kg yr of $^{136}$Xe. These new data provide valuable&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.02139v2-abstract-full').style.display = 'inline'; document.getElementById('2203.02139v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2203.02139v2-abstract-full" style="display: none;"> The KamLAND-Zen experiment has provided stringent constraints on the neutrinoless double-beta ($0谓尾尾$) decay half-life in $^{136}$Xe using a xenon-loaded liquid scintillator. We report an improved search using an upgraded detector with almost double the amount of xenon and an ultralow radioactivity container, corresponding to an exposure of 970 kg yr of $^{136}$Xe. These new data provide valuable insight into backgrounds, especially from cosmic muon spallation of xenon, and have required the use of novel background rejection techniques. We obtain a lower limit for the $0谓尾尾$ decay half-life of $T_{1/2}^{0谓} &gt; 2.3 \times 10^{26}$ yr at 90% C.L., corresponding to upper limits on the effective Majorana neutrino mass of 36-156 meV using commonly adopted nuclear matrix element calculations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2203.02139v2-abstract-full').style.display = 'none'; document.getElementById('2203.02139v2-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 February, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 4 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">7 pages, 3 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 130, 051801 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.08158">arXiv:2202.08158</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.08158">pdf</a>, <a href="https://arxiv.org/format/2202.08158">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </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.130.251901">10.1103/PhysRevLett.130.251901 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of Direct-Photon Cross Section and Double-Helicity Asymmetry at $\sqrt{s}=510$ GeV in $\vec{p}+\vec{p}$ Collisions </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=PHENIX+Collaboration"> PHENIX Collaboration</a>, <a href="/search/?searchtype=author&amp;query=Abdulameer%2C+N+J">N. J. Abdulameer</a>, <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a> , et al. (336 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2202.08158v2-abstract-short" style="display: inline;"> We present measurements of the cross section and double-helicity asymmetry $A_{LL}$ of direct-photon production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=510$ GeV. The measurements have been performed at midrapidity ($|畏|&lt;0.25$) with the PHENIX detector at the Relativistic Heavy Ion Collider. At relativistic energies, direct photons are dominantly produced from the initial quark-gluon hard scat&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.08158v2-abstract-full').style.display = 'inline'; document.getElementById('2202.08158v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.08158v2-abstract-full" style="display: none;"> We present measurements of the cross section and double-helicity asymmetry $A_{LL}$ of direct-photon production in $\vec{p}+\vec{p}$ collisions at $\sqrt{s}=510$ GeV. The measurements have been performed at midrapidity ($|畏|&lt;0.25$) with the PHENIX detector at the Relativistic Heavy Ion Collider. At relativistic energies, direct photons are dominantly produced from the initial quark-gluon hard scattering and do not interact via the strong force at leading order. Therefore, at $\sqrt{s}=510$ GeV, where leading-order-effects dominate, these measurements provide clean and direct access to the gluon helicity in the polarized proton in the gluon-momentum-fraction range $0.02&lt;x&lt;0.08$, with direct sensitivity to the sign of the gluon contribution. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.08158v2-abstract-full').style.display = 'none'; document.getElementById('2202.08158v2-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 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 16 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">358 authors from 72 institutions, 8 pages, 2 figures, 1 table, 2013 data. v2 is version accepted by Physical Review Letters. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.07345">arXiv:2202.07345</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.07345">pdf</a>, <a href="https://arxiv.org/format/2202.07345">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> </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.astropartphys.2022.102758">10.1016/j.astropartphys.2022.102758 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> KamLAND&#39;s search for correlated low-energy electron antineutrinos with astrophysical neutrinos from IceCube </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Eizuka%2C+M">M. Eizuka</a>, <a href="/search/?searchtype=author&amp;query=Futagi%2C+S">S. Futagi</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Kinoshita%2C+T">T. Kinoshita</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Kurasawa%2C+M">M. Kurasawa</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a> , et al. (45 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2202.07345v2-abstract-short" style="display: inline;"> We report the results of a search for MeV-scale astrophysical neutrinos in KamLAND presented as an excess in the number of coincident neutrino interactions associated with the publicly available high-energy neutrino datasets from the IceCube Neutrino Observatory. We find no statistically significant excess in the number of observed low-energy electron antineutrinos in KamLAND, given a coincidence&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.07345v2-abstract-full').style.display = 'inline'; document.getElementById('2202.07345v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.07345v2-abstract-full" style="display: none;"> We report the results of a search for MeV-scale astrophysical neutrinos in KamLAND presented as an excess in the number of coincident neutrino interactions associated with the publicly available high-energy neutrino datasets from the IceCube Neutrino Observatory. We find no statistically significant excess in the number of observed low-energy electron antineutrinos in KamLAND, given a coincidence time window of $\pm$500s, $\pm$1,000s, $\pm$3,600s, and $\pm$10,000s around each of the IceCube neutrinos. We use this observation to present limits from 1.8 MeV to 100 MeV on the electron antineutrino fluence, assuming a mono-energetic flux. We then compare the results to several astrophysical measurements performed by IceCube and place a limit at the 90% confidence level on the electron antineutrino isotropic thermal luminosity from the TXS 0506+056 blazar. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.07345v2-abstract-full').style.display = 'none'; document.getElementById('2202.07345v2-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> 21 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 15 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">12 pages, 5 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.03863">arXiv:2202.03863</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.03863">pdf</a>, <a href="https://arxiv.org/format/2202.03863">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.105.064912">10.1103/PhysRevC.105.064912 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of $蠄(2S)$ nuclear modification at backward and forward rapidity in $p$$+$$p$, $p$$+$Al, and $p$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a> , et al. (291 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2202.03863v2-abstract-short" style="display: inline;"> Suppression of the $J/蠄$ nuclear-modification factor has been seen as a trademark signature of final-state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold-nuclear-matter effects until the observation of strong differential suppression of the $蠄(2S)$ state in $p/d$$+$$A$ collisions suggested the presence of final-state effects. Resul&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.03863v2-abstract-full').style.display = 'inline'; document.getElementById('2202.03863v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.03863v2-abstract-full" style="display: none;"> Suppression of the $J/蠄$ nuclear-modification factor has been seen as a trademark signature of final-state effects in large collision systems for decades. In small systems, the nuclear modification was attributed to cold-nuclear-matter effects until the observation of strong differential suppression of the $蠄(2S)$ state in $p/d$$+$$A$ collisions suggested the presence of final-state effects. Results of $J/蠄$ and $蠄(2S)$ measurements in the dimuon decay channel are presented here for $p$$+$$p$, $p$$+$Al, and $p$$+$Au collision systems at $\sqrt{s_{_{NN}}}=200$ GeV. The results are predominantly shown in the form of the nuclear-modification factor, $R_{pA}$, the ratio of the $蠄(2S)$ invariant yield per nucleon-nucleon collision in collisions of proton on target nucleus to that in $p$$+$$p$ collisions. Measurements of the $J/蠄$ and $蠄(2S)$ nuclear-modification factor are compared with shadowing and transport-model predictions, as well as to complementary measurements at Large-Hadron-Collider energies. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.03863v2-abstract-full').style.display = 'none'; document.getElementById('2202.03863v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 30 June, 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">Comments:</span> <span class="has-text-grey-dark mathjax">315 authors from 69 institutions, 16 pages, 9 figures, 4 tables, 2015 data. v2 is version accepted for publication in Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 105, 064912 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2112.05680">arXiv:2112.05680</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2112.05680">pdf</a>, <a href="https://arxiv.org/format/2112.05680">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </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.105.032003">10.1103/PhysRevD.105.032003 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Transverse-single-spin asymmetries of charged pions at midrapidity in transversely polarized $p{+}p$ collisions at $\sqrt{s}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a> , et al. (286 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2112.05680v2-abstract-short" style="display: inline;"> In 2015, the PHENIX collaboration has measured single-spin asymmetries for charged pions in transversely polarized proton-proton collisions at the center of mass energy of $\sqrt{s}=200$ GeV. The pions were detected at central rapidities of $|畏|&lt;0.35$. The single-spin asymmetries are consistent with zero for each charge individually, as well as consistent with the previously published neutral-pion&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.05680v2-abstract-full').style.display = 'inline'; document.getElementById('2112.05680v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2112.05680v2-abstract-full" style="display: none;"> In 2015, the PHENIX collaboration has measured single-spin asymmetries for charged pions in transversely polarized proton-proton collisions at the center of mass energy of $\sqrt{s}=200$ GeV. The pions were detected at central rapidities of $|畏|&lt;0.35$. The single-spin asymmetries are consistent with zero for each charge individually, as well as consistent with the previously published neutral-pion asymmetries in the same rapidity range. However, they show a slight indication of charge-dependent differences which may suggest a flavor dependence in the underlying mechanisms that create these asymmetries. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.05680v2-abstract-full').style.display = 'none'; document.getElementById('2112.05680v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 10 December, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">311 authors from 68 institutions, 8 pages, 3 figures, 1 table. 2015 data. v2 is version accepted for publication in Physical Review D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 105, 032003 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2112.04918">arXiv:2112.04918</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2112.04918">pdf</a>, <a href="https://arxiv.org/format/2112.04918">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="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/10.3847/1538-4357/ac4e7e">10.3847/1538-4357/ac4e7e <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> A search for correlated low-energy electron antineutrinos in KamLAND with gamma-ray bursts </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Kinoshita%2C+T">T. Kinoshita</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+R">R. Nakamura</a> , et al. (43 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2112.04918v2-abstract-short" style="display: inline;"> We present the results of a time-coincident event search for low-energy electron antineutrinos in the KamLAND detector with gamma-ray bursts from the Gamma-ray Coordinates Network and Fermi Gamma-ray Burst Monitor. Using a variable coincidence time window of $\pm$500s plus the duration of each gamma-ray burst, no statistically significant excess above background is observed. We place the world&#39;s m&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.04918v2-abstract-full').style.display = 'inline'; document.getElementById('2112.04918v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2112.04918v2-abstract-full" style="display: none;"> We present the results of a time-coincident event search for low-energy electron antineutrinos in the KamLAND detector with gamma-ray bursts from the Gamma-ray Coordinates Network and Fermi Gamma-ray Burst Monitor. Using a variable coincidence time window of $\pm$500s plus the duration of each gamma-ray burst, no statistically significant excess above background is observed. We place the world&#39;s most stringent 90% confidence level upper limit on the electron antineutrino fluence below 17.5 MeV. Assuming a Fermi-Dirac neutrino energy spectrum from the gamma-ray burst source, we use the available redshift data to constrain the electron antineutrino luminosity and effective temperature. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2112.04918v2-abstract-full').style.display = 'none'; document.getElementById('2112.04918v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 9 December, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">9 pages, 3 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/2111.05756">arXiv:2111.05756</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2111.05756">pdf</a>, <a href="https://arxiv.org/format/2111.05756">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.105.064902">10.1103/PhysRevC.105.064902 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Systematic study of nuclear effects in $p$$+$Al, $p$$+$Au, $d$$+$Au, and $^{3}$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV using $蟺^0$ production </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Al-Bataineh%2C+H">H. Al-Bataineh</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Angerami%2C+A">A. Angerami</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Averbeck%2C+R">R. Averbeck</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Baksay%2C+G">G. Baksay</a>, <a href="/search/?searchtype=author&amp;query=Baksay%2C+L">L. Baksay</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a> , et al. (529 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2111.05756v2-abstract-short" style="display: inline;"> The PHENIX collaboration presents a systematic study of $蟺^0$ production from $p$$+$$p$, $p$$+$Al, $p$$+$Au, $d$$+$Au, and $^{3}$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. Measurements were performed with different centrality selections as well as the total inelastic, 0%--100%, selection for all collision systems. For 0%--100% collisions, the nuclear modification factors, $R_{xA}$, are cons&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.05756v2-abstract-full').style.display = 'inline'; document.getElementById('2111.05756v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2111.05756v2-abstract-full" style="display: none;"> The PHENIX collaboration presents a systematic study of $蟺^0$ production from $p$$+$$p$, $p$$+$Al, $p$$+$Au, $d$$+$Au, and $^{3}$He$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. Measurements were performed with different centrality selections as well as the total inelastic, 0%--100%, selection for all collision systems. For 0%--100% collisions, the nuclear modification factors, $R_{xA}$, are consistent with unity for $p_T$ above 8 GeV/$c$, but exhibit an enhancement in peripheral collisions and a suppression in central collisions. The enhancement and suppression characteristics are similar for all systems for the same centrality class. It is shown that for high-$p_T$-$蟺^0$ production, the nucleons in the $d$ and $^3$He interact mostly independently with the Au nucleus and that the counter intuitive centrality dependence is likely due to a physical correlation between multiplicity and the presence of a hard scattering process. These observations disfavor models where parton energy loss has a significant contribution to nuclear modifications in small systems. Nuclear modifications at lower $p_T$ resemble the Cronin effect -- an increase followed by a peak in central or inelastic collisions and a plateau in peripheral collisions. The peak height has a characteristic ordering by system size as $p$$+$Au $&gt;$ $d$$+$Au $&gt;$ $^{3}$He$+$Au $&gt;$ $p$$+$Al. For collisions with Au ions, current calculations based on initial state cold nuclear matter effects result in the opposite order, suggesting the presence of other contributions to nuclear modifications, in particular at lower $p_T$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2111.05756v2-abstract-full').style.display = 'none'; document.getElementById('2111.05756v2-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 June, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 10 November, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">554 authors from 81 institutions, 21 pages, 13 figures, and 3 tables. Data from 2008, 2014, and 2015. v2 is version accepted for publication in Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 105, 064902 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2110.07504">arXiv:2110.07504</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2110.07504">pdf</a>, <a href="https://arxiv.org/format/2110.07504">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </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.105.032004">10.1103/PhysRevD.105.032004 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Transverse single spin asymmetries of forward neutrons in $p$$+$$p$, $p$$+$Al, and $p$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV as a function of transverse and longitudinal momenta </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a> , et al. (286 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="2110.07504v2-abstract-short" style="display: inline;"> In 2015 the PHENIX collaboration at the Relativistic Heavy Ion Collider recorded $p$$+$$p$, $p$$+$Al, and $p$$+$Au collision data at center of mass energies of $\sqrt{s_{_{NN}}}=200$ GeV with the proton beam(s) transversely polarized. At very forward rapidities $畏&gt;6.8$ relative to the polarized proton beam, neutrons were detected either inclusively or in (anti)correlation with detector activity re&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2110.07504v2-abstract-full').style.display = 'inline'; document.getElementById('2110.07504v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2110.07504v2-abstract-full" style="display: none;"> In 2015 the PHENIX collaboration at the Relativistic Heavy Ion Collider recorded $p$$+$$p$, $p$$+$Al, and $p$$+$Au collision data at center of mass energies of $\sqrt{s_{_{NN}}}=200$ GeV with the proton beam(s) transversely polarized. At very forward rapidities $畏&gt;6.8$ relative to the polarized proton beam, neutrons were detected either inclusively or in (anti)correlation with detector activity related to hard collisions. The resulting single spin asymmetries, that were previously reported, have now been extracted as a function of the transverse momentum of the neutron as well as its longitudinal momentum fraction $x_F$. The explicit kinematic dependence, combined with the correlation information allows for a closer look at the interplay of different mechanisms suggested to describe these asymmetries, such as hadronic interactions or electromagnetic interactions in ultra-peripheral collisions, UPC. Events that are correlated with a hard collision indeed display a mostly negative asymmetry that increases in magnitude as a function of transverse momentum with only little dependence on $x_F$. In contrast, events that are not likely to have emerged from a hard collision display positive asymmetries for the nuclear collisions with a kinematic dependence that resembles that of a UPC based model. Because the UPC interaction depends strongly on the charge of the nucleus, those effects are very small for $p$$+$$p$ collisions, moderate for $p$$+$Al collisions, and large for $p$$+$Au collisions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2110.07504v2-abstract-full').style.display = 'none'; document.getElementById('2110.07504v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 14 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">311 authors from 68 institutions, 12 pages, 8 figures, 2015 data. v2 is version accepted for publication in Physical Review D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 105, 032004 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2108.08527">arXiv:2108.08527</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2108.08527">pdf</a>, <a href="https://arxiv.org/format/2108.08527">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="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/10.3847/1538-4357/ac32c1">10.3847/1538-4357/ac32c1 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Limits on astrophysical antineutrinos with the KamLAND experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hayashida%2C+S">S. Hayashida</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kinoshita%2C+T">T. Kinoshita</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a> , et al. (45 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="2108.08527v3-abstract-short" style="display: inline;"> We report on a search for electron antineutrinos ($\bar谓_e$) from astrophysical sources in the neutrino energy range 8.3 to 30.8 MeV with the KamLAND detector. In an exposure of 6.72 kton-year of the liquid scintillator, we observe 18 candidate events via the inverse beta decay reaction. Although there is a large background uncertainty from neutral current atmospheric neutrino interactions, we fin&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2108.08527v3-abstract-full').style.display = 'inline'; document.getElementById('2108.08527v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2108.08527v3-abstract-full" style="display: none;"> We report on a search for electron antineutrinos ($\bar谓_e$) from astrophysical sources in the neutrino energy range 8.3 to 30.8 MeV with the KamLAND detector. In an exposure of 6.72 kton-year of the liquid scintillator, we observe 18 candidate events via the inverse beta decay reaction. Although there is a large background uncertainty from neutral current atmospheric neutrino interactions, we find no significant excess over background model predictions. Assuming several supernova relic neutrino spectra, we give upper flux limits of 60--110 cm$^{-2}$ s$^{-1}$ (90% CL) in the analysis range and present a model-independent flux. We also set limits on the annihilation rates for light dark matter pairs to neutrino pairs. These data improves on the upper probability limit of $^{8}$B solar neutrinos converting into $\bar谓_e$&#39;s, $P_{谓_e \rightarrow \bar谓_e} &lt; 3.5\times10^{-5}$ (90% CL) assuming an undistorted $\bar谓_e$ shape. This corresponds to a solar $\bar谓_e$ flux of 60 cm$^{-2}$ s$^{-1}$ (90% CL) in the analysis energy range. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2108.08527v3-abstract-full').style.display = 'none'; document.getElementById('2108.08527v3-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 October, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 19 August, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 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">21 pages, 9 figures, 4 tables, accepted for publication in Astrophysical Journal</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> The Astrophysical Journal, Volume 925, Number 1, Page 14 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2107.06634">arXiv:2107.06634</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2107.06634">pdf</a>, <a href="https://arxiv.org/format/2107.06634">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.105.024901">10.1103/PhysRevC.105.024901 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Kinematic dependence of azimuthal anisotropies in $p$$+$Au, $d$$+$Au, $^3$He+Au at $\sqrt{s_{_{NN}}}$ = 200 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Ayuso%2C+C">C. Ayuso</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a> , et al. (360 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="2107.06634v2-abstract-short" style="display: inline;"> There is strong evidence for the formation of small droplets of quark-gluon plasma in $p/d/^{3}$He+Au collisions at the Relativistic Heavy Ion Collider (RHIC) and in $p$+$p$/Pb collisions at the Large Hadron Collider. In particular, the analysis of data at RHIC for different geometries obtained by varying the projectile size and shape has proven insightful. In the present analysis, we find excelle&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.06634v2-abstract-full').style.display = 'inline'; document.getElementById('2107.06634v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2107.06634v2-abstract-full" style="display: none;"> There is strong evidence for the formation of small droplets of quark-gluon plasma in $p/d/^{3}$He+Au collisions at the Relativistic Heavy Ion Collider (RHIC) and in $p$+$p$/Pb collisions at the Large Hadron Collider. In particular, the analysis of data at RHIC for different geometries obtained by varying the projectile size and shape has proven insightful. In the present analysis, we find excellent agreement with the previously published PHENIX at RHIC results on elliptical and triangular flow with an independent analysis via the two-particle correlation method, which has quite different systematic uncertainties and an independent code base. In addition, the results are extended to other detector combinations with different kinematic (pseudorapidity) coverage. These results provide additional constraints on contributions from nonflow and longitudinal decorrelations. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.06634v2-abstract-full').style.display = 'none'; document.getElementById('2107.06634v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 14 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">383 authors from 70 institutions, 13 pages, 12 figures, 4 tables, 2014,15,16 data (and supplemental material of 9 pages with 6 figures and 16 tables). v2 is version accepted for publication in Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2105.02458">arXiv:2105.02458</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2105.02458">pdf</a>, <a href="https://arxiv.org/format/2105.02458">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Solar and Stellar Astrophysics">astro-ph.SR</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/10.3847/1538-4357/ac35d1">10.3847/1538-4357/ac35d1 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for Solar Flare Neutrinos with the KamLAND detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hayashida%2C+S">S. Hayashida</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Kinoshita%2C+T">T. Kinoshita</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a> , et al. (44 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="2105.02458v2-abstract-short" style="display: inline;"> We report the result of a search for neutrinos in coincidence with solar flares from the GOES flare database. The search was performed on a 10.8 kton-year exposure of KamLAND collected from 2002 to 2019. This large exposure allows us to explore previously unconstrained parameter space for solar flare neutrinos. We found no statistical excess of neutrinos and established 90% confidence level upper&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2105.02458v2-abstract-full').style.display = 'inline'; document.getElementById('2105.02458v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2105.02458v2-abstract-full" style="display: none;"> We report the result of a search for neutrinos in coincidence with solar flares from the GOES flare database. The search was performed on a 10.8 kton-year exposure of KamLAND collected from 2002 to 2019. This large exposure allows us to explore previously unconstrained parameter space for solar flare neutrinos. We found no statistical excess of neutrinos and established 90% confidence level upper limits of $8.4 \times 10^7$ cm$^{-2}$ ($3.0 \times 10^{9}$ cm$^{-2}$) on electron anti-neutrino (electron neutrino) fluence at 20 MeV normalized to the X12 flare, assuming that the neutrino fluence is proportional to the X-ray intensity. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2105.02458v2-abstract-full').style.display = 'none'; document.getElementById('2105.02458v2-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 October, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 6 May, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">13 pages, 9 figures, accepted October 27, 2021</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> The Astrophysical Journal, Volume 924, Number 2, Page 103 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2104.10452">arXiv:2104.10452</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2104.10452">pdf</a>, <a href="https://arxiv.org/format/2104.10452">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Instrumentation and Detectors">physics.ins-det</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1748-0221/16/08/p08023">10.1088/1748-0221/16/08/p08023 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The nylon balloon for xenon loaded liquid scintillator in KamLAND-Zen 800 neutrinoless double-beta decay search experiment </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=collaboration%2C+K">KamLAND-Zen collaboration</a>, <a href="/search/?searchtype=author&amp;query=%3A"> :</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hayashida%2C+S">S. Hayashida</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Nakada%2C+T">T. Nakada</a>, <a href="/search/?searchtype=author&amp;query=Obara%2C+S">S. Obara</a>, <a href="/search/?searchtype=author&amp;query=Ozaki%2C+H">H. Ozaki</a>, <a href="/search/?searchtype=author&amp;query=Shirai%2C+J">J. Shirai</a>, <a href="/search/?searchtype=author&amp;query=Ueshima%2C+K">K. Ueshima</a>, <a href="/search/?searchtype=author&amp;query=Watanabe%2C+H">H. Watanabe</a>, <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hayashi%2C+A">A. Hayashi</a>, <a href="/search/?searchtype=author&amp;query=Honda%2C+Y">Y. Honda</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Ishikawa%2C+S">S. Ishikawa</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kamizawa%2C+K">K. Kamizawa</a> , et al. (49 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="2104.10452v3-abstract-short" style="display: inline;"> The KamLAND-Zen 800 experiment is searching for the neutrinoless double-beta decay of $^{136}$Xe by using $^{136}$Xe-loaded liquid scintillator. The liquid scintillator is enclosed inside a balloon made of thin, transparent, low-radioactivity film that we call Inner Balloon (IB). The IB, apart from guaranteeing the liquid containment, also allows to minimize the background from cosmogenic muon-spa&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2104.10452v3-abstract-full').style.display = 'inline'; document.getElementById('2104.10452v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2104.10452v3-abstract-full" style="display: none;"> The KamLAND-Zen 800 experiment is searching for the neutrinoless double-beta decay of $^{136}$Xe by using $^{136}$Xe-loaded liquid scintillator. The liquid scintillator is enclosed inside a balloon made of thin, transparent, low-radioactivity film that we call Inner Balloon (IB). The IB, apart from guaranteeing the liquid containment, also allows to minimize the background from cosmogenic muon-spallation products and $^{8}$B solar neutrinos. Indeed these events could contribute to the total counts in the region of interest around the Q-value of the double-beta decay of $^{136}$Xe. In this paper, we present an overview of the IB and describe the various steps of its commissioning minimizing the radioactive contaminations, from the material selection, to the fabrication of the balloon and its installation inside the KamLAND detector. Finally, we show the impact of the IB on the KamLAND background as measured by the KamLAND detector itself. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2104.10452v3-abstract-full').style.display = 'none'; document.getElementById('2104.10452v3-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 June, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 21 April, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> April 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">23 pages, 16 figures, to be submitted to JINST</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> 2021 JINST 16 P08023 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2102.13585">arXiv:2102.13585</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2102.13585">pdf</a>, <a href="https://arxiv.org/format/2102.13585">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </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.127.162001">10.1103/PhysRevLett.127.162001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Probing gluon spin-momentum correlations in transversely polarized protons through midrapidity isolated direct photons in $p^\uparrow+p$ collisions at $\sqrt{s}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a>, <a href="/search/?searchtype=author&amp;query=Campbell%2C+S">S. Campbell</a> , et al. (286 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="2102.13585v2-abstract-short" style="display: inline;"> Studying spin-momentum correlations in hadronic collisions offers a glimpse into a three-dimensional picture of proton structure. The transverse single-spin asymmetry for midrapidity isolated direct photons in $p^\uparrow+p$ collisions at $\sqrt{s}=200$ GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). Because direct photons in particular are produced from the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2102.13585v2-abstract-full').style.display = 'inline'; document.getElementById('2102.13585v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2102.13585v2-abstract-full" style="display: none;"> Studying spin-momentum correlations in hadronic collisions offers a glimpse into a three-dimensional picture of proton structure. The transverse single-spin asymmetry for midrapidity isolated direct photons in $p^\uparrow+p$ collisions at $\sqrt{s}=200$ GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider (RHIC). Because direct photons in particular are produced from the hard scattering and do not interact via the strong force, this measurement is a clean probe of initial-state spin-momentum correlations inside the proton and is in particular sensitive to gluon interference effects within the proton. This is the first time direct photons have been used as a probe of spin-momentum correlations at RHIC. The uncertainties on the results are a fifty-fold improvement with respect to those of the one prior measurement for the same observable, from the Fermilab E704 experiment. These results constrain gluon spin-momentum correlations in transversely polarized protons. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2102.13585v2-abstract-full').style.display = 'none'; document.getElementById('2102.13585v2-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 August, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 February, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 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">312 authors from 68 institutions, 8 pages, 2 figures, 1 table, 2015 data. v2 is version accepted by Physical Review Letters. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2101.06049">arXiv:2101.06049</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2101.06049">pdf</a>, <a href="https://arxiv.org/ps/2101.06049">ps</a>, <a href="https://arxiv.org/format/2101.06049">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> </div> </div> <p class="title is-5 mathjax"> A Search for Charged Excitation of Dark Matter with the KamLAND-Zen Detector </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hayashida%2C+S">S. Hayashida</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kinoshita%2C+T">T. Kinoshita</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+R">R. Nakamura</a> , et al. (47 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="2101.06049v1-abstract-short" style="display: inline;"> There are many theories where a dark matter particle is part of a multiplet with an electrically charged state. If WIMP dark matter ($蠂^{0}$) is accompanied by a charged excited state ($蠂^{-}$) separated by a small mass difference, it can form a stable bound state with a nucleus. In supersymmetric models, the $蠂^{0}$ and the $蠂^{-}$ could be the neutralino and a charged slepton, such as the neutra&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2101.06049v1-abstract-full').style.display = 'inline'; document.getElementById('2101.06049v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2101.06049v1-abstract-full" style="display: none;"> There are many theories where a dark matter particle is part of a multiplet with an electrically charged state. If WIMP dark matter ($蠂^{0}$) is accompanied by a charged excited state ($蠂^{-}$) separated by a small mass difference, it can form a stable bound state with a nucleus. In supersymmetric models, the $蠂^{0}$ and the $蠂^{-}$ could be the neutralino and a charged slepton, such as the neutralino-stau degenerate model. The formation binding process is expected to result in an energy deposition of {\it O}(1--10 MeV), making it suitable for detection in large liquid scintillator detectors. We describe new constraints on the bound state formation with a xenon nucleus using the KamLAND-Zen 400 Phase-II dataset. In order to enlarge the searchable parameter space, all xenon isotopes in the detector were used. For a benchmark parameter set of $m_{蠂^{0}} = 100$ GeV and $螖m = 10$ MeV, this study sets the most stringent upper limits on the recombination cross section $\langle蟽v\rangle$ and the decay-width of $蠂^{-}$ of $2.0 \times 10^{-31}$ ${\rm cm^3/s}$ and $1.1 \times 10^{-18}$ GeV, respectively (90\% confidence level). <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2101.06049v1-abstract-full').style.display = 'none'; document.getElementById('2101.06049v1-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 January, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2021. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2012.12053">arXiv:2012.12053</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2012.12053">pdf</a>, <a href="https://arxiv.org/format/2012.12053">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="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/10.3847/1538-4357/abd5bc">10.3847/1538-4357/abd5bc <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for Low-energy Electron Antineutrinos in KamLAND Associated with Gravitational Wave Events </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Abe%2C+S">S. Abe</a>, <a href="/search/?searchtype=author&amp;query=Asami%2C+S">S. Asami</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+A">A. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gando%2C+Y">Y. Gando</a>, <a href="/search/?searchtype=author&amp;query=Gima%2C+T">T. Gima</a>, <a href="/search/?searchtype=author&amp;query=Goto%2C+A">A. Goto</a>, <a href="/search/?searchtype=author&amp;query=Hachiya%2C+T">T. Hachiya</a>, <a href="/search/?searchtype=author&amp;query=Hata%2C+K">K. Hata</a>, <a href="/search/?searchtype=author&amp;query=Hayashida%2C+S">S. Hayashida</a>, <a href="/search/?searchtype=author&amp;query=Hosokawa%2C+K">K. Hosokawa</a>, <a href="/search/?searchtype=author&amp;query=Ichimura%2C+K">K. Ichimura</a>, <a href="/search/?searchtype=author&amp;query=Ieki%2C+S">S. Ieki</a>, <a href="/search/?searchtype=author&amp;query=Ikeda%2C+H">H. Ikeda</a>, <a href="/search/?searchtype=author&amp;query=Inoue%2C+K">K. Inoue</a>, <a href="/search/?searchtype=author&amp;query=Ishidoshiro%2C+K">K. Ishidoshiro</a>, <a href="/search/?searchtype=author&amp;query=Kamei%2C+Y">Y. Kamei</a>, <a href="/search/?searchtype=author&amp;query=Kawada%2C+N">N. Kawada</a>, <a href="/search/?searchtype=author&amp;query=Kishimoto%2C+Y">Y. Kishimoto</a>, <a href="/search/?searchtype=author&amp;query=Kinoshita%2C+T">T. Kinoshita</a>, <a href="/search/?searchtype=author&amp;query=Koga%2C+M">M. Koga</a>, <a href="/search/?searchtype=author&amp;query=Maemura%2C+N">N. Maemura</a>, <a href="/search/?searchtype=author&amp;query=Mitsui%2C+T">T. Mitsui</a>, <a href="/search/?searchtype=author&amp;query=Miyake%2C+H">H. Miyake</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a>, <a href="/search/?searchtype=author&amp;query=Nakamura%2C+K">K. Nakamura</a> , et al. (44 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="2012.12053v1-abstract-short" style="display: inline;"> We present the results of a search for MeV-scale electron antineutrino events in KamLAND in coincident with the 60 gravitational wave events/candidates reported by the LIGO/Virgo collaboration during their second and third observing runs. We find no significant coincident signals within a $\pm$ 500 s timing window from each gravitational wave and present 90% C.L. upper limits on the electron antin&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2012.12053v1-abstract-full').style.display = 'inline'; document.getElementById('2012.12053v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2012.12053v1-abstract-full" style="display: none;"> We present the results of a search for MeV-scale electron antineutrino events in KamLAND in coincident with the 60 gravitational wave events/candidates reported by the LIGO/Virgo collaboration during their second and third observing runs. We find no significant coincident signals within a $\pm$ 500 s timing window from each gravitational wave and present 90% C.L. upper limits on the electron antineutrino fluence between $10^{8}$-$10^{13}\,{\mathrm cm^2}$ for neutrino energies in the energy range of 1.8-111 MeV. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2012.12053v1-abstract-full').style.display = 'none'; document.getElementById('2012.12053v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 22 December, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">11 pages, 2 figures, 2 tables, Accepted for publication in ApJ</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> The Astrophysical Journal, Volume 909, Number 2 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.14187">arXiv:2011.14187</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.14187">pdf</a>, <a href="https://arxiv.org/format/2011.14187">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> </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.103.032007">10.1103/PhysRevD.103.032007 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Transverse momentum dependent forward neutron single spin asymmetries in transversely polarized $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a> , et al. (289 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="2011.14187v2-abstract-short" style="display: inline;"> In 2015, the PHENIX collaboration has measured very forward ($畏&gt;6.8$) single-spin asymmetries of inclusive neutrons in transversely polarized proton-proton and proton-nucleus collisions at a center of mass energy of 200 GeV. A previous publication from this data set concentrated on the nuclear dependence of such asymmetries. In this measurement the explicit transverse-momentum dependence of inclus&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.14187v2-abstract-full').style.display = 'inline'; document.getElementById('2011.14187v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.14187v2-abstract-full" style="display: none;"> In 2015, the PHENIX collaboration has measured very forward ($畏&gt;6.8$) single-spin asymmetries of inclusive neutrons in transversely polarized proton-proton and proton-nucleus collisions at a center of mass energy of 200 GeV. A previous publication from this data set concentrated on the nuclear dependence of such asymmetries. In this measurement the explicit transverse-momentum dependence of inclusive neutron single spin asymmetries for proton-proton collisions is extracted using a bootstrapping-unfolding technique on the transverse momenta. This explicit transverse-momentum dependence will help improve the understanding of the mechanisms that create these asymmetries. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.14187v2-abstract-full').style.display = 'none'; document.getElementById('2011.14187v2-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 February, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 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">314 authors from 66 institutions, 8 pages, 3 figures, 1 table, 2015 data. v2 is version accepted for publication in Physical Review D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 103, 032007 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2011.14170">arXiv:2011.14170</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2011.14170">pdf</a>, <a href="https://arxiv.org/format/2011.14170">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> </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.103.052009">10.1103/PhysRevD.103.052009 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Transverse single-spin asymmetries of midrapidity $蟺^0$ and $畏$ mesons in polarized $p$$+$$p$ collisions at $\sqrt{s}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Andrieux%2C+V">V. Andrieux</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Bichon%2C+L">L. Bichon</a>, <a href="/search/?searchtype=author&amp;query=Blankenship%2C+B">B. Blankenship</a>, <a href="/search/?searchtype=author&amp;query=Blau%2C+D+S">D. S. Blau</a>, <a href="/search/?searchtype=author&amp;query=Bok%2C+J+S">J. S. Bok</a>, <a href="/search/?searchtype=author&amp;query=Borisov%2C+V">V. Borisov</a>, <a href="/search/?searchtype=author&amp;query=Brooks%2C+M+L">M. L. Brooks</a>, <a href="/search/?searchtype=author&amp;query=Bryslawskyj%2C+J">J. Bryslawskyj</a>, <a href="/search/?searchtype=author&amp;query=Bumazhnov%2C+V">V. Bumazhnov</a> , et al. (289 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="2011.14170v2-abstract-short" style="display: inline;"> We present a measurement of the transverse single-spin asymmetry for $蟺^0$ and $畏$ mesons in $p^\uparrow$$+$$p$ collisions in the pseudorapidity range $|畏|&lt;0.35$ and at a center-of-mass energy of 200 GeV with the PHENIX detector at the Relativistic Heavy Ion Collider. In comparison with previous measurements in this kinematic region, these results have a factor of 3 smaller uncertainties. As hadro&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.14170v2-abstract-full').style.display = 'inline'; document.getElementById('2011.14170v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2011.14170v2-abstract-full" style="display: none;"> We present a measurement of the transverse single-spin asymmetry for $蟺^0$ and $畏$ mesons in $p^\uparrow$$+$$p$ collisions in the pseudorapidity range $|畏|&lt;0.35$ and at a center-of-mass energy of 200 GeV with the PHENIX detector at the Relativistic Heavy Ion Collider. In comparison with previous measurements in this kinematic region, these results have a factor of 3 smaller uncertainties. As hadrons, $蟺^0$ and $畏$ mesons are sensitive to both initial- and final-state nonperturbative effects for a mix of parton flavors. Comparisons of the differences in their transverse single-spin asymmetries have the potential to disentangle the possible effects of strangeness, isospin, or mass. These results can constrain the twist-3 trigluon collinear correlation function as well as the gluon Sivers function. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2011.14170v2-abstract-full').style.display = 'none'; document.getElementById('2011.14170v2-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 28 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">314 authors from 66 institutions, 10 pages, 5 figures, 2 tables, 2015 data. v2 is version accepted for publication in Phys. Rev. D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 103, 052009 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2005.14686">arXiv:2005.14686</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.14686">pdf</a>, <a href="https://arxiv.org/format/2005.14686">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.102.064905">10.1103/PhysRevC.102.064905 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Production of $蟺^0$ and $畏$ mesons in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+X">X. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Baublis%2C+V">V. Baublis</a>, <a href="/search/?searchtype=author&amp;query=Baumann%2C+C">C. Baumann</a>, <a href="/search/?searchtype=author&amp;query=Baumgart%2C+S">S. Baumgart</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a> , et al. (378 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="2005.14686v2-abstract-short" style="display: inline;"> The PHENIX experiment at the Relativistic Heavy Ion Collider measured $蟺^0$ and $畏$ mesons at midrapidity in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV in a wide transverse momentum range. Measurements were performed in the $蟺^0(畏)\rightarrow纬纬$ decay modes. A strong suppression of $蟺^0$ and $畏$ meson production at high transverse momentum was observed in central U$+$U collisions relative to b&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14686v2-abstract-full').style.display = 'inline'; document.getElementById('2005.14686v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.14686v2-abstract-full" style="display: none;"> The PHENIX experiment at the Relativistic Heavy Ion Collider measured $蟺^0$ and $畏$ mesons at midrapidity in U$+$U collisions at $\sqrt{s_{_{NN}}}=192$ GeV in a wide transverse momentum range. Measurements were performed in the $蟺^0(畏)\rightarrow纬纬$ decay modes. A strong suppression of $蟺^0$ and $畏$ meson production at high transverse momentum was observed in central U$+$U collisions relative to binary scaled $p$$+$$p$ results. Yields of $蟺^0$ and $畏$ mesons measured in U$+$U collisions show similar suppression pattern to the ones measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV for similar numbers of participant nucleons. The $畏$/$蟺^0$ ratios do not show dependence on centrality or transverse momentum, and are consistent with previously measured values in hadron-hadron, hadron-nucleus, nucleus-nucleus, and $e^+e^-$ collisions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14686v2-abstract-full').style.display = 'none'; document.getElementById('2005.14686v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 13 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 May, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">403 authors from 72 institutions, 13 pages, 6 figures, 7 tables, 2012 data. v2 is version accepted by Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 102, 064905 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2005.14276">arXiv:2005.14276</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.14276">pdf</a>, <a href="https://arxiv.org/format/2005.14276">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </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.102.092002">10.1103/PhysRevD.102.092002 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Production of $b\bar{b}$ at forward rapidity in $p$+$p$ collisions at $\sqrt{s}=510$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a> , et al. (325 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="2005.14276v2-abstract-short" style="display: inline;"> The cross section of bottom quark-antiquark ($b\bar{b}$) production in $p$+$p$ collisions at $\sqrt{s}=510$ GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider. The results are based on the yield of high mass, like-sign muon pairs measured within the PHENIX muon arm acceptance ($1.2&lt;|y|&lt;2.2$). The $b\bar{b}$ signal is extracted from like-sign dimuons by utilizing the un&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14276v2-abstract-full').style.display = 'inline'; document.getElementById('2005.14276v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.14276v2-abstract-full" style="display: none;"> The cross section of bottom quark-antiquark ($b\bar{b}$) production in $p$+$p$ collisions at $\sqrt{s}=510$ GeV is measured with the PHENIX detector at the Relativistic Heavy Ion Collider. The results are based on the yield of high mass, like-sign muon pairs measured within the PHENIX muon arm acceptance ($1.2&lt;|y|&lt;2.2$). The $b\bar{b}$ signal is extracted from like-sign dimuons by utilizing the unique properties of neutral $B$ meson oscillation. We report a differential cross section of $d蟽_{b\bar{b}\rightarrow 渭^\pm渭^\pm}/dy = 0.16 \pm 0.01~(\mbox{stat}) \pm 0.02~(\mbox{syst}) \pm 0.02~(\mbox{global})$ nb for like-sign muons in the rapidity and $p_T$ ranges $1.2&lt;|y|&lt;2.2$ and $p_T&gt;1$ GeV/$c$, and dimuon mass of 5--10 GeV/$c^2$. The extrapolated total cross section at this energy for $b\bar{b}$ production is $13.1 \pm 0.6~(\mbox{stat}) \pm 1.5~(\mbox{syst}) \pm 2.7~(\mbox{global})~渭$b. The total cross section is compared to a perturbative quantum chromodynamics calculation and is consistent within uncertainties. The azimuthal opening angle between muon pairs from $b\bar{b}$ decays and their $p_T$ distributions are compared to distributions generated using {\sc ps pythia 6}, which includes next-to-leading order processes. The azimuthal correlations and pair $p_T$ distribution are not very well described by {\sc pythia} calculations, but are still consistent within uncertainties. Flavor creation and flavor excitation subprocesses are favored over gluon splitting. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14276v2-abstract-full').style.display = 'none'; document.getElementById('2005.14276v2-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 October, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 May, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">360 authors from 69 institutions, 13 pages, 11 figures, 2 tables, 2013 data. v2 is version accepted for publication in Physical Review D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 102, 092002 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2005.14273">arXiv:2005.14273</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.14273">pdf</a>, <a href="https://arxiv.org/format/2005.14273">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> </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.102.072008">10.1103/PhysRevD.102.072008 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Polarization and cross section of midrapidity J/$蠄$ production in proton-proton collisions at $\sqrt{s}=510$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a> , et al. (325 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="2005.14273v2-abstract-short" style="display: inline;"> The PHENIX experiment has measured the spin alignment for inclusive $J/蠄\rightarrow e^{+}e^{-}$ decays in $p$+$p$ collisions at $\sqrt{s}=510$ GeV at midrapidity. The angular distributions have been measured in three different polarization frames, and the three decay angular coefficients have been extracted in a full two-dimensional analysis. Previously, PHENIX saw large longitudinal net polarizat&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14273v2-abstract-full').style.display = 'inline'; document.getElementById('2005.14273v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.14273v2-abstract-full" style="display: none;"> The PHENIX experiment has measured the spin alignment for inclusive $J/蠄\rightarrow e^{+}e^{-}$ decays in $p$+$p$ collisions at $\sqrt{s}=510$ GeV at midrapidity. The angular distributions have been measured in three different polarization frames, and the three decay angular coefficients have been extracted in a full two-dimensional analysis. Previously, PHENIX saw large longitudinal net polarization at forward rapidity at the same collision energy. This analysis at midrapidity, complementary to the previous PHENIX results, sees no sizable polarization in the measured transverse momentum range of $0.0&lt;p_T&lt;10.0$ GeV/$c$. The results are consistent with a previous one-dimensional analysis at midrapidity at $\sqrt{s}=200$ GeV. The transverse-momentum-dependent cross section for midrapidity $J/蠄$ production has additionally been measured, and after comparison to world data we find a simple logarithmic dependence of the cross section on $\sqrt{s}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14273v2-abstract-full').style.display = 'none'; document.getElementById('2005.14273v2-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 October, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 May, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">360 authors from 69 institutions, 13 pages, 15 figures, 1 table, 2013 data. v1 is version accepted for publication in Physical Review D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 102, 072008 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2005.14270">arXiv:2005.14270</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2005.14270">pdf</a>, <a href="https://arxiv.org/format/2005.14270">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevC.102.054910">10.1103/PhysRevC.102.054910 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of jet-medium interactions via direct photon-hadron correlations in Au$+$Au and $d$$+$Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U">U. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Afanasiev%2C+S">S. Afanasiev</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Al-Bataineh%2C+H">H. Al-Bataineh</a>, <a href="/search/?searchtype=author&amp;query=Alexander%2C+J">J. Alexander</a>, <a href="/search/?searchtype=author&amp;query=Al-Ta%27ani%2C+H">H. Al-Ta&#39;ani</a>, <a href="/search/?searchtype=author&amp;query=Angerami%2C+A">A. Angerami</a>, <a href="/search/?searchtype=author&amp;query=Aoki%2C+K">K. Aoki</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Aschenauer%2C+E+C">E. C. Aschenauer</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Averbeck%2C+R">R. Averbeck</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Baksay%2C+G">G. Baksay</a>, <a href="/search/?searchtype=author&amp;query=Baksay%2C+L">L. Baksay</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a> , et al. (553 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="2005.14270v2-abstract-short" style="display: inline;"> We present direct photon-hadron correlations in 200 GeV/A Au$+$Au, $d$$+$Au and $p$$+$$p$ collisions, for direct photon $p_T$ from 5--12 GeV/$c$, collected by the PHENIX Collaboration in the years from 2006 to 2011. We observe no significant modification of jet fragmentation in $d$$+$Au collisions, indicating that cold nuclear matter effects are small or absent. Hadrons carrying a large fraction o&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14270v2-abstract-full').style.display = 'inline'; document.getElementById('2005.14270v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2005.14270v2-abstract-full" style="display: none;"> We present direct photon-hadron correlations in 200 GeV/A Au$+$Au, $d$$+$Au and $p$$+$$p$ collisions, for direct photon $p_T$ from 5--12 GeV/$c$, collected by the PHENIX Collaboration in the years from 2006 to 2011. We observe no significant modification of jet fragmentation in $d$$+$Au collisions, indicating that cold nuclear matter effects are small or absent. Hadrons carrying a large fraction of the quark&#39;s momentum are suppressed in Au$+$Au compared to $p$$+$$p$ and $d$$+$Au. As the momentum fraction decreases, the yield of hadrons in Au$+$Au increases to an excess over the yield in $p$$+$$p$ collisions. The excess is at large angles and at low hadron $p_T$ and is most pronounced for hadrons associated with lower momentum direct photons. Comparison to theoretical calculations suggests that the hadron excess arises from medium response to energy deposited by jets. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2005.14270v2-abstract-full').style.display = 'none'; document.getElementById('2005.14270v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 19 November, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 28 May, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 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">578 authors from 80 institutions, 11 pages, 7 figures, data from 2007, 2008, 2010, and 2011. v2 is version accepted for publication in Physical Review C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. C 102, 054910 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2004.02681">arXiv:2004.02681</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2004.02681">pdf</a>, <a href="https://arxiv.org/ps/2004.02681">ps</a>, <a href="https://arxiv.org/format/2004.02681">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Nuclear Experiment">nucl-ex</span> </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.102.032001">10.1103/PhysRevD.102.032001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of charged pion double spin asymmetries at midrapidity in longitudinally polarized $p$$+$$p$ collisions at $\sqrt{s}=510$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/?searchtype=author&amp;query=Acharya%2C+U+A">U. A. Acharya</a>, <a href="/search/?searchtype=author&amp;query=Adare%2C+A">A. Adare</a>, <a href="/search/?searchtype=author&amp;query=Aidala%2C+C">C. Aidala</a>, <a href="/search/?searchtype=author&amp;query=Ajitanand%2C+N+N">N. N. Ajitanand</a>, <a href="/search/?searchtype=author&amp;query=Akiba%2C+Y">Y. Akiba</a>, <a href="/search/?searchtype=author&amp;query=Akimoto%2C+R">R. Akimoto</a>, <a href="/search/?searchtype=author&amp;query=Alfred%2C+M">M. Alfred</a>, <a href="/search/?searchtype=author&amp;query=Apadula%2C+N">N. Apadula</a>, <a href="/search/?searchtype=author&amp;query=Aramaki%2C+Y">Y. Aramaki</a>, <a href="/search/?searchtype=author&amp;query=Asano%2C+H">H. Asano</a>, <a href="/search/?searchtype=author&amp;query=Atomssa%2C+E+T">E. T. Atomssa</a>, <a href="/search/?searchtype=author&amp;query=Awes%2C+T+C">T. C. Awes</a>, <a href="/search/?searchtype=author&amp;query=Azmoun%2C+B">B. Azmoun</a>, <a href="/search/?searchtype=author&amp;query=Babintsev%2C+V">V. Babintsev</a>, <a href="/search/?searchtype=author&amp;query=Bai%2C+M">M. Bai</a>, <a href="/search/?searchtype=author&amp;query=Bandara%2C+N+S">N. S. Bandara</a>, <a href="/search/?searchtype=author&amp;query=Bannier%2C+B">B. Bannier</a>, <a href="/search/?searchtype=author&amp;query=Barish%2C+K+N">K. N. Barish</a>, <a href="/search/?searchtype=author&amp;query=Bathe%2C+S">S. Bathe</a>, <a href="/search/?searchtype=author&amp;query=Bazilevsky%2C+A">A. Bazilevsky</a>, <a href="/search/?searchtype=author&amp;query=Beaumier%2C+M">M. Beaumier</a>, <a href="/search/?searchtype=author&amp;query=Beckman%2C+S">S. Beckman</a>, <a href="/search/?searchtype=author&amp;query=Belmont%2C+R">R. Belmont</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+A">A. Berdnikov</a>, <a href="/search/?searchtype=author&amp;query=Berdnikov%2C+Y">Y. Berdnikov</a> , et al. (335 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="2004.02681v2-abstract-short" style="display: inline;"> The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the longitudinal double spin asymmetries, $A_{LL}$, for charged pions at midrapidity ($|畏|&lt;0.35$) in longitudinally polarized $p$$+$$p$ collisions at $\sqrt{s}=510$ GeV. These measurements are sensitive to the gluon spin contribution to the total spin of the proton in the parton momentum fraction $x$ range between 0.04 and 0&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.02681v2-abstract-full').style.display = 'inline'; document.getElementById('2004.02681v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2004.02681v2-abstract-full" style="display: none;"> The PHENIX experiment at the Relativistic Heavy Ion Collider has measured the longitudinal double spin asymmetries, $A_{LL}$, for charged pions at midrapidity ($|畏|&lt;0.35$) in longitudinally polarized $p$$+$$p$ collisions at $\sqrt{s}=510$ GeV. These measurements are sensitive to the gluon spin contribution to the total spin of the proton in the parton momentum fraction $x$ range between 0.04 and 0.09. One can infer the sign of the gluon polarization from the ordering of pion asymmetries with charge alone. The asymmetries are found to be consistent with global quantum-chromodynamics fits of deep-inelastic scattering and data at $\sqrt{s}=200$ GeV, which show a nonzero positive contribution of gluon spin to the proton spin. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2004.02681v2-abstract-full').style.display = 'none'; document.getElementById('2004.02681v2-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 July, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 6 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">360 authors, 8 pages, 6 figures, 1 table, 2013 data. v2 is version accepted for publication in Physical Review D. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. 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