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name="order"><option selected value="-announced_date_first">Announcement date (newest first)</option><option value="announced_date_first">Announcement date (oldest first)</option><option value="-submitted_date">Submission date (newest first)</option><option value="submitted_date">Submission date (oldest first)</option><option value="">Relevance</option></select> </span> </div> <div class="control"> <button class="button is-small is-link">Go</button> </div> </div> </form> </div> </div> <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/2410.13515">arXiv:2410.13515</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.13515">pdf</a>, <a href="https://arxiv.org/format/2410.13515">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</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 Experiment">nucl-ex</span> </div> </div> <p class="title is-5 mathjax"> Observation of a rare beta decay of the charmed baryon with a Graph Neural Network </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (637 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="2410.13515v1-abstract-short" style="display: inline;"> The study of beta decay of the charmed baryon provides unique insights into the fundamental mechanism of the strong and electro-weak interactions. The $螞_c^+$, being the lightest charmed baryon, undergoes disintegration solely through the charm quark weak decay. Its beta decay provides an ideal laboratory for investigating non-perturbative effects in quantum chromodynamics and for constraining the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13515v1-abstract-full').style.display = 'inline'; document.getElementById('2410.13515v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13515v1-abstract-full" style="display: none;"> The study of beta decay of the charmed baryon provides unique insights into the fundamental mechanism of the strong and electro-weak interactions. The $螞_c^+$, being the lightest charmed baryon, undergoes disintegration solely through the charm quark weak decay. Its beta decay provides an ideal laboratory for investigating non-perturbative effects in quantum chromodynamics and for constraining the fundamental parameters of the Cabibbo-Kobayashi-Maskawa matrix in weak interaction theory. This article presents the first observation of the Cabibbo-suppressed $螞_c^+$ beta decay into a neutron $螞_c^+ \rightarrow n e^+ 谓_{e}$, based on $4.5~\mathrm{fb}^{-1}$ of electron-positron annihilation data collected with the BESIII detector in the energy region above the $螞^+_c\bar螞^-_c$ threshold. A novel machine learning technique, leveraging Graph Neural Networks, has been utilized to effectively separate signals from dominant backgrounds, particularly $螞_c^+ \rightarrow 螞e^+ 谓_{e}$. This approach has yielded a statistical significance of more than $10蟽$. The absolute branching fraction of $螞_c^+ \rightarrow n e^+ 谓_{e}$ is measured to be $(3.57\pm0.34_{\mathrm{stat}}\pm0.14_{\mathrm{syst}})\times 10^{-3}$. For the first time, the CKM matrix element $\left|V_{cd}\right|$ is extracted via a charmed baryon decay to be $0.208\pm0.011_{\rm exp.}\pm0.007_{\rm LQCD}\pm0.001_{蟿_{螞_c^+}}$. This study provides a new probe to further understand fundamental interactions in the charmed baryon sector, and demonstrates the power of modern machine learning techniques in enhancing experimental capability in high energy physics research. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13515v1-abstract-full').style.display = 'none'; document.getElementById('2410.13515v1-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 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">28 pages, 6 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/2209.08464">arXiv:2209.08464</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2209.08464">pdf</a>, <a href="https://arxiv.org/ps/2209.08464">ps</a>, <a href="https://arxiv.org/format/2209.08464">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1007/JHEP12(2022)033">10.1007/JHEP12(2022)033 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Partial wave analysis of the charmed baryon hadronic decay $螞_c^+\to螞蟺^+蟺^0$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Albrecht%2C+M">M. Albrecht</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+M+R">M. R. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+X+H">X. H. Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ferroli%2C+R+B">R. Baldini Ferroli</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Becker%2C+D">D. Becker</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bloms%2C+J">J. Bloms</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a> , et al. (555 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2209.08464v3-abstract-short" style="display: inline;"> Based on $e^+e^-$ collision samples corresponding to an integrated luminosity of 4.4 $\mbox{fb$^{-1}$}$ collected with the BESIII detector at center-of-mass energies between $4.6\,\,\mathrm{GeV}$ and $4.7\,\,\mathrm{GeV}$, a partial wave analysis of the charmed baryon hadronic decay $螞_c^+\to螞蟺^+蟺^0$ is performed, and the decays $螞_c^+\to螞蟻(770)^{+}$ and $螞_c^+\to危(1385)蟺$ are studied for the firs&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2209.08464v3-abstract-full').style.display = 'inline'; document.getElementById('2209.08464v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2209.08464v3-abstract-full" style="display: none;"> Based on $e^+e^-$ collision samples corresponding to an integrated luminosity of 4.4 $\mbox{fb$^{-1}$}$ collected with the BESIII detector at center-of-mass energies between $4.6\,\,\mathrm{GeV}$ and $4.7\,\,\mathrm{GeV}$, a partial wave analysis of the charmed baryon hadronic decay $螞_c^+\to螞蟺^+蟺^0$ is performed, and the decays $螞_c^+\to螞蟻(770)^{+}$ and $螞_c^+\to危(1385)蟺$ are studied for the first time. Making use of the world-average branching fraction $\mathcal{B}(螞_c^+\to螞蟺^+蟺^0)$, their branching fractions are determined to be \begin{eqnarray*} \begin{aligned} \mathcal{B}(螞_c^+\to螞蟻(770)^+)=&amp;(4.06\pm0.30\pm0.35\pm0.23)\times10^{-2},\\ \mathcal{B}(螞_c^+\to危(1385)^+蟺^0)=&amp;(5.86\pm0.49\pm0.52\pm0.35)\times10^{-3},\\ \mathcal{B}(螞_c^+\to危(1385)^0蟺^+)=&amp;(6.47\pm0.59\pm0.66\pm0.38)\times10^{-3},\\ \end{aligned} \end{eqnarray*} where the first uncertainties are statistical, the second are systematic, and the third are from the uncertainties of the branching fractions $\mathcal{B}(螞_c^+\to螞蟺^+蟺^0)$ and $\mathcal{B}(危(1385)\to螞蟺)$. In addition, %according to amplitudes determined from the partial wave analysis, the decay asymmetry parameters are measured to be $伪_{螞蟻(770)^+}=-0.763\pm0.053\pm0.045$, $伪_{危(1385)^{+}蟺^0}=-0.917\pm0.069\pm0.056$, and $伪_{危(1385)^{0}蟺^+}=-0.789\pm0.098\pm0.056$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2209.08464v3-abstract-full').style.display = 'none'; document.getElementById('2209.08464v3-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 December, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 September, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2022. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2107.09671">arXiv:2107.09671</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2107.09671">pdf</a>, <a href="https://arxiv.org/format/2107.09671">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Cosmology and Nongalactic Astrophysics">astro-ph.CO</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="General Relativity and Quantum Cosmology">gr-qc</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1088/1475-7516/2022/01/002">10.1088/1475-7516/2022/01/002 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Hubble-induced phase transitions on the lattice with applications to Ricci reheating </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">Dario Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Lopez-Eiguren%2C+A">Asier Lopez-Eiguren</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Rubio%2C+J">Javier Rubio</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="2107.09671v2-abstract-short" style="display: inline;"> Using 3+1 classical lattice simulations, we follow the symmetry breaking pattern and subsequent non-linear evolution of a spectator field non-minimally coupled to gravity when the post-inflationary dynamics is given in terms of a stiff equation-of-state parameter. We find that the gradient energy density immediately after the transition represents a non-negligible fraction of the total energy budg&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.09671v2-abstract-full').style.display = 'inline'; document.getElementById('2107.09671v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2107.09671v2-abstract-full" style="display: none;"> Using 3+1 classical lattice simulations, we follow the symmetry breaking pattern and subsequent non-linear evolution of a spectator field non-minimally coupled to gravity when the post-inflationary dynamics is given in terms of a stiff equation-of-state parameter. We find that the gradient energy density immediately after the transition represents a non-negligible fraction of the total energy budget, steadily growing to equal the kinetic counterpart. This behaviour is reflected on the evolution of the associated equation-of-state parameter, which approaches a universal value $1/3$, independently of the shape of non-linear interactions. Combined with kination, this observation allows for the generic onset of radiation domination for arbitrary self-interacting potentials, significantly extending previous results in the literature. The produced spectrum at that time is, however, non-thermal, precluding the naive extraction of thermodynamical quantities like temperature. Potential identifications of the spectator field with the Standard Model Higgs are also discussed. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2107.09671v2-abstract-full').style.display = 'none'; document.getElementById('2107.09671v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 January, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 20 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">26 pages, 12 figures, 1 appendix. Minor revisions, updated references, matches published version. Computer generated movies of the simulation are available at https://youtube.com/playlist?list=PLl1K9-81ct6yHh6boyTiZAfNv_zlwux7-</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2104.09131">arXiv:2104.09131</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2104.09131">pdf</a>, <a href="https://arxiv.org/ps/2104.09131">ps</a>, <a href="https://arxiv.org/format/2104.09131">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1103/PhysRevD.104.012006">10.1103/PhysRevD.104.012006 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Study of the decay $D^+\to K^*(892)^+ K_S^0$ in $D^+\to K^+ K_S^0 蟺^0$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ahmed%2C+S">S. Ahmed</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Albrecht%2C+M">M. Albrecht</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+M+R">M. R. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+X+H">X. H. Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ferroli%2C+R+B">R. Baldini Ferroli</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bloms%2C+J">J. Bloms</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (492 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="2104.09131v3-abstract-short" style="display: inline;"> Based on an $e^{+}e^{-}$ collision data sample corresponding to an integrated luminosity of 2.93 $\mathrm{fb}^{-1}$ collected with the BESIII detector at $\sqrt{s}=3.773 \mathrm{GeV}$, the first amplitude analysis of the singly Cabibbo-suppressed decay $D^{+}\to K^+ K_S^0 蟺^0$ is performed. From the amplitude analysis, the $K^*(892)^+ K_S^0$ component is found to be dominant with a fraction of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2104.09131v3-abstract-full').style.display = 'inline'; document.getElementById('2104.09131v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2104.09131v3-abstract-full" style="display: none;"> Based on an $e^{+}e^{-}$ collision data sample corresponding to an integrated luminosity of 2.93 $\mathrm{fb}^{-1}$ collected with the BESIII detector at $\sqrt{s}=3.773 \mathrm{GeV}$, the first amplitude analysis of the singly Cabibbo-suppressed decay $D^{+}\to K^+ K_S^0 蟺^0$ is performed. From the amplitude analysis, the $K^*(892)^+ K_S^0$ component is found to be dominant with a fraction of $(57.1\pm2.6\pm4.2)\%$, where the first uncertainty is statistical and the second systematic. In combination with the absolute branching fraction $\mathcal{B}(D^+\to K^+ K_S^0 蟺^0)$ measured by BESIII, we obtain $\mathcal{B}(D^+\to K^*(892)^+ K_S^0)=(8.69\pm0.40\pm0.64\pm0.51)\times10^{-3}$, where the third uncertainty is due to the branching fraction $\mathcal{B}(D^+\to K^+ K_S^0 蟺^0)$. The precision of this result is significantly improved compared to the previous measurement. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2104.09131v3-abstract-full').style.display = 'none'; document.getElementById('2104.09131v3-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, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 19 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">12 pages, 15 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 104, 012006 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1809.06496">arXiv:1809.06496</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1809.06496">pdf</a>, <a href="https://arxiv.org/ps/1809.06496">ps</a>, <a href="https://arxiv.org/format/1809.06496">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</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.122.062001">10.1103/PhysRevLett.122.062001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Observation of $D^+ \to f_0(500) e^+谓_e$ and Improved Measurements of $D \to蟻e^+谓_e$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ahmed%2C+S">S. Ahmed</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Albrecht%2C+M">M. Albrecht</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Alekseev%2C+M">M. Alekseev</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+F+F">F. F. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ferroli%2C+R+B">R. Baldini Ferroli</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bennett%2C+D+W">D. W. Bennett</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bennett%2C+J+V">J. V. Bennett</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Boger%2C+E">E. Boger</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Cai%2C+H">H. Cai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Cai%2C+X">X. Cai</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Calcaterra%2C+A">A. Calcaterra</a> , et al. (438 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="1809.06496v2-abstract-short" style="display: inline;"> Using a data sample corresponding to an integrated luminosity of 2.93~fb$^{-1}$ recorded by the BESIII detector at a center-of-mass energy of $3.773$ GeV, we present an analysis of the decays $\bar{D}^0\to蟺^+蟺^0 e^-\bar谓_e$ and $D^+\to蟺^-蟺^+ e^+谓_e$. By performing a partial wave analysis, the $蟺^+蟺^-$ $S$-wave contribution to $D^+\to蟺^-蟺^+ e^+谓_e$ is observed to be $(25.7\pm1.6\pm1.1)$% with a sta&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1809.06496v2-abstract-full').style.display = 'inline'; document.getElementById('1809.06496v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1809.06496v2-abstract-full" style="display: none;"> Using a data sample corresponding to an integrated luminosity of 2.93~fb$^{-1}$ recorded by the BESIII detector at a center-of-mass energy of $3.773$ GeV, we present an analysis of the decays $\bar{D}^0\to蟺^+蟺^0 e^-\bar谓_e$ and $D^+\to蟺^-蟺^+ e^+谓_e$. By performing a partial wave analysis, the $蟺^+蟺^-$ $S$-wave contribution to $D^+\to蟺^-蟺^+ e^+谓_e$ is observed to be $(25.7\pm1.6\pm1.1)$% with a statistical significance greater than 10$蟽$, besides the dominant $P$-wave contribution. This is the first observation of the $S$-wave contribution. We measure the branching fractions $\mathcal{B}(D^{0} \to 蟻^- e^+ 谓_e) = (1.445\pm 0.058 \pm 0.039) \times10^{-3}$, $\mathcal{B}(D^{+} \to 蟻^0 e^+ 谓_e) = (1.860\pm 0.070 \pm 0.061) \times10^{-3}$, and $\mathcal{B}(D^{+} \to f_0(500) e^+ 谓_e, f_0(500)\to蟺^+蟺^-) = (6.30\pm 0.43 \pm 0.32) \times10^{-4}$. An upper limit of $\mathcal{B}(D^{+} \to f_0(980) e^+ 谓_e, f_0(980)\to蟺^+蟺^-) &lt; 2.8 \times10^{-5}$ is set at the 90% confidence level. We also obtain the hadronic form factor ratios of $D\to 蟻e^+谓_e$ at $q^{2}=0$ assuming the single-pole dominance parameterization: $r_{V}=\frac{V(0)}{A_{1}(0)}=1.695\pm0.083\pm0.051$, $r_{2}=\frac{A_{2}(0)}{A_{1}(0)}=0.845\pm0.056\pm0.039$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1809.06496v2-abstract-full').style.display = 'none'; document.getElementById('1809.06496v2-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 February, 2019; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 September, 2018; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2018. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 122, 062001 (2019) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1010.5827">arXiv:1010.5827</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1010.5827">pdf</a>, <a href="https://arxiv.org/format/1010.5827">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Theory">hep-th</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="Nuclear Theory">nucl-th</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1140/epjc/s10052-010-1534-9">10.1140/epjc/s10052-010-1534-9 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Heavy quarkonium: progress, puzzles, and opportunities </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Brambilla%2C+N">N. Brambilla</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Eidelman%2C+S">S. Eidelman</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Heltsley%2C+B+K">B. K. Heltsley</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Vogt%2C+R">R. Vogt</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bodwin%2C+G+T">G. T. Bodwin</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Eichten%2C+E">E. Eichten</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Frawley%2C+A+D">A. D. Frawley</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Meyer%2C+A+B">A. B. Meyer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Mitchell%2C+R+E">R. E. Mitchell</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Papadimitriou%2C+V">V. Papadimitriou</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Petreczky%2C+P">P. Petreczky</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Petrov%2C+A+A">A. A. Petrov</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Robbe%2C+P">P. Robbe</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Vairo%2C+A">A. Vairo</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Andronic%2C+A">A. Andronic</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Arnaldi%2C+R">R. Arnaldi</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Artoisenet%2C+P">P. Artoisenet</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bali%2C+G">G. Bali</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bertolin%2C+A">A. Bertolin</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Brodzicka%2C+J">J. Brodzicka</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bruno%2C+G+E">G. E. Bruno</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Caldwell%2C+A">A. Caldwell</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Catmore%2C+J">J. Catmore</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Chang%2C+C+-">C. -H. Chang</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="1010.5827v3-abstract-short" style="display: inline;"> A golden age for heavy quarkonium physics dawned a decade ago, initiated by the confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of related experimental activity. The early years of this period were chronicled in the Quarkonium Working Group (QWG) CERN Yellow Report (YR) in 2004, which presented a comprehensive review of the status of the field at that time and prov&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1010.5827v3-abstract-full').style.display = 'inline'; document.getElementById('1010.5827v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1010.5827v3-abstract-full" style="display: none;"> A golden age for heavy quarkonium physics dawned a decade ago, initiated by the confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of related experimental activity. The early years of this period were chronicled in the Quarkonium Working Group (QWG) CERN Yellow Report (YR) in 2004, which presented a comprehensive review of the status of the field at that time and provided specific recommendations for further progress. However, the broad spectrum of subsequent breakthroughs, surprises, and continuing puzzles could only be partially anticipated. Since the release of the YR, the BESII program concluded only to give birth to BESIII; the $B$-factories and CLEO-c flourished; quarkonium production and polarization measurements at HERA and the Tevatron matured; and heavy-ion collisions at RHIC have opened a window on the deconfinement regime. All these experiments leave legacies of quality, precision, and unsolved mysteries for quarkonium physics, and therefore beg for continuing investigations. The plethora of newly-found quarkonium-like states unleashed a flood of theoretical investigations into new forms of matter such as quark-gluon hybrids, mesonic molecules, and tetraquarks. Measurements of the spectroscopy, decays, production, and in-medium behavior of c\bar{c}, b\bar{b}, and b\bar{c} bound states have been shown to validate some theoretical approaches to QCD and highlight lack of quantitative success for others. The intriguing details of quarkonium suppression in heavy-ion collisions that have emerged from RHIC have elevated the importance of separating hot- and cold-nuclear-matter effects in quark-gluon plasma studies. This review systematically addresses all these matters and concludes by prioritizing directions for ongoing and future efforts. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1010.5827v3-abstract-full').style.display = 'none'; document.getElementById('1010.5827v3-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 February, 2011; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 27 October, 2010; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2010. </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">182 pages, 112 figures. Editors: N. Brambilla, S. Eidelman, B. K. Heltsley, R. Vogt. Section Coordinators: G. T. Bodwin, E. Eichten, A. D. Frawley, A. B. Meyer, R. E. Mitchell, V. Papadimitriou, P. Petreczky, A. A. Petrov, P. Robbe, A. Vairo</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> TUM-EFT 11/10, CLNS 10/2066, ANL-HEP-PR-10-44, Alberta Thy 11-10, CP3-10-37, FZJ-IKP-TH-2010-24, INT-PUB-10-059 </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Eur.Phys.J.C71:1534,2011 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/hep-ph/0412158">arXiv:hep-ph/0412158</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/hep-ph/0412158">pdf</a>, <a href="https://arxiv.org/ps/hep-ph/0412158">ps</a>, <a href="https://arxiv.org/format/hep-ph/0412158">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</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="Nuclear Theory">nucl-th</span> </div> </div> <p class="title is-5 mathjax"> Heavy Quarkonium Physics </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-lat?searchtype=author&amp;query=Brambilla%2C+N">N. Brambilla</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Kr%C3%A4mer%2C+M">M. Kr盲mer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Mussa%2C+R">R. Mussa</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Vairo%2C+A">A. Vairo</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bali%2C+G">G. Bali</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bodwin%2C+G+T">G. T. Bodwin</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Braaten%2C+E">E. Braaten</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Eichten%2C+E">E. Eichten</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Eidelman%2C+S">S. Eidelman</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Godfrey%2C+S">S. Godfrey</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Hoang%2C+A">A. Hoang</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Jamin%2C+M">M. Jamin</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Kharzeev%2C+D">D. Kharzeev</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Lombardo%2C+M+P">M. P. Lombardo</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Lourenco%2C+C">C. Lourenco</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Meyer%2C+A+B">A. B. Meyer</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Papadimitriou%2C+V">V. Papadimitriou</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Patrignani%2C+C">C. Patrignani</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Rosati%2C+M">M. Rosati</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Sanchis-Lozano%2C+M+A">M. A. Sanchis-Lozano</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Satz%2C+H">H. Satz</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Soto%2C+J">J. Soto</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Besson%2C+D+Z">D. Z. Besson</a>, <a href="/search/hep-lat?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-lat?searchtype=author&amp;query=B%C3%B6hrer%2C+A">A. B枚hrer</a> , et al. (60 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="hep-ph/0412158v2-abstract-short" style="display: inline;"> This report is the result of the collaboration and research effort of the Quarkonium Working Group over the last three years. It provides a comprehensive overview of the state of the art in heavy-quarkonium theory and experiment, covering quarkonium spectroscopy, decay, and production, the determination of QCD parameters from quarkonium observables, quarkonia in media, and the effects on quarkon&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('hep-ph/0412158v2-abstract-full').style.display = 'inline'; document.getElementById('hep-ph/0412158v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="hep-ph/0412158v2-abstract-full" style="display: none;"> This report is the result of the collaboration and research effort of the Quarkonium Working Group over the last three years. It provides a comprehensive overview of the state of the art in heavy-quarkonium theory and experiment, covering quarkonium spectroscopy, decay, and production, the determination of QCD parameters from quarkonium observables, quarkonia in media, and the effects on quarkonia of physics beyond the Standard Model. An introduction to common theoretical and experimental tools is included. Future opportunities for research in quarkonium physics are also discussed. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('hep-ph/0412158v2-abstract-full').style.display = 'none'; document.getElementById('hep-ph/0412158v2-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, 2005; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 13 December, 2004; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2004. </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">xviii + 487 pages, 260 figures. The full text is also available at the Quarkonium Working Group web page: http://www.qwg.to.infn.it</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> CERN-2005-005 </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> CERN Yellow Report, CERN-2005-005, Geneva: CERN, 2005.- 487 p. </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> <span class="help" style="display: inline-block;"><a href="https://github.com/arXiv/arxiv-search/releases">Search v0.5.6 released 2020-02-24</a>&nbsp;&nbsp;</span> </div> </div> </main> <footer> <div class="columns is-desktop" role="navigation" aria-label="Secondary"> <!-- MetaColumn 1 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/about">About</a></li> <li><a href="https://info.arxiv.org/help">Help</a></li> </ul> 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