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href="https://arxiv.org/ps/2502.08929">ps</a>, <a href="https://arxiv.org/format/2502.08929">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"> Precise Measurement of the $蠂_{c0}$ Resonance Parameters and Branching Fractions of $蠂_{c0,c2}\to蟺^+蟺^-/K^+K^-$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (648 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="2502.08929v1-abstract-short" style="display: inline;"> By analyzing a $蠄(3686)$ data sample containing $(107.7\pm0.6)\times10^{6}$ events taken with the BESIII detector at the BEPCII storage ring in 2009, the $蠂_{c0}$ resonance parameters are precisely measured using $蠂_{c0,c2} \to 蟺^+蟺^-/K^+K^-$ events. The mass of $蠂_{c0}$ is determined to be $M(蠂_{c0})=(3415.67\pm0.07\pm0.06\pm0.07$)~MeV/$c^2$, and its full width is&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2502.08929v1-abstract-full').style.display = 'inline'; document.getElementById('2502.08929v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2502.08929v1-abstract-full" style="display: none;"> By analyzing a $蠄(3686)$ data sample containing $(107.7\pm0.6)\times10^{6}$ events taken with the BESIII detector at the BEPCII storage ring in 2009, the $蠂_{c0}$ resonance parameters are precisely measured using $蠂_{c0,c2} \to 蟺^+蟺^-/K^+K^-$ events. The mass of $蠂_{c0}$ is determined to be $M(蠂_{c0})=(3415.67\pm0.07\pm0.06\pm0.07$)~MeV/$c^2$, and its full width is $螕(蠂_{c0})=(12.44\pm0.12\pm0.12)~{\rm MeV}$, where the first uncertainty is statistical, the second systematic, and the third for mass comes from $蠂_{c2}$ mass uncertainty. These measurements improve the precision of $蠂_{c0}$ mass by a factor of four and width by one order of magnitude over the previous individual measurements, and significantly boost our knowledge about the charmonium spectrum. Together with additional $(345.4\pm2.6)\times10^{6}$ $蠄(3686)$ data events taken in 2012, the decay branching fractions of $蠂_{c0,c2}\to蟺^+蟺^-/K^+K^-$ are measured as well, with precision improved by a factor of three compared to previous measurements. These $蠂_{c0}$ decay branching fractions provide important inputs for the study of glueballs. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2502.08929v1-abstract-full').style.display = 'none'; document.getElementById('2502.08929v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 February, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2025. </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, 1 figure</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2502.07406">arXiv:2502.07406</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2502.07406">pdf</a>, <a href="https://arxiv.org/format/2502.07406">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 $e^+e^-\to K_S^0 K_S^0 h_c$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2502.07406v1-abstract-short" style="display: inline;"> Using $e^+e^-$ collision data at 13 center-of-mass energies ranging from 4.600 to 4.950 GeV collected with the BESIII detector, we search for the unmeasured $e^+e^-\to K_S^0 K_S^0 h_c$ process . No significant signal is observed, and the upper limits of the Born cross sections at each center-of-mass energy are presented. </span> <span class="abstract-full has-text-grey-dark mathjax" id="2502.07406v1-abstract-full" style="display: none;"> Using $e^+e^-$ collision data at 13 center-of-mass energies ranging from 4.600 to 4.950 GeV collected with the BESIII detector, we search for the unmeasured $e^+e^-\to K_S^0 K_S^0 h_c$ process . No significant signal is observed, and the upper limits of the Born cross sections at each center-of-mass energy are presented. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2502.07406v1-abstract-full').style.display = 'none'; document.getElementById('2502.07406v1-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, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2502.03828">arXiv:2502.03828</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2502.03828">pdf</a>, <a href="https://arxiv.org/ps/2502.03828">ps</a>, <a href="https://arxiv.org/format/2502.03828">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"> Observation of $D^+\to \bar K_1(1270)^0渭^+谓_渭$ and $D^0\to K_1(1270)^-渭^+谓_渭$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (646 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="2502.03828v1-abstract-short" style="display: inline;"> By analyzing 7.93 $\rm fb^{-1}$ of $e^+e^-$ collision data collected at the center-of-mass energy of 3.773 GeV with the BESIII detector operated at the BEPCII collider, we report the observation of the semimuonic decays of $D^+\to \bar K_1(1270)^0渭^+谓_渭$ and $D^0\to K_1(1270)^-渭^+谓_渭$ with statistical significances of $12.5蟽$ and $6.0蟽$, respectively. Their decay branching fractions are determined&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2502.03828v1-abstract-full').style.display = 'inline'; document.getElementById('2502.03828v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2502.03828v1-abstract-full" style="display: none;"> By analyzing 7.93 $\rm fb^{-1}$ of $e^+e^-$ collision data collected at the center-of-mass energy of 3.773 GeV with the BESIII detector operated at the BEPCII collider, we report the observation of the semimuonic decays of $D^+\to \bar K_1(1270)^0渭^+谓_渭$ and $D^0\to K_1(1270)^-渭^+谓_渭$ with statistical significances of $12.5蟽$ and $6.0蟽$, respectively. Their decay branching fractions are determined to be ${\mathcal B}[D^{+}\to \bar{K}_1(1270)^0 渭^{+}谓_渭]=(2.36\pm0.20^{+0.18}_{-0.27}\pm 0.48)\times10^{-3}$ and ${\mathcal B}[D^{0}\to K_1(1270)^{-} 渭^{+}谓_渭]=(0.78\pm0.11^{+0.05}_{-0.09}\pm 0.15)\times10^{-3}$, where the first and second uncertainties are statistical and systematic, respectively, and the third originates from the input branching fraction of $\bar K_{1}(1270)^0\to K^- 蟺^+蟺^0$ or $K_1(1270)^-\to K^-蟺^+蟺^-$. Combining our branching fractions with the previous measurements of ${\mathcal B}[D^+\to \bar K_1(1270)^0e^+谓_{e}]$ and ${\mathcal B}[D^0\to K_1(1270)^-e^+谓_{e}]$, we determine the branching fraction ratios to be ${\mathcal B}[D^+\to \bar K_1(1270)^0渭^+谓_渭]/{\mathcal B}[D^+\to \bar K_1(1270)^0e^+谓_{e}]=1.03 \pm 0.14 \substack{+0.11\\-0.15}$ and ${\mathcal B}[D^0\to K_1(1270)^-渭^+谓_渭]/{\mathcal B}[D^0\to K_1(1270)^-e^+谓_{e}]=0.74\pm 0.13 \substack{+0.08\\-0.13}$. Using the branching fractions measured in this work and the world-average lifetimes of the $D^+$ and $D^0$ mesons, we determine the semimuonic partial decay width ratio to be $螕[D^+\to \bar K_1(1270)^0 渭^+谓_渭]/螕[D^0\to K_1(1270)^- 渭^+谓_渭]=1.22\pm 0.10\substack{+0.06\\-0.09}$, which is consistent with unity as predicted by isospin conservation. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2502.03828v1-abstract-full').style.display = 'none'; document.getElementById('2502.03828v1-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, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2025. </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, 2 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/2501.15447">arXiv:2501.15447</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.15447">pdf</a>, <a href="https://arxiv.org/ps/2501.15447">ps</a>, <a href="https://arxiv.org/format/2501.15447">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"> Observation of $h_{c}$ radiative decays to multiple light hadrons and the tensor state $f_2(1270)$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Cai%2C+H">H. Cai</a> , et al. (666 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="2501.15447v1-abstract-short" style="display: inline;"> Using $蠄(3686)\rightarrow 蟺^{0} h_{c}$ decays from a data sample of $(27.12\pm0.14)\times10^{8}$ $蠄(3686)$ events collected by the BESIII detector at the BEPCII collider, $h_c$ radiative decays to $纬蟺^{+}蟺^{-},~纬蟺^{+}蟺^{-}畏,~\gamma2(蟺^{+}蟺^{-})$, and $纬p\bar{p}$ are observed for the first time, each with a significance greater than $5蟽$. The corresponding branching fractions are measured. Furtherm&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.15447v1-abstract-full').style.display = 'inline'; document.getElementById('2501.15447v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.15447v1-abstract-full" style="display: none;"> Using $蠄(3686)\rightarrow 蟺^{0} h_{c}$ decays from a data sample of $(27.12\pm0.14)\times10^{8}$ $蠄(3686)$ events collected by the BESIII detector at the BEPCII collider, $h_c$ radiative decays to $纬蟺^{+}蟺^{-},~纬蟺^{+}蟺^{-}畏,~\gamma2(蟺^{+}蟺^{-})$, and $纬p\bar{p}$ are observed for the first time, each with a significance greater than $5蟽$. The corresponding branching fractions are measured. Furthermore, intermediate states below 2.8 GeV/$c^{2}$ are investigated, leading to the first observation of the decay process of $h_c\rightarrow纬f_{2}(1270)\rightarrow纬蟺^{+}蟺^{-}$ with a significance of $5.5\,蟽$. This observation represents the first instance of $h_c$ radiative decay to a tensor state. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.15447v1-abstract-full').style.display = 'none'; document.getElementById('2501.15447v1-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 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.14206">arXiv:2501.14206</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.14206">pdf</a>, <a href="https://arxiv.org/ps/2501.14206">ps</a>, <a href="https://arxiv.org/format/2501.14206">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"> Cross section measurement of $e^{+}e^{-} \to f_{1}(1285)蟺^{+}蟺^{-}$ at center-of-mass energies between $3.808$ and $4.951\rm GeV$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (639 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="2501.14206v1-abstract-short" style="display: inline;"> Using data samples collected by the \mbox{BESIII} detector located at the Beijing Electron Positron Collider, the cross sections of the process $e^+e^-\to f_{1}(1285)蟺^+蟺^-$ are measured at forty-five center-of-mass energies from $3.808$ to $4.951 {\rm GeV}$. An investigation on the cross section line shape is performed, and no significant structure is observed. </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.14206v1-abstract-full" style="display: none;"> Using data samples collected by the \mbox{BESIII} detector located at the Beijing Electron Positron Collider, the cross sections of the process $e^+e^-\to f_{1}(1285)蟺^+蟺^-$ are measured at forty-five center-of-mass energies from $3.808$ to $4.951 {\rm GeV}$. An investigation on the cross section line shape is performed, and no significant structure is observed. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.14206v1-abstract-full').style.display = 'none'; document.getElementById('2501.14206v1-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, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.10130">arXiv:2501.10130</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.10130">pdf</a>, <a href="https://arxiv.org/format/2501.10130">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"> Study of $畏\rightarrow蟺^+蟺^-l^+l^-$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?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="2501.10130v1-abstract-short" style="display: inline;"> Using a sample of $(10087\pm44)\times10^{6}$ $J/蠄$ events accumulated with the BESIII detector, we analyze the decays $畏\rightarrow蟺^+蟺^-l^+l^-$ ($l=e$ or $渭$) via the process $J/蠄\rightarrow纬畏$. The branching fraction of $畏\rightarrow蟺^+蟺^-e^+e^-$ is measured to be $\mathcal{B}(畏\rightarrow蟺^+蟺^-e^+e^-)=(3.07\pm0.12_{\rm{stat.}}\pm0.19_{\rm{syst.}}) \times10^{-4}$. No signal events are observed f&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.10130v1-abstract-full').style.display = 'inline'; document.getElementById('2501.10130v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.10130v1-abstract-full" style="display: none;"> Using a sample of $(10087\pm44)\times10^{6}$ $J/蠄$ events accumulated with the BESIII detector, we analyze the decays $畏\rightarrow蟺^+蟺^-l^+l^-$ ($l=e$ or $渭$) via the process $J/蠄\rightarrow纬畏$. The branching fraction of $畏\rightarrow蟺^+蟺^-e^+e^-$ is measured to be $\mathcal{B}(畏\rightarrow蟺^+蟺^-e^+e^-)=(3.07\pm0.12_{\rm{stat.}}\pm0.19_{\rm{syst.}}) \times10^{-4}$. No signal events are observed for the $畏\rightarrow蟺^{+}蟺^{-}渭^{+}渭^{-}$ decay, leading to an upper limit on the branching fraction of $\mathcal{B}(畏\rightarrow蟺^{+}蟺^{-}渭^{+}渭^{-})&lt;4.0\times10^{-7}$ at the 90\% confidence level. Furthermore, the $CP$-violation asymmetry parameter is found to be $\mathcal{A}_{CP}(畏\rightarrow蟺^{+}蟺^{-}e^{+}e^{-})=(-4.04\pm4.69_{\rm{stat.}}\pm0.14_{\rm{syst.}})\%$, showing no evidence of $CP$-violation with current statistics. Additionally, we extract the transition form factor from the decay amplitude of $畏\rightarrow蟺^+蟺^-e^+e^-$. Finally, axion-like particles are searched for via the decay $畏\rightarrow蟺^+蟺^-a, a\rightarrow e^+e^-$, and upper limits on this branching fraction relative to that of $畏\rightarrow蟺^+蟺^-e^+e^-$ are presented as a function of the axion-like particle mass in the range $5-200\ \mathrm{MeV}/c^{2}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.10130v1-abstract-full').style.display = 'none'; document.getElementById('2501.10130v1-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 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.08080">arXiv:2501.08080</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.08080">pdf</a>, <a href="https://arxiv.org/format/2501.08080">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 the FCNC charmonium decay $J/蠄\to D^0 渭^+ 渭^- + \text{c.c.}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Cai%2C+H">H. Cai</a> , et al. (680 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="2501.08080v1-abstract-short" style="display: inline;"> Based on a data sample of $(10087 \pm 44) \times 10^6$ $J/蠄$ events taken with the BESIII detector, we search for the flavor-changing neutral current charmonium decay $J/蠄\to D^{0} 渭^{+} 渭^{-} + \text{c.c.}$. No significant signal above the background is observed, and the upper limit on its branching fraction is set to be $\mathcal{B}(J/蠄\to D^{0}渭^{+}渭^{-} + \text{c.c.} ) &lt; 1.1 \times 10^{-7}$ at&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.08080v1-abstract-full').style.display = 'inline'; document.getElementById('2501.08080v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.08080v1-abstract-full" style="display: none;"> Based on a data sample of $(10087 \pm 44) \times 10^6$ $J/蠄$ events taken with the BESIII detector, we search for the flavor-changing neutral current charmonium decay $J/蠄\to D^{0} 渭^{+} 渭^{-} + \text{c.c.}$. No significant signal above the background is observed, and the upper limit on its branching fraction is set to be $\mathcal{B}(J/蠄\to D^{0}渭^{+}渭^{-} + \text{c.c.} ) &lt; 1.1 \times 10^{-7}$ at the 90% confidence level. This marks the first search for a flavor-changing neutral current charmonium decay involving muons in the final state. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.08080v1-abstract-full').style.display = 'none'; document.getElementById('2501.08080v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">20 pages, 4 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/2501.06426">arXiv:2501.06426</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.06426">pdf</a>, <a href="https://arxiv.org/format/2501.06426">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 $K^0_S$ invisible decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2501.06426v1-abstract-short" style="display: inline;"> Based on $(1.0087\pm0.0044)\times10^{10}$ $J/蠄$ events collected with the BESIII detector at the BEPCII $e^+e^-$ storage ring, we search for $K_{S}^{0}$ invisible decays via the $J/蠄\to 蠁K_{S}^{0} K_{S}^{0}$ process. No significant signal is observed, and the upper limit of the branching fraction of these invisible decays is set at 8.4 $\times$ $10^{-4}$ at the 90\% confidence level. This is the f&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.06426v1-abstract-full').style.display = 'inline'; document.getElementById('2501.06426v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.06426v1-abstract-full" style="display: none;"> Based on $(1.0087\pm0.0044)\times10^{10}$ $J/蠄$ events collected with the BESIII detector at the BEPCII $e^+e^-$ storage ring, we search for $K_{S}^{0}$ invisible decays via the $J/蠄\to 蠁K_{S}^{0} K_{S}^{0}$ process. No significant signal is observed, and the upper limit of the branching fraction of these invisible decays is set at 8.4 $\times$ $10^{-4}$ at the 90\% confidence level. This is the first experimental search for $K^0_S$ invisible decays. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.06426v1-abstract-full').style.display = 'none'; document.getElementById('2501.06426v1-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, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.04760">arXiv:2501.04760</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.04760">pdf</a>, <a href="https://arxiv.org/format/2501.04760">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 the leptonic decay $D^{+}\to e^{+}谓_{e}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (646 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="2501.04760v1-abstract-short" style="display: inline;"> We search for the leptonic decay $D^+\to e^+谓_{e}$ using an $e^+e^-$ collision data sample with an integrated luminosity of 20.3~fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy of 3.773~GeV. No significant signal is observed and an upper limit on the branching fraction of $D^+\to e^+谓_{e}$ is set as $9.7 \times 10^{-7}$, at the 90\% confidence level. Our upper limit is an&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.04760v1-abstract-full').style.display = 'inline'; document.getElementById('2501.04760v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.04760v1-abstract-full" style="display: none;"> We search for the leptonic decay $D^+\to e^+谓_{e}$ using an $e^+e^-$ collision data sample with an integrated luminosity of 20.3~fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy of 3.773~GeV. No significant signal is observed and an upper limit on the branching fraction of $D^+\to e^+谓_{e}$ is set as $9.7 \times 10^{-7}$, at the 90\% confidence level. Our upper limit is an order of magnitude smaller than the previous limit for this decay mode. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.04760v1-abstract-full').style.display = 'none'; document.getElementById('2501.04760v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.04451">arXiv:2501.04451</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.04451">pdf</a>, <a href="https://arxiv.org/format/2501.04451">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"> Observation of the $W$-annihilation process $D_s^+ \to 蠅蟻^+$ and measurement of $D_s^+ \to 蠁蟻^+$ in $D^+_s\to 蟺^+蟺^+蟺^-蟺^0蟺^0$ decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2501.04451v1-abstract-short" style="display: inline;"> We present the first amplitude analysis and branching fraction measurement of the decay $D^+_s\to 蟺^+蟺^+蟺^-蟺^0蟺^0$, using $e^+e^-$ collision data collected with the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV corresponding to an integrated luminosity of 7.33 fb$^{-1}$, and report the first observation of the pure $W$-annihilation decay $D_s^+ \to 蠅蟻^+$ with a branching f&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.04451v1-abstract-full').style.display = 'inline'; document.getElementById('2501.04451v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.04451v1-abstract-full" style="display: none;"> We present the first amplitude analysis and branching fraction measurement of the decay $D^+_s\to 蟺^+蟺^+蟺^-蟺^0蟺^0$, using $e^+e^-$ collision data collected with the BESIII detector at center-of-mass energies between 4.128 and 4.226 GeV corresponding to an integrated luminosity of 7.33 fb$^{-1}$, and report the first observation of the pure $W$-annihilation decay $D_s^+ \to 蠅蟻^+$ with a branching fraction of $(0.99\pm0.08_{\rm stat}\pm0.07_{\rm syst})\%$. In comparison to the low significance of the $\mathcal{D}$ wave in the decay $D_s^+ \to 蠁蟻^+$, the dominance of the $\mathcal{D}$ wave over the $\mathcal{S}$ and $\mathcal{P}$ waves, with a fraction of $(51.85\pm7.28_{\rm stat}\pm7.90_{\rm syst})\%$ observed in the decay, provides crucial information for the``polarization puzzle&#34;, as well as for the understanding of charm meson decays. The branching fraction of $D^+_s\to 蟺^+蟺^+蟺^-蟺^0蟺^0$ is measured to be $(4.41\pm0.15_{\rm stat}\pm0.13_{\rm syst})\%$. Moreover, the branching fraction of $D_s^+ \to 蠁蟻^+$ is measured to be $(3.98\pm0.33_{\rm stat}\pm0.21_{\rm syst})\%$, and the $R_蠁= {\mathcal{B}(蠁\to蟺^+蟺^-蟺^0)}/{\mathcal{B}(蠁\to K^+K^-)}$ is determined to be $(0.222\pm0.019_{\rm stat}\pm0.016_{\rm syst}$), which is consistent with the previous measurement based on charm meson decays, but deviates from the results from $e^+e^-$ annihilation and $K$-$N$ scattering experiments by more than 3$蟽$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.04451v1-abstract-full').style.display = 'none'; document.getElementById('2501.04451v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.04344">arXiv:2501.04344</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.04344">pdf</a>, <a href="https://arxiv.org/format/2501.04344">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"> Study of the electromagnetic Dalitz decay $J/蠄\to e^+e^- 蟺^0$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (639 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="2501.04344v1-abstract-short" style="display: inline;"> We study the electromagnetic Dalitz decay $J/蠄\to e^+e^- 蟺^0$ using $(10087 \pm 44) \times 10^6$ $J/蠄$ events collected by the \bes detector. The di-electron-invariant-mass dependent transition form factor of this decay is explored for the first time. A significant resonant structure corresponding to the $蟻/蠅$ resonance is observed, which cannot be described by existing theoretical models, due to&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.04344v1-abstract-full').style.display = 'inline'; document.getElementById('2501.04344v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.04344v1-abstract-full" style="display: none;"> We study the electromagnetic Dalitz decay $J/蠄\to e^+e^- 蟺^0$ using $(10087 \pm 44) \times 10^6$ $J/蠄$ events collected by the \bes detector. The di-electron-invariant-mass dependent transition form factor of this decay is explored for the first time. A significant resonant structure corresponding to the $蟻/蠅$ resonance is observed, which cannot be described by existing theoretical models, due to contributions from the isospin-conserving $J/蠄\to 蟻蟺^0$ and isospin-volating $J/蠄\to 蠅蟺^0$ decays. The observed $蟻$--$蠅$ interference is consistent with that of the pion form factor but features a relatively narrow $蟻$ peak. By taking into account the contribution of this resonant structure, the branching fraction of $J/蠄\to e^+e^- 蟺^0$ in the full $e^+e^-$ invariant mass spectrum range is also measured for the first time to be $(8.06 \pm 0.31 (\rm{stat}) \pm 0.38 (\rm{syst}))\times 10^{-7}$, which is two times larger than the prediction of the Vector Meson Dominance model due to the observed resonant contribution of $蟻/蠅$ resonances. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.04344v1-abstract-full').style.display = 'none'; document.getElementById('2501.04344v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </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, 4 figures, Submitted to Phys. Rev. Lett</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> BAM-325 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.02594">arXiv:2501.02594</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.02594">pdf</a>, <a href="https://arxiv.org/format/2501.02594">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"> Observation of $蠄(3686) \to K^{-}螞(1520)\bar螢^{+} + c.c.$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2501.02594v1-abstract-short" style="display: inline;"> Based on $(2712.4 \pm 14.3)\times 10^6$ $蠄(3686)$ events collected at the BESIII detector operating at the BEPCII collider, we present the first observation of the decay $蠄(3686) \to K^{-}螞(1520)\bar螢^{+} + c.c.$. The product branching fraction ${\cal B}[蠄(3686) \to K^{-}螞(1520)\bar螢^{+} + c.c.] \times {\cal B}[螞(1520) \to pK^{-}]$ is measured to be $(9.5 \pm 0.8 \pm 1.1) \times 10^{-7}$, where th&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.02594v1-abstract-full').style.display = 'inline'; document.getElementById('2501.02594v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.02594v1-abstract-full" style="display: none;"> Based on $(2712.4 \pm 14.3)\times 10^6$ $蠄(3686)$ events collected at the BESIII detector operating at the BEPCII collider, we present the first observation of the decay $蠄(3686) \to K^{-}螞(1520)\bar螢^{+} + c.c.$. The product branching fraction ${\cal B}[蠄(3686) \to K^{-}螞(1520)\bar螢^{+} + c.c.] \times {\cal B}[螞(1520) \to pK^{-}]$ is measured to be $(9.5 \pm 0.8 \pm 1.1) \times 10^{-7}$, where the first uncertainty is statistical and the second systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.02594v1-abstract-full').style.display = 'none'; document.getElementById('2501.02594v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 5 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2501.01661">arXiv:2501.01661</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2501.01661">pdf</a>, <a href="https://arxiv.org/ps/2501.01661">ps</a>, <a href="https://arxiv.org/format/2501.01661">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 $畏_c(2S)\to p\bar{p}K^+K^-$ and measurement of $蠂_{cJ}\to p\bar{p}K^+K^-$ in $蠄(3686)$ radiative decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Cai%2C+H">H. Cai</a> , et al. (639 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="2501.01661v1-abstract-short" style="display: inline;"> A search for $畏_c(2S)\to p\bar{p}K^+K^-$, together with measurement of branching fractions of $蠂_{cJ(J=0,1,2)}\to p\bar{p}K^+K^-$ in the $蠄(3686) \to 纬畏_c(2S)$ and the $蠄(3686) \to 纬蠂_{cJ}$ radiative decays, is performed with $(2712.4\pm14.3)\times 10^6$ $蠄(3686)$ events collected with the BESIII detector at the BEPCII collider. An evidence for $畏_c(2S)\to p\bar{p}K^+K^-$ is found, with a signific&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.01661v1-abstract-full').style.display = 'inline'; document.getElementById('2501.01661v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2501.01661v1-abstract-full" style="display: none;"> A search for $畏_c(2S)\to p\bar{p}K^+K^-$, together with measurement of branching fractions of $蠂_{cJ(J=0,1,2)}\to p\bar{p}K^+K^-$ in the $蠄(3686) \to 纬畏_c(2S)$ and the $蠄(3686) \to 纬蠂_{cJ}$ radiative decays, is performed with $(2712.4\pm14.3)\times 10^6$ $蠄(3686)$ events collected with the BESIII detector at the BEPCII collider. An evidence for $畏_c(2S)\to p\bar{p}K^+K^-$ is found, with a significance of $3.3蟽$. The product branching fraction of $\mathcal{B}[蠄(3686)\to纬畏_c(2S)]\cdot\mathcal{B}[畏_c(2S)\to p\bar{p}K^+K^-]$ is determined to be $(1.98\mkern 2mu\pm\mkern 2mu0.41_{\text{stat.}}\mkern 2mu\pm\mkern 2mu0.99_{\text{syst.}})\times 10^{-7}$. The product branching fractions of $\mathcal{B}[蠄(3686)\to纬蠂_{cJ}]\cdot\mathcal{B}[蠂_{cJ}\to p\bar{p}K^+K^-]$ are measured to be $(2.49\mkern 2mu\pm\mkern 2mu 0.03_{\text{stat.}}\mkern 2mu\pm\mkern 2mu 0.15_{\text{syst.}})\times 10^{-5}$, $(1.83\mkern 2mu \pm\mkern 2mu 0.02_{\text{stat.}}\mkern 2mu \pm\mkern 2mu 0.11_{\text{syst.}})\times 10^{-5}$, and $(2.43\mkern 2mu\pm\mkern 2mu 0.02_{\text{stat.}}\mkern 2mu\pm\mkern 2mu 0.15_{\text{syst.}})\times 10^{-5}$, for $J=0,\ 1$, and 2, respectively. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2501.01661v1-abstract-full').style.display = 'none'; document.getElementById('2501.01661v1-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 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2025. </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, 2 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/2412.20305">arXiv:2412.20305</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.20305">pdf</a>, <a href="https://arxiv.org/ps/2412.20305">ps</a>, <a href="https://arxiv.org/format/2412.20305">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"> Measurement of Born cross section of $e^+e^-\to危^0\bar危^0$ at $\sqrt{s} = 3.50-4.95$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (649 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="2412.20305v1-abstract-short" style="display: inline;"> Using $e^+e^-$ collision data collected with the BESIII detector at the BEPCII collider at thirty-two center-of-mass energies from 3.50 to 4.95 GeV, corresponding to an integrated luminosity of 25 $\rm{fb^{-1}}$, we measure the Born cross section of the $e^+e^-\to危^0\bar危^0$ reaction and the effective form factor. No significant charmonium(-like) state, i.e., $蠄(3770)$, $蠄(4040)$, $蠄(4160)$,&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.20305v1-abstract-full').style.display = 'inline'; document.getElementById('2412.20305v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.20305v1-abstract-full" style="display: none;"> Using $e^+e^-$ collision data collected with the BESIII detector at the BEPCII collider at thirty-two center-of-mass energies from 3.50 to 4.95 GeV, corresponding to an integrated luminosity of 25 $\rm{fb^{-1}}$, we measure the Born cross section of the $e^+e^-\to危^0\bar危^0$ reaction and the effective form factor. No significant charmonium(-like) state, i.e., $蠄(3770)$, $蠄(4040)$, $蠄(4160)$, $蠄(4230)$, $蠄(4360)$, $蠄(4415)$, or $蠄(4660)$, decaying into the $危^0\bar危^0$ final state is observed by fitting the $e^+e^- \to 危^0\bar危^0$ dressed cross section. The upper limits for the product of the branching fraction and the electronic partial width at the 90% confidence level are provided for each assumed charmonium(-like) state. In addition, the ratios of the Born cross section and the effective form factor between the $e^+e^-\to危^0\bar危^0$ and the $e^+e^-\to危^+\bar危^-$ reactions are provided, which can be used to validate the prediction of the vector meson dominance model. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.20305v1-abstract-full').style.display = 'none'; document.getElementById('2412.20305v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 28 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">9 pages, 3 figures, 1 Supplemental Material</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2412.19702">arXiv:2412.19702</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.19702">pdf</a>, <a href="https://arxiv.org/ps/2412.19702">ps</a>, <a href="https://arxiv.org/format/2412.19702">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 the double Dalitz decays $畏/畏&#39; \to e^+e^-渭^+渭^-$ and $畏&#39; \to 渭^+渭^-渭^+渭^-$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (648 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="2412.19702v1-abstract-short" style="display: inline;"> Using a data sample of $(10087 \pm 44) \times {10^{6}}$ $J/蠄$ events collected with the BESIII detector, we search for the decays $畏/畏&#39;\to e^+e^-渭^+渭^-$ and $畏&#39; \to 渭^+渭^-渭^+渭^-$ via the radiative decays $J/蠄\to纬畏$/$纬畏&#39;$. No excess of events over expected background is observed for any of the decays of interest. At 90% confidence level, we report the first upper limits on the branching fractions o&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.19702v1-abstract-full').style.display = 'inline'; document.getElementById('2412.19702v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.19702v1-abstract-full" style="display: none;"> Using a data sample of $(10087 \pm 44) \times {10^{6}}$ $J/蠄$ events collected with the BESIII detector, we search for the decays $畏/畏&#39;\to e^+e^-渭^+渭^-$ and $畏&#39; \to 渭^+渭^-渭^+渭^-$ via the radiative decays $J/蠄\to纬畏$/$纬畏&#39;$. No excess of events over expected background is observed for any of the decays of interest. At 90% confidence level, we report the first upper limits on the branching fractions of $畏&#39; \to e^{+}e^{-}渭^{+}渭^{-}$ and $畏&#39; \to 渭^{+}渭^{-}渭^{+}渭^{-}$ to be $ 1.75 \times {10^{-6}}$ and $5.28 \times {10^{-7}}$, respectively. In addition, we set an upper limit on the branching fraction of $畏\to e^{+}e^{-}渭^{+}渭^{-}$ to be $6.88 \times {10^{-6}}$, which improves the previous result by about two orders of magnitude. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.19702v1-abstract-full').style.display = 'none'; document.getElementById('2412.19702v1-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 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">11 pages</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2412.13832">arXiv:2412.13832</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.13832">pdf</a>, <a href="https://arxiv.org/format/2412.13832">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"> Measurement of the Branching Fraction for the Decay $蠂_{cJ}\to p\bar{p}畏蟺^{0}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2412.13832v2-abstract-short" style="display: inline;"> Using $(2712.4\pm 14.3)\times10^6 蠄(3686)$ events collected by the BESIII detector operating at the BEPCII collider, we present the first observations of the decays $蠂_{cJ}(J=0,1,2)\to p\bar{p}畏蟺^{0}$. Their decay branching fractions are determined to be ${\cal B}(蠂_{c0}\to p\bar{p}畏蟺^{0})=({2.41 \pm 0.07 \pm 0.19}) \times 10^{-4}$,&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.13832v2-abstract-full').style.display = 'inline'; document.getElementById('2412.13832v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.13832v2-abstract-full" style="display: none;"> Using $(2712.4\pm 14.3)\times10^6 蠄(3686)$ events collected by the BESIII detector operating at the BEPCII collider, we present the first observations of the decays $蠂_{cJ}(J=0,1,2)\to p\bar{p}畏蟺^{0}$. Their decay branching fractions are determined to be ${\cal B}(蠂_{c0}\to p\bar{p}畏蟺^{0})=({2.41 \pm 0.07 \pm 0.19}) \times 10^{-4}$, ${\cal B}(蠂_{c1}\to p\bar{p}畏蟺^{0})=({1.95 \pm 0.05 \pm 0.12}) \times 10^{-4}$, and ${\cal B}(蠂_{c2}\to p\bar{p}畏蟺^{0})=({1.31 \pm 0.05 \pm 0.08}) \times 10^{-4}$, where the first uncertainties are statistical and the second systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.13832v2-abstract-full').style.display = 'none'; document.getElementById('2412.13832v2-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 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 18 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2412.12998">arXiv:2412.12998</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.12998">pdf</a>, <a href="https://arxiv.org/format/2412.12998">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"> Observation of the charmonium decay $畏_c\to纬纬$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Cai%2C+H">H. Cai</a> , et al. (658 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="2412.12998v1-abstract-short" style="display: inline;"> Using $(2712.4\pm14.3)\times10^{6}$ $蠄(3686)$ events collected with the BESIII detector at the BEPCII collider, the decay $畏_c\to纬纬$ in $J/蠄\to纬畏_c$ is observed for the first time. We determine the product branching fraction $\mathcal{B}(J/蠄\to纬畏_c)\times\mathcal{B}(畏_c\to纬纬)=(5.23\pm0.26_{\rm{stat.}}\pm0.30_{\rm{syst.}})\times10^{-6}$. This result is well consistent with the LQCD calculation&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.12998v1-abstract-full').style.display = 'inline'; document.getElementById('2412.12998v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.12998v1-abstract-full" style="display: none;"> Using $(2712.4\pm14.3)\times10^{6}$ $蠄(3686)$ events collected with the BESIII detector at the BEPCII collider, the decay $畏_c\to纬纬$ in $J/蠄\to纬畏_c$ is observed for the first time. We determine the product branching fraction $\mathcal{B}(J/蠄\to纬畏_c)\times\mathcal{B}(畏_c\to纬纬)=(5.23\pm0.26_{\rm{stat.}}\pm0.30_{\rm{syst.}})\times10^{-6}$. This result is well consistent with the LQCD calculation $(5.34\pm0.16)\times10^{-6}$ from HPQCD in 2023. By using the world-average values of $\mathcal{B}(J/蠄\to纬畏_c)$ and the total decay width of $畏_c$, the partial decay width $螕(畏_c\to纬纬)$ is determined to be $(11.30\pm0.56_{\rm{stat.}}\pm0.66_{\rm{syst.}}\pm1.14_{\rm{ref.}})~\rm{keV}$, which deviates from the corresponding world-average value by $3.4蟽$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.12998v1-abstract-full').style.display = 'none'; document.getElementById('2412.12998v1-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 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">10 pages, 4 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/2412.11040">arXiv:2412.11040</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.11040">pdf</a>, <a href="https://arxiv.org/format/2412.11040">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"> Amplitude analysis and branching fraction measurement of the Cabibbo-favored decay $D^+ \to K^-蟺^+蟺^+蟺^0$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (651 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="2412.11040v1-abstract-short" style="display: inline;"> An amplitude analysis of the Cabibbo-favored decay $D^+ \to K^-蟺^+蟺^+蟺^0$ is performed, using 7.93 $\rm{fb}^{-1}$ of $e^+e^-$ collision data collected with the BESIII detector at the center-of-mass energy of 3.773 GeV. The branching fractions of the intermediate processes are measured, with the dominant contribution $D^+ \to \bar{K}^{*}(892)^0蟻(770)^+$ observed to have a branching fraction of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.11040v1-abstract-full').style.display = 'inline'; document.getElementById('2412.11040v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.11040v1-abstract-full" style="display: none;"> An amplitude analysis of the Cabibbo-favored decay $D^+ \to K^-蟺^+蟺^+蟺^0$ is performed, using 7.93 $\rm{fb}^{-1}$ of $e^+e^-$ collision data collected with the BESIII detector at the center-of-mass energy of 3.773 GeV. The branching fractions of the intermediate processes are measured, with the dominant contribution $D^+ \to \bar{K}^{*}(892)^0蟻(770)^+$ observed to have a branching fraction of $(4.15\pm0.07_{\rm stat.}\pm0.17_{\rm syst.})\%$. With the detection efficiency derived from the amplitude analysis, the absolute branching fraction of $D^+ \to K^-蟺^+蟺^+蟺^0$ is measured to be $(6.06\pm0.04_{\rm stat.}\pm0.07_{\rm syst.})\%$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.11040v1-abstract-full').style.display = 'none'; document.getElementById('2412.11040v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2412.10803">arXiv:2412.10803</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.10803">pdf</a>, <a href="https://arxiv.org/format/2412.10803">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"> Study of the semileptonic decay $D^0\rightarrow \bar{K}^0蟺^-e^+谓_e$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (650 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="2412.10803v1-abstract-short" style="display: inline;"> We report an improved study of the semileptonic decay $D^0 \rightarrow \bar{K}^0蟺^-e^+谓_{e}$ based on a sample of $7.9~\mathrm{fb}^{-1}$ of $e^+e^-$ annihilation data collected at a center-of-mass energy of 3.773~GeV with the BESIII detector at the BEPCII collider. The branching fraction of this decay is measured to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.10803v1-abstract-full').style.display = 'inline'; document.getElementById('2412.10803v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.10803v1-abstract-full" style="display: none;"> We report an improved study of the semileptonic decay $D^0 \rightarrow \bar{K}^0蟺^-e^+谓_{e}$ based on a sample of $7.9~\mathrm{fb}^{-1}$ of $e^+e^-$ annihilation data collected at a center-of-mass energy of 3.773~GeV with the BESIII detector at the BEPCII collider. The branching fraction of this decay is measured to be $\mathcal{B}(D^0\rightarrow \bar{K}^0蟺^-e^+谓_{e}) = (1.444 \pm 0.022_{\rm stat} \pm 0.024_{\rm syst})\%$, which is the most precise to date, where the first uncertainty is statistical and the second is systematic. Based on investigation of the decay dynamics, we find that the decay is dominated by the $K^{*}(892)^-$ component and present an improved measurement of its branching fraction to be $\mathcal{B}(D^0\rightarrow K^{*}(892)^-e^+谓_e) = (2.039 \pm 0.032_{\rm stat} \pm 0.034_{\rm syst})\%$. We also determine the ratios of the hadronic form factors for the $K^{*}(892)^-e^+谓_e$ decay to be $r_{V} = V(0)/A_1(0) = 1.48 \pm 0.05_{\rm stat} \pm 0.02_{\rm syst}$ and $r_{2} = A_2(0)/A_1(0) = 0.70 \pm 0.04_{\rm stat} \pm 0.02_{\rm syst}$, where $V(0)$ is the vector form factor and $A_{1,2}(0)$ are the axial form factors. In addition, the $\bar{K}^0蟺^-$ $\mathcal{S}$-wave component is found to account for $(5.87 \pm 0.32_{\rm stat} \pm 0.16_{\rm syst})\%$ of the total decay rate, corresponding to a branching fraction of $\mathcal{B}[D^0\rightarrow (\bar{K}^0蟺^-)_{S-{\rm wave}}e^+谓_e] = (0.085 \pm 0.005_{\rm stat} \pm 0.003_{\rm syst})\%$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.10803v1-abstract-full').style.display = 'none'; document.getElementById('2412.10803v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">20 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/2412.06409">arXiv:2412.06409</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.06409">pdf</a>, <a href="https://arxiv.org/ps/2412.06409">ps</a>, <a href="https://arxiv.org/format/2412.06409">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"> Study of the decay 蠄(3686) \to 危^{0}\bar危^{0}蠁 </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (644 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="2412.06409v1-abstract-short" style="display: inline;"> Using $(27.12\pm 0.14)\times 10^{8}$ $蠄(3686)$ events collected with the BESIII detector operating at the BEPCII collider, the decay $蠄(3686)\to危^{0}\bar危^{0}蠁$ is observed for the first time with a statistical significance of 7.6$蟽$. Its branching fraction is measured to be $(2.64 \pm 0.32_{\textrm{stat}} \pm 0.12_{\textrm{sys}}) \times 10^{-6}$, where the first uncertainty is statistical and the&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.06409v1-abstract-full').style.display = 'inline'; document.getElementById('2412.06409v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.06409v1-abstract-full" style="display: none;"> Using $(27.12\pm 0.14)\times 10^{8}$ $蠄(3686)$ events collected with the BESIII detector operating at the BEPCII collider, the decay $蠄(3686)\to危^{0}\bar危^{0}蠁$ is observed for the first time with a statistical significance of 7.6$蟽$. Its branching fraction is measured to be $(2.64 \pm 0.32_{\textrm{stat}} \pm 0.12_{\textrm{sys}}) \times 10^{-6}$, where the first uncertainty is statistical and the second is systematic. In addition, we search for potential intermediate states in the $危^{0}蠁$($\bar危^{0}蠁$) invariant mass distribution and a possible threshold enhancement in the $危^{0}\bar危^{0}$ system, but no conclusive evidence of is observed. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.06409v1-abstract-full').style.display = 'none'; document.getElementById('2412.06409v1-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 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2412.06247">arXiv:2412.06247</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2412.06247">pdf</a>, <a href="https://arxiv.org/ps/2412.06247">ps</a>, <a href="https://arxiv.org/format/2412.06247">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"> Partial wave analyses of $蠄(3686)\to p\bar{p}蟺^0$ and $蠄(3686)\to p\bar{p}畏$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (644 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="2412.06247v1-abstract-short" style="display: inline;"> Using a sample of $(2712\pm14)\times10^6$ $蠄(3686)$ events collected with the BESIII detector, we perform partial wave analyses of the decays $蠄(3686)\to p\bar{p}蟺^0$ and $蠄(3686)\to p\bar{p}畏$. The branching fractions of $蠄(3686)\to p\bar{p}蟺^0$ and $蠄(3686)\to p\bar{p}畏$ are determined to be $(133.9\pm11.2\pm2.3)\times10^{-6}$ or $(183.7\pm13.7\pm3.2)\times10^{-6}$ and&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.06247v1-abstract-full').style.display = 'inline'; document.getElementById('2412.06247v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2412.06247v1-abstract-full" style="display: none;"> Using a sample of $(2712\pm14)\times10^6$ $蠄(3686)$ events collected with the BESIII detector, we perform partial wave analyses of the decays $蠄(3686)\to p\bar{p}蟺^0$ and $蠄(3686)\to p\bar{p}畏$. The branching fractions of $蠄(3686)\to p\bar{p}蟺^0$ and $蠄(3686)\to p\bar{p}畏$ are determined to be $(133.9\pm11.2\pm2.3)\times10^{-6}$ or $(183.7\pm13.7\pm3.2)\times10^{-6}$ and $(61.5\pm6.5\pm1.1)\times10^{-6}$ or $(84.4\pm6.9\pm1.4)\times10^{-6}$, respectively, where the two solutions are caused by an ambiguous phase angle between resonant and continuum processes. Several well-established $N^*$ states are observed in the $p蟺^0$ and $p畏$ systems, and the corresponding branching fractions are measured. The ratio of decay widths $螕_{N(1535)\to N畏}/螕_{N(1535)\to N蟺}$ is determined to be $0.99\pm0.05\pm0.17$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2412.06247v1-abstract-full').style.display = 'none'; document.getElementById('2412.06247v1-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 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> December 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">19 pages, 7 figures, submitted to PRD</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.19642">arXiv:2411.19642</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.19642">pdf</a>, <a href="https://arxiv.org/format/2411.19642">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"> Measurement of the Inclusive Cross Sections of Prompt $J/蠄$ and $蠄(3686)$ Production in $e^{+}e^{-}$ Annihilation from $\sqrt{s}=3.808$ to $4.951$ GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+M+R">M. R. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (599 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="2411.19642v1-abstract-short" style="display: inline;"> The inclusive cross sections of prompt $J/蠄$ and $蠄(3686)$ production are measured at center-of-mass energies from 3.808 to 4.951 GeV. The dataset used is 22 fb$^{-1}$ of $e^{+}e^{-}$ annihilation data collected with the BESIII detector operating at the BEPCII storage ring. The results obtained are in agreement with the previous BESIII measurements of exclusive $J/蠄$ and $蠄(3686)$ production. The&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.19642v1-abstract-full').style.display = 'inline'; document.getElementById('2411.19642v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.19642v1-abstract-full" style="display: none;"> The inclusive cross sections of prompt $J/蠄$ and $蠄(3686)$ production are measured at center-of-mass energies from 3.808 to 4.951 GeV. The dataset used is 22 fb$^{-1}$ of $e^{+}e^{-}$ annihilation data collected with the BESIII detector operating at the BEPCII storage ring. The results obtained are in agreement with the previous BESIII measurements of exclusive $J/蠄$ and $蠄(3686)$ production. The average values obtained for the cross sections measured in the center-of-mass energy ranges from 4.527 to 4.951 GeV for $J/蠄$ and from 4.843 to 4.951 GeV for $蠄(3686)$, where the impact of known resonances is negligible, are $14.0\pm1.7\pm3.1$ pb and $15.3\pm3.0$ pb, respectively. For $J/蠄$, the first and the second uncertainties are statistical and systematic, respectively. For $蠄(3686)$, the uncertainty is total. These values are useful for testing charmonium production models. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.19642v1-abstract-full').style.display = 'none'; document.getElementById('2411.19642v1-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 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 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">20 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/2411.15752">arXiv:2411.15752</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.15752">pdf</a>, <a href="https://arxiv.org/format/2411.15752">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"> Measurement of cross sections of $e^+e^-\to K^0_S K^0_S 蠄(3686)$ from $\sqrt{s}=$ 4.682 to 4.951 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2411.15752v1-abstract-short" style="display: inline;"> The process $e^+e^-\to K^0_S K^0_S 蠄(3686)$ is studied by analyzing $e^+e^-$ collision data samples collected at eight center-of-mass energies ranging from 4.682 to 4.951 GeV with the BESIII detector operating at the BEPCII collider, corresponding to an integrated luminosity of $4.1~{\rm fb}^{-1}$. Observation of the $e^+e^-\to K^0_S K^0_S 蠄(3686)$ process is found for the first time with a statis&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.15752v1-abstract-full').style.display = 'inline'; document.getElementById('2411.15752v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.15752v1-abstract-full" style="display: none;"> The process $e^+e^-\to K^0_S K^0_S 蠄(3686)$ is studied by analyzing $e^+e^-$ collision data samples collected at eight center-of-mass energies ranging from 4.682 to 4.951 GeV with the BESIII detector operating at the BEPCII collider, corresponding to an integrated luminosity of $4.1~{\rm fb}^{-1}$. Observation of the $e^+e^-\to K^0_S K^0_S 蠄(3686)$ process is found for the first time with a statistical significance of $6.3蟽$, and the cross sections at each center-of-mass energy are measured. The ratio of cross sections of $e^+e^-\to K_S^0 K_S^0 蠄(3686)$ relative to $e^+e^-\to K^+ K^- 蠄(3686)$ is determined to be $\frac{蟽(e^+e^-\to K_S^0 K_S^0 蠄(3686))}{蟽(e^+e^-\to K^+ K^- 蠄(3686))}=0.45 \pm 0.25$, which is consistent with the prediction based on isospin symmetry. The uncertainty includes both statistical and systematic contributions. Additionally, the $K_S^0蠄(3686)$ invariant mass distribution is found to be consistent with three-body phase space. The significance of a contribution beyond three-body phase space is only $0.8蟽$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.15752v1-abstract-full').style.display = 'none'; document.getElementById('2411.15752v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2411.11648">arXiv:2411.11648</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.11648">pdf</a>, <a href="https://arxiv.org/ps/2411.11648">ps</a>, <a href="https://arxiv.org/format/2411.11648">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> </div> <p class="title is-5 mathjax"> Evidence for Two Excited $惟^{-}$ Hyperons </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (650 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="2411.11648v1-abstract-short" style="display: inline;"> Using $e^+e^-$ collision data corresponding to an integrated luminosity of 19 fb$^{-1}$ collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70 GeV, we report the first evidence for a new excited $惟^{-}$ hyperon, the $惟^*(2109)^{-}$, through the process $e^+ e^- \to 惟^*(2109)^{-} \bar惟^{+} +c.c.$ with a significance of 3.7 $蟽$. The mass and width of $惟^*(2109)^{-}$ ar&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.11648v1-abstract-full').style.display = 'inline'; document.getElementById('2411.11648v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.11648v1-abstract-full" style="display: none;"> Using $e^+e^-$ collision data corresponding to an integrated luminosity of 19 fb$^{-1}$ collected by the BESIII detector at center-of-mass energies ranging from 4.13 to 4.70 GeV, we report the first evidence for a new excited $惟^{-}$ hyperon, the $惟^*(2109)^{-}$, through the process $e^+ e^- \to 惟^*(2109)^{-} \bar惟^{+} +c.c.$ with a significance of 3.7 $蟽$. The mass and width of $惟^*(2109)^{-}$ are measured to be $2108.8 \pm 5.5_{\rm stat} \pm 1.5_{\rm syst} {\rm MeV}/c^{2}$ and $21.6 \pm 17.7_{\rm stat} \pm 9.4_{\rm syst} {\rm MeV}$, respectively. We also present evidence for production of the $惟^*(2012)^{-}$ in the process $e^+ e^- \to 惟^*(2012)^{-} \bar惟^{+} +c.c.$ with a significance of 3.7 $蟽$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.11648v1-abstract-full').style.display = 'none'; document.getElementById('2411.11648v1-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 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 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, 2 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/2411.07730">arXiv:2411.07730</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2411.07730">pdf</a>, <a href="https://arxiv.org/ps/2411.07730">ps</a>, <a href="https://arxiv.org/format/2411.07730">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"> Study of the light scalar $a_{0}(980)$ through the decay $D^{0} \to a_{0}(980)^-e^{+} 谓_{e}$ with $a_{0}(980)^- \to 畏蟺^-$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (649 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="2411.07730v1-abstract-short" style="display: inline;"> Using 7.93 ${\rm fb^{-1}}$ of $e^+e^-$ collision data collected at a center-of-mass energy of 3.773 ${\rm GeV}$ with the BESIII detector, we present an analysis of the decay $D^{0} \to 畏蟺^- e^+ 谓_{e}$. The branching fraction of the decay $D^{0} \to a_{0}(980)^{-} e^+ 谓_{e}$ with $a_{0}(980)^{-} \to 畏蟺^{-}$ is measured to be $(0.86\pm0.17_{\text{stat}}\pm0.05_{\text{syst}})\times 10^{-4}$. The deca&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07730v1-abstract-full').style.display = 'inline'; document.getElementById('2411.07730v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2411.07730v1-abstract-full" style="display: none;"> Using 7.93 ${\rm fb^{-1}}$ of $e^+e^-$ collision data collected at a center-of-mass energy of 3.773 ${\rm GeV}$ with the BESIII detector, we present an analysis of the decay $D^{0} \to 畏蟺^- e^+ 谓_{e}$. The branching fraction of the decay $D^{0} \to a_{0}(980)^{-} e^+ 谓_{e}$ with $a_{0}(980)^{-} \to 畏蟺^{-}$ is measured to be $(0.86\pm0.17_{\text{stat}}\pm0.05_{\text{syst}})\times 10^{-4}$. The decay dynamics of this process is studied with a single-pole parameterization of the hadronic form factor and the Flatt茅 formula describing the $a_0(980)$ line shape in the differential decay rate. The product of the form factor $f^{ a_0}_{+}(0)$ and the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cd}|$ is determined for the first time with the result $f^{ a_0}_+(0)|V_{cd}|=0.126\pm0.013_{\rm stat}\pm0.003_{\rm syst}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2411.07730v1-abstract-full').style.display = 'none'; document.getElementById('2411.07730v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.21841">arXiv:2410.21841</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.21841">pdf</a>, <a href="https://arxiv.org/ps/2410.21841">ps</a>, <a href="https://arxiv.org/format/2410.21841">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 $螞$-$\bar螞 $ oscillation in $J/蠄\rightarrow螞\bar螞$ decay </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (638 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="2410.21841v2-abstract-short" style="display: inline;"> Using $(10087\pm44)\times 10^{6}$ $J/蠄$ decays collected by the BESIII detector at the BEPCII collider, we search for baryon number violation via $螞-\bar螞$ oscillation in the decay $J/蠄\to 螞\bar螞$. No evidence for $螞-\bar螞$ oscillation is observed. The upper limit on the time-integrated probability of $螞-\bar螞$ oscillation is estimated to be $1.4\times 10^{-6}$, corresponding to an oscillation par&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.21841v2-abstract-full').style.display = 'inline'; document.getElementById('2410.21841v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.21841v2-abstract-full" style="display: none;"> Using $(10087\pm44)\times 10^{6}$ $J/蠄$ decays collected by the BESIII detector at the BEPCII collider, we search for baryon number violation via $螞-\bar螞$ oscillation in the decay $J/蠄\to 螞\bar螞$. No evidence for $螞-\bar螞$ oscillation is observed. The upper limit on the time-integrated probability of $螞-\bar螞$ oscillation is estimated to be $1.4\times 10^{-6}$, corresponding to an oscillation parameter less than $2.1\times 10^{-18}~\mathrm{GeV}$ at $90\%$ confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.21841v2-abstract-full').style.display = 'none'; document.getElementById('2410.21841v2-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 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 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, 2 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/2410.20063">arXiv:2410.20063</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.20063">pdf</a>, <a href="https://arxiv.org/format/2410.20063">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/10.1007/JHEP01(2025)089">10.1007/JHEP01(2025)089 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of the branching fraction of $D^+ \to 蟿^+谓_蟿$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (650 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="2410.20063v3-abstract-short" style="display: inline;"> By analyzing $e^{+}e^{-}$ collision data with an integrated luminosity of 7.9~fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy of 3.773~GeV, the branching fraction of $D^+\to蟿^+谓_蟿$ is determined as $\mathcal{B}=(9.9\pm 1.1_\mathrm{stat}\pm 0.5_\mathrm{syst})\times10^{-4}$. Taking the most precise result&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.20063v3-abstract-full').style.display = 'inline'; document.getElementById('2410.20063v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.20063v3-abstract-full" style="display: none;"> By analyzing $e^{+}e^{-}$ collision data with an integrated luminosity of 7.9~fb$^{-1}$ collected with the BESIII detector at the center-of-mass energy of 3.773~GeV, the branching fraction of $D^+\to蟿^+谓_蟿$ is determined as $\mathcal{B}=(9.9\pm 1.1_\mathrm{stat}\pm 0.5_\mathrm{syst})\times10^{-4}$. Taking the most precise result $\mathcal{B}(D^+\to渭^+谓_渭)=(3.981\pm 0.079_\mathrm{stat}\pm0.040_\mathrm{syst})\times10^{-4}$, we determine $R_{蟿/渭} = 螕(D^+\to蟿^+谓_蟿)/螕(D^+\to渭^+谓_渭)= 2.49\pm0.31$, achieving a factor of two improvement in precision compared to the previous BESIII result. This measurement is in agreement with the standard model prediction of lepton flavor universality within one standard deviation. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.20063v3-abstract-full').style.display = 'none'; document.getElementById('2410.20063v3-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 February, 2025; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 26 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">Journal ref:</span> JHEP 01 (2025) 089 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.18464">arXiv:2410.18464</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.18464">pdf</a>, <a href="https://arxiv.org/ps/2410.18464">ps</a>, <a href="https://arxiv.org/format/2410.18464">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 $畏_c(2S)\to p\bar{p}$ and branching fraction measurements of $蠂_{cJ} \to p\bar{p}$ via $蠄(2S)$ radiative decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (640 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="2410.18464v1-abstract-short" style="display: inline;"> Using $(27.12\pm0.14) \times 10^{8}$ $蠄(2S)$ events collected by the BESIII detector operating at BEPCII, we search for the decay $畏_c(2S)\to p\bar{p}$ via the process $蠄(2S)\to 纬畏_c(2S)$, and only find a signal with a significance of $1.7\,蟽$. The upper limit of the product branching fraction at the 90% confidence level is determined to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18464v1-abstract-full').style.display = 'inline'; document.getElementById('2410.18464v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.18464v1-abstract-full" style="display: none;"> Using $(27.12\pm0.14) \times 10^{8}$ $蠄(2S)$ events collected by the BESIII detector operating at BEPCII, we search for the decay $畏_c(2S)\to p\bar{p}$ via the process $蠄(2S)\to 纬畏_c(2S)$, and only find a signal with a significance of $1.7\,蟽$. The upper limit of the product branching fraction at the 90% confidence level is determined to be $\mathcal{B}(蠄(2S)\to 纬畏_c(2S))\times \mathcal{B}(畏_c(2S)\to p\bar{p})&lt;2.4\times 10^{-7}$. The branching fractions of $蠂_{cJ}\to p\bar{p}~(J=0,1,2)$ are also measured to be $\mathcal{B}(蠂_{c0}\to p\bar{p})=(2.51\pm0.02\pm0.08)\times 10^{-4}$, $\mathcal{B}(蠂_{c1}\to p\bar{p})=(8.16\pm0.09\pm0.25)\times 10^{-4}$, and $\mathcal{B}(蠂_{c2}\to p\bar{p})=(8.33\pm0.09\pm0.22)\times 10^{-4}$, where the first uncertainty is statistical and the second systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.18464v1-abstract-full').style.display = 'none'; document.getElementById('2410.18464v1-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 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.16912">arXiv:2410.16912</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.16912">pdf</a>, <a href="https://arxiv.org/ps/2410.16912">ps</a>, <a href="https://arxiv.org/format/2410.16912">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"> Measurement of the branching fractions of the decays $螞_{c}^{+}\rightarrow螞K_{S}^{0}K^{+}$, $螞_{c}^{+}\rightarrow螞K_{S}^{0}蟺^{+}$ and $螞_{c}^{+}\rightarrow螞K^{*+}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (639 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="2410.16912v1-abstract-short" style="display: inline;"> Studies are performed of the Cabibbo-favored decay $螞_{c}^{+}\to螞K_{S}^{0}K^+$ and the singly Cabibbo-suppressed decay $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$, based on a sample of $e^{+}e^{-}$ collision data, corresponding to an integrated luminosity of 4.5 fb$^{-1}$, accumulated at center-of-mass energies between $4599.53$ MeV and $4698.82$ MeV with the BESIII detector. The decay&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.16912v1-abstract-full').style.display = 'inline'; document.getElementById('2410.16912v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.16912v1-abstract-full" style="display: none;"> Studies are performed of the Cabibbo-favored decay $螞_{c}^{+}\to螞K_{S}^{0}K^+$ and the singly Cabibbo-suppressed decay $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$, based on a sample of $e^{+}e^{-}$ collision data, corresponding to an integrated luminosity of 4.5 fb$^{-1}$, accumulated at center-of-mass energies between $4599.53$ MeV and $4698.82$ MeV with the BESIII detector. The decay $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$ is observed for the first time. The branching fractions of $螞_{c}^{+}\to螞K_{S}^{0}K^+$ and $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$ are measured to be $(3.04\pm0.30\pm0.16)\times 10^{-3}$ and $(1.73\pm0.27\pm0.10)\times 10^{-3}$, respectively, where the first uncertainties are statistical and the second are systematic. These results correspond to the most precise measurement of these quantities for both decays. Evidence of a $K^{*+}$ contribution in the $螞_{c}^{+}\to螞K_{S}^{0}蟺^+$ decay is found with a statistical significance of $4.7蟽$. The branching fraction of $螞_{c}^{+}\to螞K^{*+}$ is calculated under three possible interference scenarios. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.16912v1-abstract-full').style.display = 'none'; document.getElementById('2410.16912v1-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, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <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 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/10.1038/s41467-024-55042-y">10.1038/s41467-024-55042-y <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </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-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?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="2410.13515v2-abstract-short" style="display: inline;"> The beta decay of the lightest charmed baryon $螞_c^+$ provides unique insights into the fundamental mechanism of strong and electro-weak interactions, serving as a testbed for investigating non-perturbative quantum chromodynamics and constraining the Cabibbo-Kobayashi-Maskawa (CKM) matrix parameters. This article presents the first observation of the Cabibbo-suppressed decay&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13515v2-abstract-full').style.display = 'inline'; document.getElementById('2410.13515v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13515v2-abstract-full" style="display: none;"> The beta decay of the lightest charmed baryon $螞_c^+$ provides unique insights into the fundamental mechanism of strong and electro-weak interactions, serving as a testbed for investigating non-perturbative quantum chromodynamics and constraining the Cabibbo-Kobayashi-Maskawa (CKM) matrix parameters. This article presents the first observation of the Cabibbo-suppressed decay $螞_c^+ \rightarrow n e^+ 谓_{e}$, utilizing $4.5~\mathrm{fb}^{-1}$ of electron-positron annihilation data collected with the BESIII detector. A novel Graph Neural Network based technique effectively separates signals from dominant backgrounds, notably $螞_c^+ \rightarrow 螞e^+ 谓_{e}$, achieving a statistical significance exceeding $10蟽$. The absolute branching fraction 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 as $0.208\pm0.011_{\rm exp.}\pm0.007_{\rm LQCD}\pm0.001_{蟿_{螞_c^+}}$. This work highlights a new approach to further understand fundamental interactions in the charmed baryon sector, and showcases the power of modern machine learning techniques in experimental high-energy physics. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13515v2-abstract-full').style.display = 'none'; document.getElementById('2410.13515v2-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, 2025; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 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">27 pages, 5 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nature Commun. 16, 681 (2025) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.13478">arXiv:2410.13478</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.13478">pdf</a>, <a href="https://arxiv.org/format/2410.13478">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"> Observation of $蠂_{c0}\to危^{+}\bar危^{-}畏$ and evidence for $蠂_{c1,2}\to危^{+}\bar危^{-}畏$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (634 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="2410.13478v1-abstract-short" style="display: inline;"> Using $(27.12\pm 0.14)\times10^{8}$ $蠄(3686)$ events collected with the BESIII detector, the decay $蠂_{c0}\to危^{+}\bar危^{-}畏$ is observed for the first time with a statistical significance of $7.0蟽$, and evidence for $蠂_{c1}\to危^{+}\bar危^{-}畏$ and $蠂_{c2}\to危^{+}\bar危^{-}畏$ is found with statistical significances of $4.3蟽$ and $4.6蟽$, respectively. The branching fractions are determined to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13478v1-abstract-full').style.display = 'inline'; document.getElementById('2410.13478v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13478v1-abstract-full" style="display: none;"> Using $(27.12\pm 0.14)\times10^{8}$ $蠄(3686)$ events collected with the BESIII detector, the decay $蠂_{c0}\to危^{+}\bar危^{-}畏$ is observed for the first time with a statistical significance of $7.0蟽$, and evidence for $蠂_{c1}\to危^{+}\bar危^{-}畏$ and $蠂_{c2}\to危^{+}\bar危^{-}畏$ is found with statistical significances of $4.3蟽$ and $4.6蟽$, respectively. The branching fractions are determined to be $\mathcal{B}(蠂_{c0}\to危^{+}\bar危^{-}畏)=({1.26 \pm 0.20 \pm 0.13}) \times 10^{-4}, ~\mathcal{B}(蠂_{c1}\to危^{+}\bar危^{-}畏)=({5.10 \pm 1.21 \pm 0.67}) \times 10^{-5}$, and $\mathcal{B}(蠂_{c2}\to危^{+}\bar危^{-}畏)=({5.46 \pm 1.18 \pm 0.50}) \times 10^{-5}$, where the first uncertainties are statistical, and the second ones are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13478v1-abstract-full').style.display = 'none'; document.getElementById('2410.13478v1-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> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.13368">arXiv:2410.13368</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.13368">pdf</a>, <a href="https://arxiv.org/format/2410.13368">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> </div> <p class="title is-5 mathjax"> Observation of the Singly Cabibbo-Suppressed Decay $螞_c^{+}\to p蟺^0$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (638 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="2410.13368v1-abstract-short" style="display: inline;"> Utilizing 4.5${~\rm{fb}}^{-1}$ of $e^+e^-$ annihilation data collected with the BESIII detector at the BEPCII collider at center-of-mass energies between 4.600 and 4.699 GeV, the first observation of the singly Cabibbo-suppressed decay $螞_c^{+}\to p蟺^0$ is presented, with a statistical significance of $5.4蟽$. The ratio of the branching fractions of $螞_c^{+}\to p蟺^0$ and $螞_c^{+}\to p畏$ is measured&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13368v1-abstract-full').style.display = 'inline'; document.getElementById('2410.13368v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.13368v1-abstract-full" style="display: none;"> Utilizing 4.5${~\rm{fb}}^{-1}$ of $e^+e^-$ annihilation data collected with the BESIII detector at the BEPCII collider at center-of-mass energies between 4.600 and 4.699 GeV, the first observation of the singly Cabibbo-suppressed decay $螞_c^{+}\to p蟺^0$ is presented, with a statistical significance of $5.4蟽$. The ratio of the branching fractions of $螞_c^{+}\to p蟺^0$ and $螞_c^{+}\to p畏$ is measured as $\mathcal{B}(螞_c^{+}\to p蟺^0)/\mathcal{B}(螞_c^{+}\to p畏)=(0.120\pm0.026_{\rm stat.}\pm0.007_{\rm syst.})$. This result resolves the longstanding discrepancy between earlier experimental searches, providing both a decisive conclusion and valuable input for QCD-inspired theoretical models. A sophisticated deep learning approach using a Transformer-based architecture is employed to distinguish the signal from the prevalent hadronic backgrounds, complemented by thorough validation and systematic uncertainty quantification. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.13368v1-abstract-full').style.display = 'none'; document.getElementById('2410.13368v1-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">9 pages, 4 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/2410.12620">arXiv:2410.12620</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.12620">pdf</a>, <a href="https://arxiv.org/format/2410.12620">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 $e^{+}e^{-} \to 蠁蠂_{c0}$ and $蠁畏_{c2}(1D)$ at center-of-mass energies from 4.47 to 4.95 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (644 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="2410.12620v1-abstract-short" style="display: inline;"> Utilizing a data set of $6.7$ fb$^{-1}$ from electron-positron collisions recorded by the BESIII detector at the BEPCII storage ring, a search is conducted for the processes $e^{+}e^{-} \to 蠁蠂_{c0}$ and $蠁畏_{c2}(1D)$ across center-of-mass energies from 4.47 to 4.95 GeV. In the absence of any significant signals, upper limits are set. These include limits on the Born cross sections for&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12620v1-abstract-full').style.display = 'inline'; document.getElementById('2410.12620v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.12620v1-abstract-full" style="display: none;"> Utilizing a data set of $6.7$ fb$^{-1}$ from electron-positron collisions recorded by the BESIII detector at the BEPCII storage ring, a search is conducted for the processes $e^{+}e^{-} \to 蠁蠂_{c0}$ and $蠁畏_{c2}(1D)$ across center-of-mass energies from 4.47 to 4.95 GeV. In the absence of any significant signals, upper limits are set. These include limits on the Born cross sections for $e^{+}e^{-} \to 蠁蠂_{c0}$, as well as the product of the Born cross section for $e^{+}e^{-} \to 蠁畏_{c2}(1D)$ and a sum of five branching fractions. Furthermore, the product of the electronic width of $Y(4660)$ and the branching fraction of the $Y(4660) \to 蠁蠂_{c0}$, denoted as $螕^{Y(4660)}_{e^{+}e^{-}} \mathcal{B}_{Y(4660) \to 蠁蠂_{c0}}$, is determined to be $&lt; 0.40$ eV at the 90\% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.12620v1-abstract-full').style.display = 'none'; document.getElementById('2410.12620v1-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 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">14 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/2410.11607">arXiv:2410.11607</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.11607">pdf</a>, <a href="https://arxiv.org/format/2410.11607">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"> Observation of $蠂_{cJ}\to p \bar p K^0_S K^- 蟺^+ + c.c.$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (648 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="2410.11607v1-abstract-short" style="display: inline;"> By analyzing $(27.12\pm0.14)\times10^8$ $蠄(3686)$ events collected with the BESIII detector operating at the BEPCII collider, the decays of $蠂_{cJ} \to p \bar{p} K^0_S K^- 蟺^+ +c.c.(J=0, 1, 2)$ are observed for the first time with statistical significances greater than $10蟽$. The branching fractions of these decays are determined to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11607v1-abstract-full').style.display = 'inline'; document.getElementById('2410.11607v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.11607v1-abstract-full" style="display: none;"> By analyzing $(27.12\pm0.14)\times10^8$ $蠄(3686)$ events collected with the BESIII detector operating at the BEPCII collider, the decays of $蠂_{cJ} \to p \bar{p} K^0_S K^- 蟺^+ +c.c.(J=0, 1, 2)$ are observed for the first time with statistical significances greater than $10蟽$. The branching fractions of these decays are determined to be $\mathcal{B}(蠂_{c0}\to p \bar p K^{0}_{S} K^- 蟺^+ + c.c.)=(2.61\pm0.27\pm0.32)\times10^{-5},$ $\mathcal{B}(蠂_{c1}\to p \bar p K^{0}_{S} K^- 蟺^+ + c.c.)=(4.16\pm0.24\pm0.46)\times10^{-5},$ and $\mathcal{B}(蠂_{c2}\to p \bar p K^{0}_{S} K^- 蟺^+ + c.c.)=(5.63\pm0.28\pm0.46)\times10^{-5}$, respectively. The processes $蠂_{c1,2} \to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.$ are also observed, with statistical significances of 5.7$蟽$ and 7.0$蟽$, respectively. Evidence for $蠂_{c0} \to\bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.$ is found with statistical significances of 3.3$蟽$ each. The corresponding branching fractions are determined to be $\mathcal{B}(蠂_{c0}\to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.) =(1.61^{+0.68}_{-0.64}\pm0.23)\times10^{-5}$, $\mathcal{B}(蠂_{c1}\to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.)=(4.06^{+0.80}_{-0.76}\pm0.52)\times10^{-5}$, and $\mathcal{B}(蠂_{c2}\to \bar{p} 螞(1520) K^0_S 蟺^{+} + c.c.)=(4.09^{+0.87}_{-0.84}\pm0.42)\times10^{-5}$. Here, the first uncertainties are statistical and the second ones are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.11607v1-abstract-full').style.display = 'none'; document.getElementById('2410.11607v1-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 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">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/2410.08603">arXiv:2410.08603</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.08603">pdf</a>, <a href="https://arxiv.org/format/2410.08603">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"> Observation of $D^+\to畏^\prime渭^+谓_渭$ and First Study of $D^+\to 畏^\prime \ell^+谓_\ell$ Decay Dynamics </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (643 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="2410.08603v1-abstract-short" style="display: inline;"> Using $20.3\,\rm fb^{-1}$ of $e^+e^-$ collision data collected at the center-of-mass energy 3.773\,GeV with the BESIII detector, we report the first observation of the semileptonic decay $D^+\to 畏^\prime 渭^+谓_渭$ with significance of $8.6蟽$ including systematic uncertainties, and an improved measurement of $D^+\to 畏^\prime e^+谓_e$. The branching fractions of $D^+\to 畏^\prime 渭^+谓_渭$ and&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08603v1-abstract-full').style.display = 'inline'; document.getElementById('2410.08603v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.08603v1-abstract-full" style="display: none;"> Using $20.3\,\rm fb^{-1}$ of $e^+e^-$ collision data collected at the center-of-mass energy 3.773\,GeV with the BESIII detector, we report the first observation of the semileptonic decay $D^+\to 畏^\prime 渭^+谓_渭$ with significance of $8.6蟽$ including systematic uncertainties, and an improved measurement of $D^+\to 畏^\prime e^+谓_e$. The branching fractions of $D^+\to 畏^\prime 渭^+谓_渭$ and $D^+\to 畏^\prime e^+谓_e$ are determined to be $(1.92\pm0.28_{\rm stat}\pm 0.08_{\rm syst})\times 10^{-4}$ and $(1.79\pm0.19_{\rm stat}\pm 0.07_{\rm syst})\times 10^{-4}$, respectively. From an analysis of the $D^+\to 畏^\prime \ell^+谓_\ell$ decay dynamics, the product of the hadronic form factor $f_+^{畏^{\prime}}(0)$ and the CKM matrix element $|V_{cd}|$ is measured for the first time, giving $f^{畏^\prime}_+(0)|V_{cd}| = (5.92\pm0.56_{\rm stat}\pm0.13_{\rm syst})\times 10^{-2}$. No evidence for violation of $渭-e$ lepton-flavor universality is found in both the full range and several bins of $\ell^+谓_\ell$ four-momentum transfer. The $畏-畏^\prime$ mixing angle in the quark flavor basis is determined to be $蠁_{\rm P} =(39.8\pm0.8_{\rm stat}\pm0.3_{\rm syst})^\circ$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.08603v1-abstract-full').style.display = 'none'; document.getElementById('2410.08603v1-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 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.07626">arXiv:2410.07626</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.07626">pdf</a>, <a href="https://arxiv.org/format/2410.07626">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"> Precision Measurement of the Branching Fraction of $D^{+}\to 渭^{+}谓_渭$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (643 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="2410.07626v1-abstract-short" style="display: inline;"> Using $20.3~\mathrm{fb}^{-1}$ of $e^+e^-$ collision data collected at a center-of-mass energy of $E_{\rm cm}=3.773$ GeV with the BESIII detector operating at the BEPCII collider, we determine the branching fraction of the leptonic decay $D^+\to渭^+谓_渭$ to be $(3.981\pm0.079_{\rm stat}\pm0.040_{\rm syst})\times10^{-4}$. Interpreting our measurement with knowledge of the Fermi coupling constant&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.07626v1-abstract-full').style.display = 'inline'; document.getElementById('2410.07626v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.07626v1-abstract-full" style="display: none;"> Using $20.3~\mathrm{fb}^{-1}$ of $e^+e^-$ collision data collected at a center-of-mass energy of $E_{\rm cm}=3.773$ GeV with the BESIII detector operating at the BEPCII collider, we determine the branching fraction of the leptonic decay $D^+\to渭^+谓_渭$ to be $(3.981\pm0.079_{\rm stat}\pm0.040_{\rm syst})\times10^{-4}$. Interpreting our measurement with knowledge of the Fermi coupling constant $G_F$, the masses of the $D^+$ and $渭^+$ as well as the lifetime of the $D^+$, we determine $f_{D^+}|V_{cd}|=(47.53\pm0.48_{\rm stat}\pm0.24_{\rm syst}\pm0.12_{\rm input})~\mathrm{MeV}$. This result is a factor of 2.3 more precise than the previous best measurement. Using the value of the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element $|V_{cd}|$ given by the global standard model fit, we obtain the $D^+$ decay constant $f_{D^+}=(211.5\pm2.3_{\rm stat}\pm1.1_{\rm syst}\pm0.8_{\rm input})$ MeV. Alternatively, using the value of $f_{D^+}$ from a precise lattice quantum chromodynamics calculation, we extract $|V_{cd}|=0.2242\pm0.0023_{\rm stat}\pm0.0011_{\rm syst}\pm0.0009_{\rm input}$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.07626v1-abstract-full').style.display = 'none'; document.getElementById('2410.07626v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 October, 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">9 pages, 2 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/2410.06500">arXiv:2410.06500</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.06500">pdf</a>, <a href="https://arxiv.org/format/2410.06500">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 the radiative decays $D^+\to纬蟻^+$ and $D^+\to纬K^{*+}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (648 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="2410.06500v1-abstract-short" style="display: inline;"> We search for the radiative decays $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ using 20.3~fb$^{-1}$ of $e^+e^-$ annihilation data collected at the center-of-mass energy $\sqrt{s}=3.773$ GeV by the BESIII detector operating at the BEPCII collider. No significant signals are observed, and the upper limits on the branching fractions of $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ at 90\% confidence level ar&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06500v1-abstract-full').style.display = 'inline'; document.getElementById('2410.06500v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.06500v1-abstract-full" style="display: none;"> We search for the radiative decays $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ using 20.3~fb$^{-1}$ of $e^+e^-$ annihilation data collected at the center-of-mass energy $\sqrt{s}=3.773$ GeV by the BESIII detector operating at the BEPCII collider. No significant signals are observed, and the upper limits on the branching fractions of $D^{+} \to 纬蟻^+$ and $D^{+} \to 纬K^{*+}$ at 90\% confidence level are set to be $1.3\times10^{-5}$ and $1.8\times10^{-5}$, respectively. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.06500v1-abstract-full').style.display = 'none'; document.getElementById('2410.06500v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.05736">arXiv:2410.05736</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.05736">pdf</a>, <a href="https://arxiv.org/ps/2410.05736">ps</a>, <a href="https://arxiv.org/format/2410.05736">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"> Observation of an axial-vector state in the study of $蠄(3686) \to 蠁畏畏&#39;$ decay </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (625 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="2410.05736v1-abstract-short" style="display: inline;"> Using (2712.4 $\pm$ 14.3)$\times 10^{6}$ $蠄(3686)$ events collected with the BESIII detector at BEPCII, a partial wave analysis of the decay $蠄(3686) \to 蠁畏畏&#39; $ is performed with the covariant tensor approach. An axial-vector state with a mass near 2.3 $\rm GeV/c^2$ is observed for the first time. Its mass and width are measured to be 2316&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.05736v1-abstract-full').style.display = 'inline'; document.getElementById('2410.05736v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.05736v1-abstract-full" style="display: none;"> Using (2712.4 $\pm$ 14.3)$\times 10^{6}$ $蠄(3686)$ events collected with the BESIII detector at BEPCII, a partial wave analysis of the decay $蠄(3686) \to 蠁畏畏&#39; $ is performed with the covariant tensor approach. An axial-vector state with a mass near 2.3 $\rm GeV/c^2$ is observed for the first time. Its mass and width are measured to be 2316 $\pm 9_{\mathrm{stat}} \pm 30_{\mathrm{syst}}\,\rm MeV/c^2$ and 89 $\pm 15_{\mathrm{stat}} \pm 26_{\mathrm{syst}}\,\rm MeV$, respectively. The product branching fractions of $\mathcal{B}(蠄(3686) \to X(2300) 畏&#39;) \mathcal{B}(X(2300)\to 蠁畏)$ and $\mathcal{B}(蠄(3686) \to X(2300) 畏)\mathcal{B}(X(2300)\to 蠁畏&#39;)$ are determined to be (4.8 $\pm 1.3_{\mathrm{stat}} \pm 0.7_{\mathrm{syst}})\times 10^{-6}$ and (2.2 $\pm 0.7_{\mathrm{stat}} \pm 0.7_{\mathrm{syst}})\times 10^{-6}$, respectively. The branching fraction $\mathcal{B}(蠄(3686) \to 蠁畏畏&#39;)$ is measured for the first time to be (3.14$\pm0.17_{\mathrm{stat}}\pm0.24_{\mathrm{syst}})\times10^{-5}$. The first uncertainties are statistical and the second are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.05736v1-abstract-full').style.display = 'none'; document.getElementById('2410.05736v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2410.02421">arXiv:2410.02421</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2410.02421">pdf</a>, <a href="https://arxiv.org/format/2410.02421">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 lepton number violating decays of $D_s^+\to h^-h^0e^+e^+$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (650 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="2410.02421v2-abstract-short" style="display: inline;"> Based on 7.33 fb$^{-1}$ of $e^+e^-$ collision data collected by the BESIII detector operating at the BEPCII collider at center-of-mass energies from 4.128 to 4.226 GeV, a search for the Majorana neutrino $谓_m$ is conducted in the lepton-number-violating decays of $D_s^+\to h^-h^0e^+e^+$. Here, $h^-$ represents a $K^-$ or $蟺^-$, and $h^0$ represents a $蟺^0$, $K_S^0$ or $蠁$. No significant signal is&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.02421v2-abstract-full').style.display = 'inline'; document.getElementById('2410.02421v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2410.02421v2-abstract-full" style="display: none;"> Based on 7.33 fb$^{-1}$ of $e^+e^-$ collision data collected by the BESIII detector operating at the BEPCII collider at center-of-mass energies from 4.128 to 4.226 GeV, a search for the Majorana neutrino $谓_m$ is conducted in the lepton-number-violating decays of $D_s^+\to h^-h^0e^+e^+$. Here, $h^-$ represents a $K^-$ or $蟺^-$, and $h^0$ represents a $蟺^0$, $K_S^0$ or $蠁$. No significant signal is observed, and the upper limits of their branching fractions at the 90\% confidence level are determined to be $\mathcal{B}(D_s^+\to 蠁蟺^-e^+e^+) &lt; 6.9 \times 10^{-5}$, $\mathcal{B}(D_s^+\to 蠁K^-e^+e^+) &lt; 9.9 \times 10^{-5}$, $\mathcal{B}(D_s^+\to K_S^0蟺^-e^+e^+) &lt; 1.3 \times 10^{-5}$, $\mathcal{B}(D_s^+\to K_S^0K^-e^+e^+) &lt; 2.9 \times 10^{-5}$, $\mathcal{B}(D_s^+\to 蟺^-蟺^0e^+e^+) &lt; 2.9 \times 10^{-5}$ and $\mathcal{B}(D_s^+\to K^-蟺^0e^+e^+) &lt; 3.4 \times 10^{-5}$. The Majorana neutrino is searched for with different mass assumptions within the range [0.20, 0.80] GeV$/c^2$ in the decay of $D_s^+\to蠁e^+谓_m$ with $谓_m\to蟺^-e^+$, and the upper limits of the branching fractions at the 90\% confidence level are at the level of $10^{-5}-10^{-2}$, depending on the mass of the Majorana neutrino. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2410.02421v2-abstract-full').style.display = 'none'; document.getElementById('2410.02421v2-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 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 3 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.15044">arXiv:2409.15044</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.15044">pdf</a>, <a href="https://arxiv.org/ps/2409.15044">ps</a>, <a href="https://arxiv.org/format/2409.15044">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.110.112001">10.1103/PhysRevD.110.112001 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for $D^0\to K^-畏e^+谓_e$, $D^+\to K_S^0 畏e^+谓_e$ and $D^+\to 畏畏e^+谓_e$ decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (634 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="2409.15044v3-abstract-short" style="display: inline;"> By analyzing $e^+e^-$ annihilation data corresponding to an integrated luminosity of 7.93 fb$^{-1}$, collected at the center-of-mass energy of 3.773 GeV with the BESIII detector, we search for the semileptonic decays $D^0\to K^-畏e^+谓_e$, $D^+\to K_S^0 畏e^+谓_e$ and $D^+\to 畏畏e^+谓_e$ for the first time. We present evidence for $D^0\to K^-畏e^+谓_e$ with a significance of $3.3蟽$. The branching fraction&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.15044v3-abstract-full').style.display = 'inline'; document.getElementById('2409.15044v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.15044v3-abstract-full" style="display: none;"> By analyzing $e^+e^-$ annihilation data corresponding to an integrated luminosity of 7.93 fb$^{-1}$, collected at the center-of-mass energy of 3.773 GeV with the BESIII detector, we search for the semileptonic decays $D^0\to K^-畏e^+谓_e$, $D^+\to K_S^0 畏e^+谓_e$ and $D^+\to 畏畏e^+谓_e$ for the first time. We present evidence for $D^0\to K^-畏e^+谓_e$ with a significance of $3.3蟽$. The branching fraction of $D^0\to K^-畏e^+谓_e$ is measured to be $(0.84_{-0.34}^{+0.29}\pm0.22)\times 10^{-4}$. Here, the first uncertainties are statistical and the second ones are systematic. No significant signals are observed for the decays $D^+\to K_S^0 畏e^+谓_e$ and $D^+\to 畏畏e^+谓_e$ and we set the upper limits on their branching fractions. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.15044v3-abstract-full').style.display = 'none'; document.getElementById('2409.15044v3-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 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 23 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">10 pages,4 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> 110, 112001 </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. D 2024 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.07197">arXiv:2409.07197</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.07197">pdf</a>, <a href="https://arxiv.org/format/2409.07197">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"> Measurements of the $CP$-even fractions of $D^0\to蟺^{+}蟺^{-}蟺^{0}$ and $D^0\to K^{+}K^{-}蟺^{0}$ at BESIII </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (648 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="2409.07197v1-abstract-short" style="display: inline;"> The $CP$-even fractions ($F_{+}$) of the decays $D^0\to蟺^{+}蟺^{-}蟺^{0}$ and $D^0\to K^{+}K^{-}蟺^{0}$ are measured with a quantum-correlated $蠄(3770)\to D\bar{D}$ data sample collected by the BESIII experiment corresponding to an integrated luminosity of 7.93 $\mathrm{fb}^{-1}$. The results are $F_{+}^{蟺^{+}蟺^{-}蟺^{0}}=0.9406\pm0.0036\pm0.0021$ and $F_{+}^{K^{+}K^{-}蟺^{0}}=0.631\pm0.014\pm0.011$, w&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.07197v1-abstract-full').style.display = 'inline'; document.getElementById('2409.07197v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.07197v1-abstract-full" style="display: none;"> The $CP$-even fractions ($F_{+}$) of the decays $D^0\to蟺^{+}蟺^{-}蟺^{0}$ and $D^0\to K^{+}K^{-}蟺^{0}$ are measured with a quantum-correlated $蠄(3770)\to D\bar{D}$ data sample collected by the BESIII experiment corresponding to an integrated luminosity of 7.93 $\mathrm{fb}^{-1}$. The results are $F_{+}^{蟺^{+}蟺^{-}蟺^{0}}=0.9406\pm0.0036\pm0.0021$ and $F_{+}^{K^{+}K^{-}蟺^{0}}=0.631\pm0.014\pm0.011$, where the first uncertainties are statistical and the second systematic. These measurements are consistent with the previous determinations, and the uncertainties for $F_{+}^{蟺^{+}蟺^{-}蟺^{0}}$ and $F_{+}^{K^{+}K^{-}蟺^{0}}$ are reduced by factors of 3.9 and 2.6, respectively. The reported results provide important inputs for the precise measurement of the angle $纬$ of the Cabibbo-Kobayashi-Maskawa matrix and indirect $CP$ violation in charm mixing. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.07197v1-abstract-full').style.display = 'none'; document.getElementById('2409.07197v1-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 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">19 pages, 8 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/2409.04276">arXiv:2409.04276</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.04276">pdf</a>, <a href="https://arxiv.org/ps/2409.04276">ps</a>, <a href="https://arxiv.org/format/2409.04276">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"> Study of the decay $D^0\rightarrow 蟻(770)^-e^+谓_e$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (646 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="2409.04276v1-abstract-short" style="display: inline;"> We present a study of the semileptonic decay $D^0\rightarrow 蟺^-蟺^0e^{+}谓_{e}$ using an $e^+e^-$ annihilation data sample of $7.93~\mathrm{fb}^{-1}$ collected at the center-of-mass energy of 3.773 GeV with the BESIII detector. The branching fraction of $D^0\to 蟻(770)^-e^+谓_e$ is measured to be $(1.439 \pm 0.033(\rm stat.) \pm 0.027(\rm syst.)) \times10^{-3}$, which is a factor 1.6 more precise tha&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.04276v1-abstract-full').style.display = 'inline'; document.getElementById('2409.04276v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.04276v1-abstract-full" style="display: none;"> We present a study of the semileptonic decay $D^0\rightarrow 蟺^-蟺^0e^{+}谓_{e}$ using an $e^+e^-$ annihilation data sample of $7.93~\mathrm{fb}^{-1}$ collected at the center-of-mass energy of 3.773 GeV with the BESIII detector. The branching fraction of $D^0\to 蟻(770)^-e^+谓_e$ is measured to be $(1.439 \pm 0.033(\rm stat.) \pm 0.027(\rm syst.)) \times10^{-3}$, which is a factor 1.6 more precise than previous measurements. By performing an amplitude analysis, we measure the hadronic form-factor ratios of $D^0\to 蟻(770)^-e^+谓_e$ at $q^2=0$ assuming the single-pole-dominance parametrization: $r_{V}=V(0)/A_1(0)=1.548\pm0.079(\rm stat.)\pm0.041(\rm syst.)$ and $r_{2}=A_2(0)/A_1(0)=0.823\pm0.056(\rm stat.)\pm0.026(\rm syst.)$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.04276v1-abstract-full').style.display = 'none'; document.getElementById('2409.04276v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 6 September, 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">12 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/2409.02578">arXiv:2409.02578</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.02578">pdf</a>, <a href="https://arxiv.org/format/2409.02578">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 the massless dark photon with $D^0\to蠅纬&#39;$ and $D^0\to纬纬&#39;$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (648 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="2409.02578v2-abstract-short" style="display: inline;"> Using $7.9~\rm{fb^{-1}}$ of $e^+e^-$ collision data collected at $\sqrt{s}=3.773$ GeV with the BESIII detector at the BEPCII collider, we search for the massless dark photon with the flavor-changing neutral current processes $D^0\to蠅纬&#39;$ and $D^0\to纬纬&#39;$ for the first time. No significant signals are observed, and the upper limits at the 90% confidence level on the massless dark photon branching fra&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.02578v2-abstract-full').style.display = 'inline'; document.getElementById('2409.02578v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.02578v2-abstract-full" style="display: none;"> Using $7.9~\rm{fb^{-1}}$ of $e^+e^-$ collision data collected at $\sqrt{s}=3.773$ GeV with the BESIII detector at the BEPCII collider, we search for the massless dark photon with the flavor-changing neutral current processes $D^0\to蠅纬&#39;$ and $D^0\to纬纬&#39;$ for the first time. No significant signals are observed, and the upper limits at the 90% confidence level on the massless dark photon branching fraction are set to be $1.1\times10^{-5}$ and $2.0\times10^{-6}$ for $D^0\to蠅纬&#39;$ and $D^0\to纬纬&#39;$, respectively. These results provide the most stringent constraint on the new physics energy scale associated with $cu纬&#39;$ coupling in the world, with the new physics energy scale related parameter $|\mathbb{C}|^2+|\mathbb{C}_5|^2&lt;8.2\times10^{-17}~\rm{GeV}^{-2}$ at the 90% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.02578v2-abstract-full').style.display = 'none'; document.getElementById('2409.02578v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 October, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 4 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">10 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/2409.01419">arXiv:2409.01419</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.01419">pdf</a>, <a href="https://arxiv.org/format/2409.01419">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"> Study of $D^{+} \to K_{S}^{0}K^{*}(892)^{+}$ in $D^{+} \to K_{S}^{0} K_{S}^{0} 蟺^{+}$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (638 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="2409.01419v1-abstract-short" style="display: inline;"> Using a data sample of $e^+e^-$ collisions corresponding to an integrated luminosity of 7.93 $\rm fb^{-1}$ collected with the BESIII detector at the center-of-mass energy 3.773~GeV, we perform the first amplitude analysis of the decay $D^{+} \to K_{S}^{0} K_{S}^{0} 蟺^{+}$. The absolute branching fraction of $D^{+} \to K_{S}^{0}K_{S}^{0} 蟺^{+}$ is measured to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.01419v1-abstract-full').style.display = 'inline'; document.getElementById('2409.01419v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.01419v1-abstract-full" style="display: none;"> Using a data sample of $e^+e^-$ collisions corresponding to an integrated luminosity of 7.93 $\rm fb^{-1}$ collected with the BESIII detector at the center-of-mass energy 3.773~GeV, we perform the first amplitude analysis of the decay $D^{+} \to K_{S}^{0} K_{S}^{0} 蟺^{+}$. The absolute branching fraction of $D^{+} \to K_{S}^{0}K_{S}^{0} 蟺^{+}$ is measured to be $(2.97 \pm 0.09_{\rm stat.} \pm 0.05_{\rm syst.})\times10^{-3}$. The dominant intermediate process is $D^{+} \to K_{S}^{0}K^{*}(892)^{+}$, whose branching fraction is determined to be $(8.72 \pm 0.28_{\rm stat.} \pm 0.15_{\rm syst.}) \times 10^{-3}$, including all the $K^*(892)^+$ decays. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.01419v1-abstract-full').style.display = 'none'; document.getElementById('2409.01419v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 September, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2409.00427">arXiv:2409.00427</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2409.00427">pdf</a>, <a href="https://arxiv.org/format/2409.00427">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/10.1007/JHEP11(2024)062">10.1007/JHEP11(2024)062 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of Born cross sections of $e^+e^-\to螢^0\bar螢^0$ and search for charmonium(-like) states at $\sqrt{s}$ = 3.51-4.95 GeV </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (648 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="2409.00427v2-abstract-short" style="display: inline;"> Using $e^+e^-$ collision data collected by the BESIII detector at BEPCII corresponding to an integrated luminosity of 30 $\rm fb^{-1}$, we measure Born cross sections and effective form factors for the process $e^+e^-\to螢^0\bar螢^0$ at forty-five center-of-mass energies between 3.51 and 4.95 GeV. The dressed cross section is fitted, assuming a power-law function plus a charmonium(-like) state, i.e.&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.00427v2-abstract-full').style.display = 'inline'; document.getElementById('2409.00427v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2409.00427v2-abstract-full" style="display: none;"> Using $e^+e^-$ collision data collected by the BESIII detector at BEPCII corresponding to an integrated luminosity of 30 $\rm fb^{-1}$, we measure Born cross sections and effective form factors for the process $e^+e^-\to螢^0\bar螢^0$ at forty-five center-of-mass energies between 3.51 and 4.95 GeV. The dressed cross section is fitted, assuming a power-law function plus a charmonium(-like) state, i.e., $蠄(3770)$, $蠄(4040)$, $蠄(4160)$, $蠄(4230)$, $蠄(4360)$, $蠄(4415)$ or $蠄(4660)$. No significant charmonium(-like) state decaying into $螢^0\bar螢^0$ is observed. Upper limits at the 90% confidence level on the product of the branching fraction and the electronic partial width are provided for each decay. In addition, ratios of the Born cross sections and the effective form factors for $e^+e^-\to螢^0\bar螢^0$ and $e^+e^-\to螢^-\bar螢^+$ are also presented to test isospin symmetry and the vector meson dominance model. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2409.00427v2-abstract-full').style.display = 'none'; document.getElementById('2409.00427v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 31 August, 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">23 pages, 2 tables, 4 figures, consistent with the publication in JHEP05(2024)022</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> JHEP11(2024)062 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2408.17071">arXiv:2408.17071</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2408.17071">pdf</a>, <a href="https://arxiv.org/format/2408.17071">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.110.112010">10.1103/PhysRevD.110.112010 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Search for $h_c \to 蟺^+蟺^-J/蠄$ via $蠄(3686)\to 蟺^0h_c$ </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Brueggemann%2C+A">A. Brueggemann</a> , et al. (653 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="2408.17071v2-abstract-short" style="display: inline;"> Using $(2712.4 \pm 14.3) \times 10^6~蠄$(3686) events collected with the BESIII detector operating at the BEPCII collider, we search for the hadronic transition $h_c \to 蟺^+蟺^-J/蠄$ via $蠄(3686)\to 蟺^0 h_c$. No significant signal is observed. We set the most stringent upper limits to date on the branching fractions $\mathcal{B}(蠄(3686)\to 蟺^0 h_c)\times\mathcal{B}(h_c\to蟺^+蟺^-J/蠄)$ and&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.17071v2-abstract-full').style.display = 'inline'; document.getElementById('2408.17071v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2408.17071v2-abstract-full" style="display: none;"> Using $(2712.4 \pm 14.3) \times 10^6~蠄$(3686) events collected with the BESIII detector operating at the BEPCII collider, we search for the hadronic transition $h_c \to 蟺^+蟺^-J/蠄$ via $蠄(3686)\to 蟺^0 h_c$. No significant signal is observed. We set the most stringent upper limits to date on the branching fractions $\mathcal{B}(蠄(3686)\to 蟺^0 h_c)\times\mathcal{B}(h_c\to蟺^+蟺^-J/蠄)$ and $\mathcal{B}(h_c \to 蟺^+蟺^-J/蠄)$ at the 90$\%$ confidence level, which are determined to be $6.7\times 10^{-7}$ and $9.4 \times10^{-4}$, respectively. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.17071v2-abstract-full').style.display = 'none'; document.getElementById('2408.17071v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 December, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 30 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">Journal ref:</span> Phys. Rev. D 110, 112010 (2024) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2408.16654">arXiv:2408.16654</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2408.16654">pdf</a>, <a href="https://arxiv.org/format/2408.16654">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/10.1016/j.scib.2024.12.019">10.1016/j.scib.2024.12.019 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Measurement of the Decay $螢^{0}\to螞纬$ with Entangled $螢^{0}\bar螢^{0}$ Pairs </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (638 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="2408.16654v3-abstract-short" style="display: inline;"> In this Letter, a systematic study of the weak radiative hyperon decay $螢^{0}\to螞纬$ at an electron-positron collider using entangled $螢^{0}\bar螢^{0}$ pair events is presented. The absolute branching fraction for this decay has been measured for the first time, and is $\left(1.347 \pm 0.066_{\mathrm stat.}\pm0.054_{\mathrm syst.}\right)\times 10^{-3}$. The decay asymmetry parameter, which character&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.16654v3-abstract-full').style.display = 'inline'; document.getElementById('2408.16654v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2408.16654v3-abstract-full" style="display: none;"> In this Letter, a systematic study of the weak radiative hyperon decay $螢^{0}\to螞纬$ at an electron-positron collider using entangled $螢^{0}\bar螢^{0}$ pair events is presented. The absolute branching fraction for this decay has been measured for the first time, and is $\left(1.347 \pm 0.066_{\mathrm stat.}\pm0.054_{\mathrm syst.}\right)\times 10^{-3}$. The decay asymmetry parameter, which characterizes the effect of parity violation in the decay, is determined to be $-0.741 \pm 0.062_{\mathrm stat.}\pm 0.019_{\mathrm syst.}$. The obtained results are consistent with the world average values within the uncertainties, offering valuable insights into the underlying mechanism governing the weak radiative hyperon decays. The charge conjugation parity ($CP$) symmetries of branching fraction and decay asymmetry parameter in the decay are also studied. No statistically significant violation of charge conjugation parity symmetry is observed. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.16654v3-abstract-full').style.display = 'none'; document.getElementById('2408.16654v3-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 8 January, 2025; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 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">7 pages, 1 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/2408.16279">arXiv:2408.16279</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2408.16279">pdf</a>, <a href="https://arxiv.org/ps/2408.16279">ps</a>, <a href="https://arxiv.org/format/2408.16279">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"> Model-independent determination of the strong-phase difference between $D^0$ and $\bar{D}^0 \to 蟺^+蟺^-蟺^+蟺^-$ decays </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (647 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="2408.16279v2-abstract-short" style="display: inline;"> Measurements of the strong-phase difference between $D^0$ and $\bar{D}^0\to蟺^+蟺^-蟺^+蟺^-$ are performed in bins of phase space. The study exploits a sample of quantum-correlated $D\bar{D}$ mesons collected by the BESIII experiment in $e^+e^-$ collisions at a center-of-mass energy of 3.773~GeV, corresponding to an integrated luminosity of 2.93~fb$^{-1}$. Here, $D$ denotes a neutral charm meson in a&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.16279v2-abstract-full').style.display = 'inline'; document.getElementById('2408.16279v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2408.16279v2-abstract-full" style="display: none;"> Measurements of the strong-phase difference between $D^0$ and $\bar{D}^0\to蟺^+蟺^-蟺^+蟺^-$ are performed in bins of phase space. The study exploits a sample of quantum-correlated $D\bar{D}$ mesons collected by the BESIII experiment in $e^+e^-$ collisions at a center-of-mass energy of 3.773~GeV, corresponding to an integrated luminosity of 2.93~fb$^{-1}$. Here, $D$ denotes a neutral charm meson in a superposition of flavor eigenstates. The reported results are valuable for measurements of the $C\!P$-violating phase $纬$ (also denoted $蠁_3$) in $B^\pm \to DK^\pm$, $D \to 蟺^+蟺^-蟺^+蟺^-$ decays, and the binning schemes are designed to provide good statistical sensitivity to this parameter. The expected uncertainty on $纬$ arising from the precision of the strong-phase measurements, when applied to very large samples of $B$-meson decays, is around $1.5^\circ$ or $2^\circ$, depending on the binning scheme. The binned strong-phase parameters are combined to give a value of $F_+^{4蟺} = 0.746 \pm 0.010 \pm 0.004$ for the $C\!P$-even fraction of $D^0 \to 蟺^+蟺^-蟺^+蟺^-$ decays, which is around 30\% more precise than the previous best measurement of this quantity. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.16279v2-abstract-full').style.display = 'none'; document.getElementById('2408.16279v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 14 November, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 29 August, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2408.08826">arXiv:2408.08826</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2408.08826">pdf</a>, <a href="https://arxiv.org/format/2408.08826">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 the rare decay $J/蠄\to 纬D^0+c.c.$ at BESIII </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (642 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="2408.08826v1-abstract-short" style="display: inline;"> Using $(10087\pm44)\times10^6J/蠄$ events collected with the BESIII detector, we search for the rare decay $J/蠄\to 纬D^0+c.c.$ for the first time. No obvious signal is observed and the upper limit on the branching fraction is determined to be ${\cal B}(J/蠄\to 纬D^{0}+c.c.)&lt; 9.1 \times 10^{-8}$ at 90\% confidence level. </span> <span class="abstract-full has-text-grey-dark mathjax" id="2408.08826v1-abstract-full" style="display: none;"> Using $(10087\pm44)\times10^6J/蠄$ events collected with the BESIII detector, we search for the rare decay $J/蠄\to 纬D^0+c.c.$ for the first time. No obvious signal is observed and the upper limit on the branching fraction is determined to be ${\cal B}(J/蠄\to 纬D^{0}+c.c.)&lt; 9.1 \times 10^{-8}$ at 90\% confidence level. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.08826v1-abstract-full').style.display = 'none'; document.getElementById('2408.08826v1-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 August, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2024. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2408.06677">arXiv:2408.06677</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2408.06677">pdf</a>, <a href="https://arxiv.org/format/2408.06677">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Experiment">hep-ex</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="High Energy Physics - Phenomenology">hep-ph</span> </div> </div> <p class="title is-5 mathjax"> Search for $畏_c(2S)\to蠅蠅$ and $蠅蠁$ decays and measurements of $蠂_{cJ}\to蠅蠅$ and $蠅蠁$ in $蠄(2S)$ radiative processes </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/hep-ex?searchtype=author&amp;query=BESIII+Collaboration"> BESIII Collaboration</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ablikim%2C+M">M. Ablikim</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Achasov%2C+M+N">M. N. Achasov</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Adlarson%2C+P">P. Adlarson</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Afedulidis%2C+O">O. Afedulidis</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ai%2C+X+C">X. C. Ai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Aliberti%2C+R">R. Aliberti</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Amoroso%2C+A">A. Amoroso</a>, <a href="/search/hep-ex?searchtype=author&amp;query=An%2C+Q">Q. An</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bai%2C+Y">Y. Bai</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bakina%2C+O">O. Bakina</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Balossino%2C+I">I. Balossino</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Ban%2C+Y">Y. Ban</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bao%2C+H+-">H. -R. Bao</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Batozskaya%2C+V">V. Batozskaya</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Begzsuren%2C+K">K. Begzsuren</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berger%2C+N">N. Berger</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Berlowski%2C+M">M. Berlowski</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bertani%2C+M">M. Bertani</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bettoni%2C+D">D. Bettoni</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianchi%2C+F">F. Bianchi</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bianco%2C+E">E. Bianco</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Bortone%2C+A">A. Bortone</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Boyko%2C+I">I. Boyko</a>, <a href="/search/hep-ex?searchtype=author&amp;query=Briere%2C+R+A">R. A. Briere</a> , et al. (643 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="2408.06677v1-abstract-short" style="display: inline;"> Using $(2712\pm 14)$ $\times$ 10$^{6}$ $蠄(2S)$ events collected with the BESIII detector at the BEPCII collider, we search for the decays $畏_{c}(2S)\to蠅蠅$ and $畏_{c}(2S)\to蠅蠁$ via the process $蠄(2S)\to纬畏_{c}(2S)$. Evidence of $畏_{c}(2S)\to蠅蠅$ is found with a statistical significance of $3.2蟽$. The branching fraction is measured to be&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.06677v1-abstract-full').style.display = 'inline'; document.getElementById('2408.06677v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2408.06677v1-abstract-full" style="display: none;"> Using $(2712\pm 14)$ $\times$ 10$^{6}$ $蠄(2S)$ events collected with the BESIII detector at the BEPCII collider, we search for the decays $畏_{c}(2S)\to蠅蠅$ and $畏_{c}(2S)\to蠅蠁$ via the process $蠄(2S)\to纬畏_{c}(2S)$. Evidence of $畏_{c}(2S)\to蠅蠅$ is found with a statistical significance of $3.2蟽$. The branching fraction is measured to be $\mathcal{B}(畏_{c}(2S)\to蠅蠅)=(5.65\pm3.77(\rm stat.)\pm5.32(\rm syst.))\times10^{-4}$. No statistically significant signal is observed for the decay $畏_{c}(2S)\to蠅蠁$. The upper limit of the branching fraction at the 90\% confidence level is determined to be $\mathcal{B}(蠄(2S)\to纬畏_{c}(2S),畏_{c}(2S)\to蠅蠁)&lt;2.24\times 10^{-7}$. We also update the branching fractions of $蠂_{cJ}\to 蠅蠅$ and $蠂_{cJ}\to蠅蠁$ decays via the $蠄(2S)\to纬蠂_{cJ}$ transition. The branching fractions are determined to be $\mathcal{B}(蠂_{c0}\to蠅蠅)=(10.63\pm0.11\pm0.46)\times 10^{-4}$, $\mathcal{B}(蠂_{c1}\to蠅蠅)=(6.39\pm0.07\pm0.29)\times 10^{-4}$, $\mathcal{B}(蠂_{c2}\to蠅蠅)=(8.50\pm0.08\pm0.38)\times 10^{-4}$, $\mathcal{B}(蠂_{c0}\to蠅蠁)=(1.18\pm0.03\pm0.05)\times 10^{-4}$, $\mathcal{B}(蠂_{c1}\to蠅蠁)=(2.03\pm0.15\pm0.12)\times 10^{-5}$, and $\mathcal{B}(蠂_{c2}\to蠅蠁)=(9.37\pm1.07\pm0.59)\times 10^{-6}$, where the first uncertainties are statistical and the second are systematic. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2408.06677v1-abstract-full').style.display = 'none'; document.getElementById('2408.06677v1-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, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2024. </p> </li> </ol> <nav 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