{"id":2,"date":"2018-12-20T16:09:33","date_gmt":"2018-12-20T13:09:33","guid":{"rendered":"http:\/\/belle.lebedev.ru\/bsm\/?page_id=2"},"modified":"2020-09-17T17:52:58","modified_gmt":"2020-09-17T14:52:58","slug":"publications","status":"publish","type":"page","link":"https:\/\/belle.lebedev.ru\/bsm\/publications\/","title":{"rendered":"\u041f\u0443\u0431\u043b\u0438\u043a\u0430\u0446\u0438\u0438"},"content":{"rendered":"<h3 align=\"center\">2020 \u0433\u043e\u0434<\/h3>\n<div class=\"publication-archive\">\n<ol style=\"padding: 0; padding-left: 18pt;\">\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurements of production cross sections of <nobr><span class='MathJax_Preview'>\\(W Z\\)<\/span><script type='math\/tex'>W Z<\/script><\/nobr> and same-sign <nobr><span class='MathJax_Preview'>\\(W W\\)<\/span><script type='math\/tex'>W W<\/script><\/nobr> boson pairs in association with two jets in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 809 (2020) 135710<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2020.135710\" target=\"_blank\">10.1016\/j.physletb.2020.135710<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4136'); div.style.display = '';}\"> &#8230; \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c &#8230;<\/span><span class=\"description\" id=\"4136\" style=\"display: none;\">Measurements of production cross sections of <nobr><span class='MathJax_Preview'>\\(W Z\\)<\/span><script type='math\/tex'>W Z<\/script><\/nobr> and same-sign <nobr><span class='MathJax_Preview'>\\(W W\\)<\/span><script type='math\/tex'>W W<\/script><\/nobr> boson pairs in association with two jets in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV at the LHC are reported. The data sample corresponds to an integrated luminosity of <nobr>137&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>,<\/nobr> collected with the CMS detector during 2016&ndash;2018. The measurements are performed in the leptonic decay modes <nobr><span class='MathJax_Preview'>\\(W^\\pm Z \\to {\\cal l}^\\pm \\nu {\\cal l}^{\\prime \\pm} {\\cal l}^{\\prime \\mp}\\)<\/span><script type='math\/tex'>W^\\pm Z \\to {\\cal l}^\\pm \\nu {\\cal l}^{\\prime \\pm} {\\cal l}^{\\prime \\mp}<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(W^\\pm W^\\pm \\to {\\cal l}^\\pm \\nu {\\cal l}^{\\prime \\pm} \\nu\\)<\/span><script type='math\/tex'>W^\\pm W^\\pm \\to {\\cal l}^\\pm \\nu {\\cal l}^{\\prime \\pm} \\nu<\/script>,<\/nobr> where <nobr><span class='MathJax_Preview'>\\({\\cal l}, {\\cal l}^\\prime = e, \\mu\\)<\/span><script type='math\/tex'>{\\cal l}, {\\cal l}^\\prime = e, \\mu<\/script>.<\/nobr> Differential fiducial cross sections as functions of the invariant masses of the jet and charged lepton pairs, as well as of the leading-lepton transverse momentum, are measured for <nobr><span class='MathJax_Preview'>\\(W^\\pm W^\\pm\\)<\/span><script type='math\/tex'>W^\\pm W^\\pm<\/script><\/nobr> production and are consistent with the standard model predictions. The dependence of differential cross sections on the invariant mass of the jet pair is also measured for <nobr><span class='MathJax_Preview'>\\(W Z\\)<\/span><script type='math\/tex'>W Z<\/script><\/nobr> production. An observation of electroweak production of <nobr><span class='MathJax_Preview'>\\(W Z\\)<\/span><script type='math\/tex'>W Z<\/script><\/nobr> boson pairs is reported with an observed (expected) significance of 6.8 (5.3) standard deviations. Constraints are obtained on the structure of quartic vector boson interactions in the framework of effective field theory.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of CKM matrix elements in single top quark <nobr><span class='MathJax_Preview'>\\(t\\)<\/span><script type='math\/tex'>t<\/script>-channel<\/nobr> production in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 808 (2020) 135609<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2020.135609\" target=\"_blank\">10.1016\/j.physletb.2020.135609<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4127'); div.style.display = '';}\"> &#8230; \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c &#8230;<\/span><span class=\"description\" id=\"4127\" style=\"display: none;\">The first direct, model-independent measurement is presented of the modulus of the Cabibbo\u2013Kobayashi\u2013Maskawa (CKM) matrix elements <nobr><span class='MathJax_Preview'>\\(|V_{tb}|\\)<\/span><script type='math\/tex'>|V_{tb}|<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(|V_{td}|\\)<\/span><script type='math\/tex'>|V_{td}|<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\(|V_{ts}|\\)<\/span><script type='math\/tex'>|V_{ts}|<\/script>,<\/nobr> in final states enriched in single top quark <nobr><span class='MathJax_Preview'>\\(t\\)<\/span><script type='math\/tex'>t<\/script>-channel<\/nobr> events. The analysis uses proton-proton collision data from the LHC, collected during 2016 by the CMS experiment, at a centre-of-mass energy of 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> Processes directly sensitive to these matrix elements are considered at both the production and decay vertices of the top quark. In the standard model hypothesis of CKM unitarity, a lower limit of <nobr><span class='MathJax_Preview'>\\(|V_{tb}| > 0.970\\)<\/span><script type='math\/tex'>|V_{tb}| > 0.970<\/script><\/nobr> is measured at the 95% confidence level. Several theories beyond the standard model are considered, and by releasing all constraints among the involved parameters, the values <nobr><span class='MathJax_Preview'>\\(|V_{tb}| = 0.988 \\pm 0.024\\)<\/span><script type='math\/tex'>|V_{tb}| = 0.988 \\pm 0.024<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\(|V_{td}|^2 + |V_{ts}|^2 = 0.06 \\pm 0.06\\)<\/span><script type='math\/tex'>|V_{td}|^2 + |V_{ts}|^2 = 0.06 \\pm 0.06<\/script>,<\/nobr> where the uncertainties include both statistical and systematic components, are measured.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script><\/nobr> pair production cross section and search for resonances decaying to <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S) \\mu^+ \\mu^-\\)<\/span><script type='math\/tex'>\\Upsilon(1S) \\mu^+ \\mu^-<\/script><\/nobr> in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 808 (2020) 135578<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2020.135578\" target=\"_blank\">10.1016\/j.physletb.2020.135578<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3835'); div.style.display = '';}\"> &#8230; \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c &#8230;<\/span><span class=\"description\" id=\"3835\" style=\"display: none;\">The fiducial cross section for <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script><\/nobr> pair production in proton-proton collisions at a center-of-mass energy of 13&nbsp;TeV in the region where both <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script><\/nobr> mesons have an absolute rapidity below 2.0 is measured to be <nobr><span class='MathJax_Preview'>\\(79 \\pm 11\\ (\\)<\/span><script type='math\/tex'>79 \\pm 11\\ (<\/script>stat<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ \\pm 6\\ (\\)<\/span><script type='math\/tex'>)\\ \\pm 6\\ (<\/script>syst<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ \\pm 3 ({\\cal B})\\)<\/span><script type='math\/tex'>)\\ \\pm 3 ({\\cal B})<\/script>&nbsp;pb<\/nobr> assuming the mesons are produced unpolarized. The last uncertainty corresponds to the uncertainty in the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script><\/nobr> meson dimuon branching fraction. The measurement is performed in the final state with four muons using proton-proton collision data collected in 2016 by the CMS experiment at the LHC, corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> This process serves as a standard model reference in a search for narrow resonances decaying to <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S) \\mu^+ \\mu^-\\)<\/span><script type='math\/tex'>\\Upsilon(1S) \\mu^+ \\mu^-<\/script><\/nobr> in the same final state. Such a resonance could indicate the existence of a tetraquark that is a bound state of two <nobr><span class='MathJax_Preview'>\\(b\\)<\/span><script type='math\/tex'>b<\/script><\/nobr> quarks and two <nobr><span class='MathJax_Preview'>\\(\\overline{b}\\)<\/span><script type='math\/tex'>\\overline{b}<\/script><\/nobr> antiquarks. The tetraquark search is performed for masses in the vicinity of four times the bottom quark mass, between 17.5 and 19.5&nbsp;GeV, while a generic search for other resonances is performed for masses between 16.5 and 27&nbsp;GeV. No significant excess of events compatible with a narrow resonance is observed in the data. Limits on the production cross section times branching fraction to four muons via an intermediate <nobr><span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script><\/nobr> resonance are set as a function of the resonance mass.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Heavy flavor spectroscopy results from CMS<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Sergey Polikarpov<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Proceedings of Science (Beauty2019) 011<br \/>DOI: <a href=\"https:\/\/doi.org\/10.22323\/1.377.0011\" target=\"_blank\">10.22323\/1.377.0011<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('213'); div.style.display = '';}\"> &#8230; \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c &#8230;<\/span><span class=\"description\" id=\"213\" style=\"display: none;\">The observation of the <nobr><span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0 \\to B^0 K_S^0\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0 \\to B^0 K_S^0<\/script><\/nobr> decay and the evidence for the <nobr><span class='MathJax_Preview'>\\(B_{s1}(5830)^0 \\to B^{*0} K_S^0\\)<\/span><script type='math\/tex'>B_{s1}(5830)^0 \\to B^{*0} K_S^0<\/script><\/nobr> decay by the CMS experiment are reported, as well as the study of the <nobr><span class='MathJax_Preview'>\\(B^+ \\to J\/\\psi \\Lambda p\\)<\/span><script type='math\/tex'>B^+ \\to J\/\\psi \\Lambda p<\/script><\/nobr> decay, performed using the data collected in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script><\/nobr> = 8&nbsp;TeV. In addition, the observation of the <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0 \\to J\/\\psi \\Lambda \\phi\\)<\/span><script type='math\/tex'>\\Lambda_b^0 \\to J\/\\psi \\Lambda \\phi<\/script><\/nobr> decay and measurement of its branching fraction, relative to the <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0 \\to \\psi(2S) \\Lambda\\)<\/span><script type='math\/tex'>\\Lambda_b^0 \\to \\psi(2S) \\Lambda<\/script><\/nobr> decay, using the proton-proton collision data collected at at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV is presented.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for a light pseudoscalar Higgs boson in the boosted <nobr><span class='MathJax_Preview'>\\(\\mu \\mu \\tau \\tau\\)<\/span><script type='math\/tex'>\\mu \\mu \\tau \\tau<\/script><\/nobr> final state in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2008 (2020) 139<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP08(2020)139\" target=\"_blank\">10.1007\/JHEP08(2020)139<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4159'); div.style.display = '';}\"> &#8230; \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c &#8230;<\/span><span class=\"description\" id=\"4159\" style=\"display: none;\">A search for a light pseudoscalar Higgs boson <nobr><span class='MathJax_Preview'>\\((a)\\)<\/span><script type='math\/tex'>(a)<\/script><\/nobr> decaying from the 125&nbsp;GeV (or a heavier) scalar Higgs boson <nobr><span class='MathJax_Preview'>\\((H)\\)<\/span><script type='math\/tex'>(H)<\/script><\/nobr> is performed using the 2016 LHC proton-proton collision data at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>,<\/nobr> collected by the CMS experiment. The analysis considers gluon fusion and vector boson fusion production of the <nobr><span class='MathJax_Preview'>\\(H\\)<\/span><script type='math\/tex'>H<\/script>,<\/nobr> followed by the decay <nobr><span class='MathJax_Preview'>\\(H \\to a a \\to \\mu \\mu \\tau \\tau\\)<\/span><script type='math\/tex'>H \\to a a \\to \\mu \\mu \\tau \\tau<\/script>,<\/nobr> and considers pseudoscalar masses in the range <nobr><span class='MathJax_Preview'>\\(3.6 < m_a < 21\\)<\/span><script type='math\/tex'>3.6 < m_a < 21<\/script>&nbsp;GeV.<\/nobr> Because of the large mass difference between the <nobr><span class='MathJax_Preview'>\\(H\\)<\/span><script type='math\/tex'>H<\/script><\/nobr> and the <nobr><span class='MathJax_Preview'>\\(a\\)<\/span><script type='math\/tex'>a<\/script><\/nobr> bosons and the small masses of the <nobr><span class='MathJax_Preview'>\\(a\\)<\/span><script type='math\/tex'>a<\/script><\/nobr> boson decay products, both the <nobr><span class='MathJax_Preview'>\\(\\mu \\mu\\)<\/span><script type='math\/tex'>\\mu \\mu<\/script><\/nobr> and the <nobr><span class='MathJax_Preview'>\\(\\tau \\tau\\)<\/span><script type='math\/tex'>\\tau \\tau<\/script><\/nobr> pairs have high Lorentz boost and are collimated. The <nobr><span class='MathJax_Preview'>\\(\\tau \\tau\\)<\/span><script type='math\/tex'>\\tau \\tau<\/script><\/nobr> reconstruction efficiency is increased by modifying the standard technique for hadronic <nobr><span class='MathJax_Preview'>\\(\\tau\\)<\/span><script type='math\/tex'>\\tau<\/script><\/nobr> lepton decay reconstruction to account for a nearby muon. No significant signal is observed. Model-independent limits are set at 95% confidence level, as a function of <nobr><span class='MathJax_Preview'>\\(m_a\\)<\/span><script type='math\/tex'>m_a<\/script>,<\/nobr> on the branching fraction <nobr><span class='MathJax_Preview'>\\(({\\cal B})\\)<\/span><script type='math\/tex'>({\\cal B})<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(H \\to a a \\to \\mu \\mu \\tau \\tau\\)<\/span><script type='math\/tex'>H \\to a a \\to \\mu \\mu \\tau \\tau<\/script>,<\/nobr> down to <nobr><span class='MathJax_Preview'>\\(1.5\\ (2.0) \\times 10^{-4}\\)<\/span><script type='math\/tex'>1.5\\ (2.0) \\times 10^{-4}<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(m_H = 125\\ (300)\\)<\/span><script type='math\/tex'>m_H = 125\\ (300)<\/script>&nbsp;GeV.<\/nobr> Model-dependent limits on <nobr><span class='MathJax_Preview'>\\({\\cal B}(H \\to a a)\\)<\/span><script type='math\/tex'>{\\cal B}(H \\to a a)<\/script><\/nobr> are set within the context of two Higgs doublets plus singlet models, with the most stringent results obtained for Type-III models. These results extend current LHC searches for heavier <nobr><span class='MathJax_Preview'>\\(a\\)<\/span><script type='math\/tex'>a<\/script><\/nobr> bosons that decay to resolved lepton pairs and provide the first such bounds for an <nobr><span class='MathJax_Preview'>\\(H\\)<\/span><script type='math\/tex'>H<\/script><\/nobr> boson with a mass above 125&nbsp;GeV.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">The <nobr><span class='MathJax_Preview'>\\(XYZ\\)<\/span><script type='math\/tex'>XYZ<\/script><\/nobr> states: Experimental and theoretical status and perspectives<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>N.&nbsp;Brambilla, S.&nbsp;Eidelman, C.&nbsp;Hanhart, A.&nbsp;Nefediev, C.-P.&nbsp;Shen, C.E.&nbsp;Thomas, A.&nbsp;Vairo, C.-Z.&nbsp;Yuan<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Reports 873 (2020) 1\u2013154<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physrep.2020.05.001\" target=\"_blank\">10.1016\/j.physrep.2020.05.001<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2932'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2932\" style=\"display: none;\">The quark model was formulated in 1964 to classify mesons as bound states made of a quark&ndash;antiquark pair, and baryons as bound states made of three quarks. For a long time all known mesons and baryons could be classified within this scheme. Quantum Chromodynamics (QCD), however, in principle also allows the existence of more complex structures, generically called exotic hadrons or simply exotics. These include four-quark hadrons (tetraquarks and hadronic molecules), five-quark hadrons (pentaquarks) and states with active gluonic degrees of freedom (hybrids), and even states of pure glue (glueballs). Exotic hadrons have been systematically searched for in numerous experiments for many years. Remarkably, in the past fifteen years, many new hadrons that do not exhibit the expected properties of ordinary (not exotic) hadrons have been discovered in the quarkonium spectrum. These hadrons are collectively known as <nobr><span class='MathJax_Preview'>\\(XYZ\\)<\/span><script type='math\/tex'>XYZ<\/script><\/nobr> states. Some of them, like the charged states, are undoubtedly exotic. Parallel to the experimental progress, the last decades have also witnessed an enormous theoretical effort to reach a theoretical understanding of the <nobr><span class='MathJax_Preview'>\\(XYZ\\)<\/span><script type='math\/tex'>XYZ<\/script><\/nobr> states. Theoretical approaches include not only phenomenological extensions of the quark model to exotics, but also modern non-relativistic effective field theories and lattice QCD calculations. The present work aims at reviewing the rapid progress in the field of exotic <nobr><span class='MathJax_Preview'>\\(XYZ\\)<\/span><script type='math\/tex'>XYZ<\/script><\/nobr> hadrons over the past few years both in experiments and theory. It concludes with a summary on future prospects and challenges.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the associated production of a <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson with charm or bottom quark jets in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 102 (2020) 032007<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.102.032007\" target=\"_blank\">10.1103\/PhysRevD.102.032007<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3765'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3765\" style=\"display: none;\">Ratios of cross sections, <nobr><span class='MathJax_Preview'>\\(\\sigma(Z + c\\ \\)<\/span><script type='math\/tex'>\\sigma(Z + c\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\/\\sigma(Z +\\ \\)<\/span><script type='math\/tex'>)\/\\sigma(Z +\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\\)<\/span><script type='math\/tex'>)<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\sigma(Z + b\\ \\)<\/span><script type='math\/tex'>\\sigma(Z + b\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\/\\sigma(Z +\\ \\)<\/span><script type='math\/tex'>)\/\\sigma(Z +\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\\)<\/span><script type='math\/tex'>)<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\(\\sigma(Z + c\\ \\)<\/span><script type='math\/tex'>\\sigma(Z + c\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\/\\sigma(Z + b\\ \\)<\/span><script type='math\/tex'>)\/\\sigma(Z + b\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\\)<\/span><script type='math\/tex'>)<\/script><\/nobr> in the associated production of a <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson with at least one charm or bottom quark jet are measured in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV. The data sample, collected by the CMS experiment at the CERN LHC, corresponds to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>,<\/nobr> with a fiducial volume of <nobr><span class='MathJax_Preview'>\\(p_T > 30\\)<\/span><script type='math\/tex'>p_T > 30<\/script>&nbsp;GeV<\/nobr> and <nobr><span class='MathJax_Preview'>\\(|\\eta| < 2.4\\)<\/span><script type='math\/tex'>|\\eta| < 2.4<\/script><\/nobr> for the jets, where <nobr><span class='MathJax_Preview'>\\(p_T\\)<\/span><script type='math\/tex'>p_T<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(\\eta\\)<\/span><script type='math\/tex'>\\eta<\/script><\/nobr> represent transverse momentum and pseudorapidity, respectively. The <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson candidates come from leptonic decays into electrons or muons with <nobr><span class='MathJax_Preview'>\\(p_T > 25\\)<\/span><script type='math\/tex'>p_T > 25<\/script>&nbsp;GeV<\/nobr> and <nobr><span class='MathJax_Preview'>\\(|\\eta| < 2.4\\)<\/span><script type='math\/tex'>|\\eta| < 2.4<\/script>,<\/nobr> and the dilepton mass satisfies <nobr><span class='MathJax_Preview'>\\(71 < m_Z < 111\\)<\/span><script type='math\/tex'>71 < m_Z < 111<\/script>&nbsp;GeV.<\/nobr> The measured values are <nobr><span class='MathJax_Preview'>\\(\\sigma(Z + c\\ \\)<\/span><script type='math\/tex'>\\sigma(Z + c\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\/\\sigma(Z +\\ \\)<\/span><script type='math\/tex'>)\/\\sigma(Z +\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ = 0.102 \\pm 0.002 \\pm 0.009\\)<\/span><script type='math\/tex'>)\\ = 0.102 \\pm 0.002 \\pm 0.009<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\sigma(Z + b\\ \\)<\/span><script type='math\/tex'>\\sigma(Z + b\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\/\\sigma(Z +\\ \\)<\/span><script type='math\/tex'>)\/\\sigma(Z +\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ =\\)<\/span><script type='math\/tex'>)\\ =<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(0.0633 \\pm 0.0004 \\pm 0.0015\\)<\/span><script type='math\/tex'>0.0633 \\pm 0.0004 \\pm 0.0015<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\(\\sigma(Z + c\\ \\)<\/span><script type='math\/tex'>\\sigma(Z + c\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\/\\sigma(Z + b\\ \\)<\/span><script type='math\/tex'>)\/\\sigma(Z + b\\ <\/script>jets<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ = 1.62 \\pm 0.03 \\pm 0.15\\)<\/span><script type='math\/tex'>)\\ = 1.62 \\pm 0.03 \\pm 0.15<\/script>.<\/nobr> Results on the inclusive and differential cross section ratios as functions of jet and <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson transverse momentum are compared with predictions from leading and next-to-leading order perturbative quantum chromodynamics calculations. These are the first measurements of the cross section ratios at 13&nbsp;TeV.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for physics beyond the standard model in events with jets and two same-sign or at least three charged leptons in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">European Physical Journal C 80 (2020) 752<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1140\/epjc\/s10052-020-8168-3\" target=\"_blank\">10.1140\/epjc\/s10052-020-8168-3<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3773'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3773\" style=\"display: none;\">A data sample of events from proton-proton collisions with at least two jets, and two isolated same-sign or three or more charged leptons, is studied in a search for signatures of new physics phenomena. The data correspond to an integrated luminosity of <nobr>137&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> at a center-of-mass energy of 13&nbsp;TeV, collected in 2016&ndash;2018 by the CMS experiment at the LHC. The search is performed using a total of 168 signal regions defined using several kinematic variables. The properties of the events are found to be consistent with the expectations from standard model processes. Exclusion limits at 95% confidence level are set on cross sections for the pair production of gluinos or squarks for various decay scenarios in the context of supersymmetric models conserving or violating <nobr><span class='MathJax_Preview'>\\(R\\)<\/span><script type='math\/tex'>R<\/script><\/nobr> parity. The observed lower mass limits are as large as 2.1&nbsp;TeV for gluinos and 0.9&nbsp;TeV for top and bottom squarks. To facilitate reinterpretations, model-independent limits are provided in a set of simplified signal regions.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Combination of the <nobr><span class='MathJax_Preview'>\\(W\\)<\/span><script type='math\/tex'>W<\/script><\/nobr> boson polarization measurements in top quark decays using ATLAS and CMS data at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 8&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>ATLAS and CMS Collaborations<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2008 (2020) 051<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP08(2020)051\" target=\"_blank\">10.1007\/JHEP08(2020)051<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4139'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4139\" style=\"display: none;\">The combination of measurements of the <nobr><span class='MathJax_Preview'>\\(W\\)<\/span><script type='math\/tex'>W<\/script><\/nobr> boson polarization in top quark decays performed by the ATLAS and CMS collaborations is presented. The measurements are based on proton-proton collision data produced at the LHC at a centre-of-mass energy of 8&nbsp;TeV, and corresponding to an integrated luminosity of about <nobr>20&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> for each experiment. The measurements used events containing one lepton and having different jet multiplicities in the final state. The results are quoted as fractions of <nobr><span class='MathJax_Preview'>\\(W\\)<\/span><script type='math\/tex'>W<\/script><\/nobr> bosons with longitudinal <nobr><span class='MathJax_Preview'>\\((F_0)\\)<\/span><script type='math\/tex'>(F_0)<\/script>,<\/nobr> left-handed <nobr><span class='MathJax_Preview'>\\((F_L)\\)<\/span><script type='math\/tex'>(F_L)<\/script>,<\/nobr> or right-handed <nobr><span class='MathJax_Preview'>\\((F_R)\\)<\/span><script type='math\/tex'>(F_R)<\/script><\/nobr> polarizations. The resulting combined measurements of the polarization fractions are <nobr><span class='MathJax_Preview'>\\(F_0 = 0.693 \\pm 0.014\\)<\/span><script type='math\/tex'>F_0 = 0.693 \\pm 0.014<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(F_L = 0.315 \\pm 0.011\\)<\/span><script type='math\/tex'>F_L = 0.315 \\pm 0.011<\/script>.<\/nobr> The fraction <nobr><span class='MathJax_Preview'>\\(F_R\\)<\/span><script type='math\/tex'>F_R<\/script><\/nobr> is calculated from the unitarity constraint to be <nobr><span class='MathJax_Preview'>\\(F_R = -0.008 \\pm 0.007\\)<\/span><script type='math\/tex'>F_R = -0.008 \\pm 0.007<\/script>.<\/nobr> These results are in agreement with the standard model predictions at next-to-next-to-leading order in perturbative quantum chromodynamics and represent an improvement in precision of 25 (29)% for <nobr><span class='MathJax_Preview'>\\(F_0\\)<\/span><script type='math\/tex'>F_0<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\((F_L)\\)<\/span><script type='math\/tex'>(F_L)<\/script><\/nobr> with respect to the most precise single measurement. A limit on anomalous right-handed vector <nobr><span class='MathJax_Preview'>\\((V_R)\\)<\/span><script type='math\/tex'>(V_R)<\/script>,<\/nobr> and left- and right-handed tensor <nobr><span class='MathJax_Preview'>\\((g_L\\)<\/span><script type='math\/tex'>(g_L<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(g_R)\\)<\/span><script type='math\/tex'>g_R)<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(tWb\\)<\/span><script type='math\/tex'>tWb<\/script><\/nobr> couplings is set while fixing all others to their standard model values. The allowed regions are <nobr><span class='MathJax_Preview'>\\([-0.11\\)<\/span><script type='math\/tex'>[-0.11<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(0.16]\\)<\/span><script type='math\/tex'>0.16]<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(V_R\\)<\/span><script type='math\/tex'>V_R<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\([-0.08\\)<\/span><script type='math\/tex'>[-0.08<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(0.05]\\)<\/span><script type='math\/tex'>0.05]<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(g_L\\)<\/span><script type='math\/tex'>g_L<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\([-0.04\\)<\/span><script type='math\/tex'>[-0.04<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(0.02]\\)<\/span><script type='math\/tex'>0.02]<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(g_R\\)<\/span><script type='math\/tex'>g_R<\/script>,<\/nobr> at 95% confidence level. Limits on the corresponding Wilson coefficients are also derived.<br \/>\n<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Study of central exclusive <nobr><span class='MathJax_Preview'>\\(\\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\pi^+ \\pi^-<\/script><\/nobr> production in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 5.02 and 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">European Physical Journal C 80 (2020) 718<br \/>DOI: <a href=\"https:\/\/doi.org\/https:\/\/doi.org\/10.1140\/epjc\/s10052-020-8166-5\" target=\"_blank\">https:\/\/doi.org\/10.1140\/epjc\/s10052-020-8166-5<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3890'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3890\" style=\"display: none;\">Central exclusive and semiexclusive production of <nobr><span class='MathJax_Preview'>\\(\\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\pi^+ \\pi^-<\/script><\/nobr> pairs is measured with the CMS detector in proton-proton collisions at the LHC at center-of-mass energies of 5.02 and 13&nbsp;TeV. The theoretical description of these non-perturbative processes, which have not yet been measured in detail at the LHC, poses a significant challenge to models. The two pions are measured and identified in the CMS silicon tracker based on specific energy loss, whereas the absence of other particles is ensured by calorimeter information. The total and differential cross sections of exclusive and semiexclusive central <nobr><span class='MathJax_Preview'>\\(\\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\pi^+ \\pi^-<\/script><\/nobr> production are measured as functions of invariant mass, transverse momentum, and rapidity of the <nobr><span class='MathJax_Preview'>\\(\\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\pi^+ \\pi^-<\/script><\/nobr> system in the fiducial region defined as transverse momentum <nobr><span class='MathJax_Preview'>\\(p_T(\\pi) > 0.2\\)<\/span><script type='math\/tex'>p_T(\\pi) > 0.2<\/script>&nbsp;GeV<\/nobr> and pseudorapidity <nobr><span class='MathJax_Preview'>\\(|\\eta(\\pi)| < 2.4\\)<\/span><script type='math\/tex'>|\\eta(\\pi)| < 2.4<\/script>.<\/nobr> The production cross sections for the four resonant channels <nobr><span class='MathJax_Preview'>\\(f_0(500)\\)<\/span><script type='math\/tex'>f_0(500)<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\rho^0(770)\\)<\/span><script type='math\/tex'>\\rho^0(770)<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(f_0(980)\\)<\/span><script type='math\/tex'>f_0(980)<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\(f_2(1270)\\)<\/span><script type='math\/tex'>f_2(1270)<\/script><\/nobr> are extracted using a simple model. These results represent the first measurement of this process at the LHC collision energies of 5.02 and 13&nbsp;TeV.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Scintillation properties of <nobr><span class='MathJax_Preview'>\\((Zn_{0.9}Pb_{0.1})(W_{0.9}Mo_{0.1})O_4\\)<\/span><script type='math\/tex'>(Zn_{0.9}Pb_{0.1})(W_{0.9}Mo_{0.1})O_4<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\((Zn_{0.9}Cd_{0.1})(W_{0.9}Mo_{0.1})O_4\\)<\/span><script type='math\/tex'>(Zn_{0.9}Cd_{0.1})(W_{0.9}Mo_{0.1})O_4<\/script><\/nobr> mixed crystals<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>E.N.&nbsp;Galashov, D.V.&nbsp;Matvienko, V.A.&nbsp;Moskovskyh, B.I.&nbsp;Sikach and B.A.&nbsp;Shwartz\t<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of Instrumentation 15 (2020) C07028<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1748-0221\/15\/07\/C07028\" target=\"_blank\">10.1088\/1748-0221\/15\/07\/C07028<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4281'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4281\" style=\"display: none;\">Scintillation properties of <nobr><span class='MathJax_Preview'>\\((Zn_{0.9}Pb_{0.1})(W_{0.9}Mo_{0.1})O_4\\)<\/span><script type='math\/tex'>(Zn_{0.9}Pb_{0.1})(W_{0.9}Mo_{0.1})O_4<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\((Zn_{0.9}Cd_{0.1})(W_{0.9}Mo_{0.1})O_4\\)<\/span><script type='math\/tex'>(Zn_{0.9}Cd_{0.1})(W_{0.9}Mo_{0.1})O_4<\/script><\/nobr> mixed crystals with doping of <nobr><span class='MathJax_Preview'>\\(Eu\\)<\/span><script type='math\/tex'>Eu<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(Sm\\)<\/span><script type='math\/tex'>Sm<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(Pr\\)<\/span><script type='math\/tex'>Pr<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(Ce\\)<\/span><script type='math\/tex'>Ce<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(Sc\\)<\/span><script type='math\/tex'>Sc<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(Yt\\)<\/span><script type='math\/tex'>Yt<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(Nb\\)<\/span><script type='math\/tex'>Nb<\/script><\/nobr> are studied. Measurements of theirlight yields relative to pure <nobr><span class='MathJax_Preview'>\\(ZnWO_4\\)<\/span><script type='math\/tex'>ZnWO_4<\/script><\/nobr> at room temperature, decay times and energy resolutions at 662&nbsp;keV are presented. Emission spectra are obtained with <nobr><span class='MathJax_Preview'>\\(^{239}Pu\\)<\/span><script type='math\/tex'>^{239}Pu<\/script><\/nobr> source of alpha particles.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for charged Higgs bosons decaying into a top and a bottom quark in the all-jet final state of <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2007 (2020) 126<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP07(2020)126\" target=\"_blank\">10.1007\/JHEP07(2020)126<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3767'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3767\" style=\"display: none;\">A search for charged Higgs bosons <nobr><span class='MathJax_Preview'>\\((H^\\pm)\\)<\/span><script type='math\/tex'>(H^\\pm)<\/script><\/nobr> decaying into a top and a bottom quark in the all-jet final state is presented. The analysis uses LHC proton-proton collision data recorded with the CMS detector in 2016 at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> No significant excess is observed above the expected background. Model-independent upper limits at 95% confidence level are set on the product of the <nobr><span class='MathJax_Preview'>\\(H^\\pm\\)<\/span><script type='math\/tex'>H^\\pm<\/script><\/nobr> production cross section and branching fraction in two scenarios. For production in association with a top quark, limits of 21.3 to 0.007&nbsp;pb are obtained for <nobr><span class='MathJax_Preview'>\\(H^\\pm\\)<\/span><script type='math\/tex'>H^\\pm<\/script><\/nobr> masses in the range of 0.2 to 3&nbsp;TeV. Combining this with a search in leptonic final states results in improved limits of 9.25 to 0.005&nbsp;pb. The complementary <nobr><span class='MathJax_Preview'>\\(s\\)<\/span><script type='math\/tex'>s<\/script>-channel<\/nobr> production of an <nobr><span class='MathJax_Preview'>\\(H^\\pm\\)<\/span><script type='math\/tex'>H^\\pm<\/script><\/nobr> is investigated in the mass range of 0.8 to 3&nbsp;TeV and the corresponding upper limits are 4.5 to 0.023&nbsp;pb. These results are interpreted using different minimal supersymmetric extensions of the standard model.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the cross section for <nobr><span class='MathJax_Preview'>\\(t \\overline{t}\\)<\/span><script type='math\/tex'>t \\overline{t}<\/script><\/nobr> production with additional jets and <nobr><span class='MathJax_Preview'>\\(b\\)<\/span><script type='math\/tex'>b<\/script><\/nobr> jets in <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2007 (2020) 125<\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2980'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2980\" style=\"display: none;\">Measurements of the cross section for the production of top quark pairs in association with a pair of jets from bottom quarks <nobr><span class='MathJax_Preview'>\\((\\sigma_{t \\overline{t} b \\overline{b}})\\)<\/span><script type='math\/tex'>(\\sigma_{t \\overline{t} b \\overline{b}})<\/script><\/nobr> and in association with a pair of jets from quarks of any flavor or gluons <nobr><span class='MathJax_Preview'>\\((\\sigma_{t \\overline{t} j j})\\)<\/span><script type='math\/tex'>(\\sigma_{t \\overline{t} j j})<\/script><\/nobr> and their ratio are presented. The data were collected in proton-proton collisions at a center-of-mass energy of 13&nbsp;TeV by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The measurements are performed in a fiducial phase space and extrapolated to the full phase space, separately for the dilepton and lepton+jets channels, where lepton corresponds to either an electron or a muon. The results of the measurements in the fiducial phase space for the dilepton and lepton+jets channels, respectively, are <nobr><span class='MathJax_Preview'>\\(\\sigma_{t \\overline{t} j j} = 2.36 \\pm 0.02\\)<\/span><script type='math\/tex'>\\sigma_{t \\overline{t} j j} = 2.36 \\pm 0.02<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 0.20\\)<\/span><script type='math\/tex'>\\pm\\ 0.20<\/script>&nbsp;(syst)&nbsp;pb<\/nobr> and <nobr><span class='MathJax_Preview'>\\(31.0 \\pm 0.2\\)<\/span><script type='math\/tex'>31.0 \\pm 0.2<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 2.9\\)<\/span><script type='math\/tex'>\\pm\\ 2.9<\/script>&nbsp;(syst)&nbsp;pb,<\/nobr> and for the cross section ratio <nobr><span class='MathJax_Preview'>\\(0.017 \\pm 0.001\\)<\/span><script type='math\/tex'>0.017 \\pm 0.001<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 0.001\\)<\/span><script type='math\/tex'>\\pm\\ 0.001<\/script>&nbsp;(syst)<\/nobr> and <nobr><span class='MathJax_Preview'>\\(0.020 \\pm 0.001\\)<\/span><script type='math\/tex'>0.020 \\pm 0.001<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 0.001\\)<\/span><script type='math\/tex'>\\pm\\ 0.001<\/script>&nbsp;(syst).<\/nobr> The values of <nobr><span class='MathJax_Preview'>\\(\\sigma_{t \\overline{t} b \\overline{b}}\\)<\/span><script type='math\/tex'>\\sigma_{t \\overline{t} b \\overline{b}}<\/script><\/nobr> are determined from the product of the <nobr><span class='MathJax_Preview'>\\(\\sigma_{t \\overline{t} j j}\\)<\/span><script type='math\/tex'>\\sigma_{t \\overline{t} j j}<\/script><\/nobr> and the cross section ratio, obtaining, respectively, <nobr><span class='MathJax_Preview'>\\(0.040 \\pm 0.002\\)<\/span><script type='math\/tex'>0.040 \\pm 0.002<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 0.005\\)<\/span><script type='math\/tex'>\\pm\\ 0.005<\/script>&nbsp;(syst)&nbsp;pb<\/nobr> and <nobr><span class='MathJax_Preview'>\\(0.62 \\pm 0.03\\)<\/span><script type='math\/tex'>0.62 \\pm 0.03<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 0.07\\)<\/span><script type='math\/tex'>\\pm\\ 0.07<\/script>&nbsp;(syst)&nbsp;pb.<\/nobr> These measurements are the most precise to date and are consistent, within the uncertainties, with the standard model expectations obtained using a matrix element calculation at next-to-leading order in quantum chromodynamics matched to a parton shower.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">The production of isolated photons in <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s_{NN}}\\)<\/span><script type='math\/tex'>\\sqrt{s_{NN}}<\/script> =<\/nobr> 5.02&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2007 (2020) 116<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP07(2020)116\" target=\"_blank\">10.1007\/JHEP07(2020)116<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4069'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4069\" style=\"display: none;\">The transverse energy <nobr><span class='MathJax_Preview'>\\((E_T^\\gamma)\\)<\/span><script type='math\/tex'>(E_T^\\gamma)<\/script><\/nobr> spectra of photons isolated from other particles are measured using proton-proton <nobr><span class='MathJax_Preview'>\\((p p)\\)<\/span><script type='math\/tex'>(p p)<\/script><\/nobr> and lead-lead <nobr><span class='MathJax_Preview'>\\((Pb Pb)\\)<\/span><script type='math\/tex'>(Pb Pb)<\/script><\/nobr> collisions at the LHC at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s_{NN}}\\)<\/span><script type='math\/tex'>\\sqrt{s_{NN}}<\/script> =<\/nobr> 5.02&nbsp;TeV with integrated luminosities of <nobr>27.4&nbsp;pb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> and <nobr>404&nbsp;<span class='MathJax_Preview'>\\(\\mu\\)<\/span><script type='math\/tex'>\\mu<\/script>b<\/nobr><nobr><span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> data, respectively. The results are presented for photons with <nobr><span class='MathJax_Preview'>\\(25 < E_T^\\gamma < 200\\)<\/span><script type='math\/tex'>25 < E_T^\\gamma < 200<\/script>&nbsp;GeV<\/nobr> in the pseudorapidity range <nobr><span class='MathJax_Preview'>\\(|\\eta| < 1.44\\)<\/span><script type='math\/tex'>|\\eta| < 1.44<\/script>,<\/nobr> and for different centrality intervals for <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> collisions. Photon production in <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> collisions is consistent with that in <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions scaled by the number of binary nucleon-nucleon collisions, demonstrating that photons do not interact with the quark-gluon plasma. Therefore, isolated photons can provide information about the initial energy of the associated parton in photon+jet measurements. The results are compared with predictions from the next-to-leading-order <span style=\"font-variant: small-caps;\">jetphox<\/span> generator for differentparton distribution functions (PDFs) and nuclear PDFs (nPDFs). The comparisons can help to constrain the nPDFs global fits.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of quark- and gluon-like jet fractions using jet charge in <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions at 5.02&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2007 (2020) 115<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP07(2020)115\" target=\"_blank\">10.1007\/JHEP07(2020)115<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4072'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4072\" style=\"display: none;\">The momentum-weighted sum of the electric charges of particles inside a jet, known as jet charge, is sensitive to the electric charge of the particle initiating the parton shower. This paper presents jet charge distributions in <nobr><span class='MathJax_Preview'>\\(\\sqrt{s_{NN}}\\)<\/span><script type='math\/tex'>\\sqrt{s_{NN}}<\/script> =<\/nobr> 5.02&nbsp;TeV lead-lead <nobr><span class='MathJax_Preview'>\\((Pb Pb)\\)<\/span><script type='math\/tex'>(Pb Pb)<\/script><\/nobr> and proton-proton <nobr><span class='MathJax_Preview'>\\((p p)\\)<\/span><script type='math\/tex'>(p p)<\/script><\/nobr> collisions recorded with the CMS detector at the LHC. These data correspond to integrated luminosities of <nobr>404&nbsp;<span class='MathJax_Preview'>\\(\\mu\\)<\/span><script type='math\/tex'>\\mu<\/script>b<\/nobr><nobr><span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> and <nobr>27.4&nbsp;pb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions, respectively. Leveraging the sensitivity of the jet charge to fundamental differences in the electric charges of quarks and gluons, the jet charge distributions from simulated events are used as templates to extract the quark- and gluon-like jet fractions from data. The modification of these jet fractions is examined by comparing <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(Pb Pb\\)<\/span><script type='math\/tex'>Pb Pb<\/script><\/nobr> data as a function of the overlap of the colliding <nobr><span class='MathJax_Preview'>\\(Pb\\)<\/span><script type='math\/tex'>Pb<\/script><\/nobr> nuclei (centrality). This measurement tests the color charge dependence of jet energy loss due to interactions with the quark-gluon plasma. No significant modification between different centrality classes and with respect to <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> results is observed in the extracted quark- and gluon-like jet fractions.<br \/>\n<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Addendum: Measurement of <nobr><span class='MathJax_Preview'>\\(\\Gamma_{ee}(J\/\\psi)\\)<\/span><script type='math\/tex'>\\Gamma_{ee}(J\/\\psi)<\/script><\/nobr> with KEDR detector<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>KEDR Collaboration  <\/i><\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4259'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4259\" style=\"display: none;\">Addendum to Journal of High Energy Physics 1805 (2018) 119.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for disappearing tracks in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 806 (2020) 135502<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2020.135502\" target=\"_blank\">10.1016\/j.physletb.2020.135502<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4110'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4110\" style=\"display: none;\">A search is presented for long-lived charged particles that decay within the volume of the silicon tracker of the CMS experiment. Such particles can produce events with an isolated track that is missing hits in the outermost layers of the silicon tracker, and is also associated with little energy deposited in the calorimeters and no hits in the muon detectors. The search for events with this &ldquo;disappearing track&rdquo; signature is performed in a sample of proton-proton collisions recorded by the CMS experiment at the LHC with a center-of-mass energy of 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>101&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> recorded in 2017 and 2018. The observation of 48 events is consistent with the estimated background of <nobr><span class='MathJax_Preview'>\\(47.8\\ ^{+2.7}_{-2.3}\\)<\/span><script type='math\/tex'>47.8\\ ^{+2.7}_{-2.3}<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 8.1\\)<\/span><script type='math\/tex'>\\pm\\ 8.1<\/script>&nbsp;(syst)<\/nobr> events. Upper limits are set on chargino production in the context of an anomaly-mediated supersymmetry breaking model for purely wino and higgsino neutralino scenarios. At 95% confidence level, the first constraint is placed on chargino masses in the higgsino case, excluding below 750 (175)&nbsp;GeV for a lifetime of 3 (0.05)&nbsp;ns. In the wino case, the results of this search are combined with a previous CMS search to produce a result representing the complete LHC data set recorded in 2015&ndash;2018, the most stringent constraints to date. At 95% confidence level, chargino masses in the wino case are excluded below 884 (474)&nbsp;GeV for a lifetime of 3 (0.2)&nbsp;ns.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">CALICE highly granular calorimeters: imaging properties for hadronic shower analysis<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Chadeeva on behalf of the CMS collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of Instrumentation 15 (2020) C07014<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1748-0221\/15\/07\/C07014\" target=\"_blank\">10.1088\/1748-0221\/15\/07\/C07014<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4213'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4213\" style=\"display: none;\">The CALICE collaboration pioneered the new trend in calorimetry &mdash; highly granular devices for high energy and particle physics applications. During the last fifteen years, several highly granular electromagnetic and hadron calorimeters based on different technologies were constructed and successfully tested. The technologies comprise optical readout, signal collection with semiconducting devices and gaseous detectors. All current CALICE prototypes address technological aspects such as embedded electronics. Dedicated tools are developed for the analysis of test beam data collected with the standalone and combined setups of both physics and technological prototypes of highly granular calorimeters. The tools are described, which help to improve the precision of hadronic shower analysis including the implementation of a calorimeter-based particle identification.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for <nobr><span class='MathJax_Preview'>\\(B^0\\)<\/span><script type='math\/tex'>B^0<\/script><\/nobr> decays to invisible final states <nobr><span class='MathJax_Preview'>\\((+ \\gamma)\\)<\/span><script type='math\/tex'>(+ \\gamma)<\/script><\/nobr> at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Belle Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 102 (2020) 012003<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.102.012003\" target=\"_blank\">10.1103\/PhysRevD.102.012003<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4107'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4107\" style=\"display: none;\">We report searches for <nobr><span class='MathJax_Preview'>\\(B^0 \\to\\ \\)<\/span><script type='math\/tex'>B^0 \\to\\ <\/script>invisible<\/nobr> and <nobr><span class='MathJax_Preview'>\\(B^0 \\to\\ \\)<\/span><script type='math\/tex'>B^0 \\to\\ <\/script>invisible<\/nobr><nobr><span class='MathJax_Preview'>\\({} + \\gamma\\)<\/span><script type='math\/tex'>{} + \\gamma<\/script><\/nobr> decays, where the energy of the photon is required to be larger than 0.5&nbsp;GeV. These results are obtained from a <nobr>711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> data sample that contains <nobr><span class='MathJax_Preview'>\\(772 \\times 10^6\\)<\/span><script type='math\/tex'>772 \\times 10^6<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(B \\overline{B}\\)<\/span><script type='math\/tex'>B \\overline{B}<\/script><\/nobr> pairs and was collected near the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script><\/nobr> resonance with the Belle detector at the KEKB <nobr><span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script><\/nobr> collider. We observe no significant signal for either decay and set upper limits on their branching fractions at 90% confidence level of <nobr><span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to\\ \\)<\/span><script type='math\/tex'>{\\cal B}(B^0 \\to\\ <\/script>invisible<\/nobr><nobr><span class='MathJax_Preview'>\\() < 7.8 \\times 10^{-5}\\)<\/span><script type='math\/tex'>) < 7.8 \\times 10^{-5}<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to\\ \\)<\/span><script type='math\/tex'>{\\cal B}(B^0 \\to\\ <\/script>invisible<\/nobr><nobr><span class='MathJax_Preview'>\\({} + \\gamma) < 1.6 \\times 10^{-5}\\)<\/span><script type='math\/tex'>{} + \\gamma) < 1.6 \\times 10^{-5}<\/script>.<\/nobr><\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Dalitz analysis of <nobr><span class='MathJax_Preview'>\\(D^0 \\to K^- \\pi^+ \\eta\\)<\/span><script type='math\/tex'>D^0 \\to K^- \\pi^+ \\eta<\/script><\/nobr> decays at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Y.Q.&nbsp;Chen, L.K.&nbsp;Li, W.B.&nbsp;Yan, ... , K.&nbsp;Chilikin et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 102 (2020) 012002<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.102.012002\" target=\"_blank\">10.1103\/PhysRevD.102.012002<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4022'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4022\" style=\"display: none;\">We present the results of the first Dalitz plot analysis of the decay <nobr><span class='MathJax_Preview'>\\(D^0 \\to K^- \\pi^+ \\eta\\)<\/span><script type='math\/tex'>D^0 \\to K^- \\pi^+ \\eta<\/script>.<\/nobr> The analysis is performed on a data set corresponding to an integrated luminosity of <nobr>953&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> collected by the Belle detector at the asymmetric-energy <nobr><span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script><\/nobr> KEKB collider. The Dalitz plot is well described by a combination of the six resonant decay channels <nobr><span class='MathJax_Preview'>\\(\\overline{K}{}^*(892)^0 \\eta\\)<\/span><script type='math\/tex'>\\overline{K}{}^*(892)^0 \\eta<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(K^- a_0(980)^+\\)<\/span><script type='math\/tex'>K^- a_0(980)^+<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(K^- a_2(1320)^+\\)<\/span><script type='math\/tex'>K^- a_2(1320)^+<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\overline{K}{}^*(1410)^0 \\eta\\)<\/span><script type='math\/tex'>\\overline{K}{}^*(1410)^0 \\eta<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(K^*(1680)^- \\pi^+\\)<\/span><script type='math\/tex'>K^*(1680)^- \\pi^+<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(K_2^*(1980)^- \\pi^+\\)<\/span><script type='math\/tex'>K_2^*(1980)^- \\pi^+<\/script>,<\/nobr> together with <nobr><span class='MathJax_Preview'>\\(K \\pi\\)<\/span><script type='math\/tex'>K \\pi<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(K \\eta\\)<\/span><script type='math\/tex'>K \\eta<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(S\\)<\/span><script type='math\/tex'>S<\/script>-wave<\/nobr> components. The decays <nobr><span class='MathJax_Preview'>\\(K^*(1680)^- \\to K^- \\eta\\)<\/span><script type='math\/tex'>K^*(1680)^- \\to K^- \\eta<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(K_2^*(1980)^- \\to K^- \\eta\\)<\/span><script type='math\/tex'>K_2^*(1980)^- \\to K^- \\eta<\/script><\/nobr> are observed for the first time. We measure ratio of the branching fractions, <nobr><span class='MathJax_Preview'>\\(\\frac{{\\cal B}(D^0 \\to K^- \\pi^+ \\eta)}{{\\cal B}(D^0 \\to K^- \\pi^+)} = 0.500 \\pm 0.002\\ (\\)<\/span><script type='math\/tex'>\\frac{{\\cal B}(D^0 \\to K^- \\pi^+ \\eta)}{{\\cal B}(D^0 \\to K^- \\pi^+)} = 0.500 \\pm 0.002\\ (<\/script>stat<\/nobr><nobr><span class='MathJax_Preview'>\\()\\)<\/span><script type='math\/tex'>)<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(\\pm\\ 0.020\\ (\\)<\/span><script type='math\/tex'>\\pm\\ 0.020\\ (<\/script>syst<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ \\pm 0.003\\ ({\\cal B}_{PDG})\\)<\/span><script type='math\/tex'>)\\ \\pm 0.003\\ ({\\cal B}_{PDG})<\/script>.<\/nobr> Using the Dalitz fit result, the ratio <nobr><span class='MathJax_Preview'>\\(\\frac{{\\cal B}(K^*(1680) \\to K \\eta)}{{\\cal B}(K^*(1680) \\to K \\pi)}\\)<\/span><script type='math\/tex'>\\frac{{\\cal B}(K^*(1680) \\to K \\eta)}{{\\cal B}(K^*(1680) \\to K \\pi)}<\/script><\/nobr> is measured to be <nobr><span class='MathJax_Preview'>\\(0.11 \\pm 0.02\\ (\\)<\/span><script type='math\/tex'>0.11 \\pm 0.02\\ (<\/script>stat<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ ^{+0.06}_{-0.04}\\ (\\)<\/span><script type='math\/tex'>)\\ ^{+0.06}_{-0.04}\\ (<\/script>syst<\/nobr><nobr><span class='MathJax_Preview'>\\()\\ \\pm 0.04\\ ({\\cal B}_{PDG})\\)<\/span><script type='math\/tex'>)\\ \\pm 0.04\\ ({\\cal B}_{PDG})<\/script>;<\/nobr> this is much lower than the theoretical expectations <nobr><span class='MathJax_Preview'>\\((\\approx 1)\\)<\/span><script type='math\/tex'>(\\approx 1)<\/script><\/nobr> made under the assumption that <nobr><span class='MathJax_Preview'>\\(K^*(1680)\\)<\/span><script type='math\/tex'>K^*(1680)<\/script><\/nobr> is a pure <nobr><span class='MathJax_Preview'>\\(1^3D_1\\)<\/span><script type='math\/tex'>1^3D_1<\/script><\/nobr> state. The product branching fraction <nobr><span class='MathJax_Preview'>\\({\\cal B} \\left( D^0 \\to [K_2^*(1980)^- \\to K^- \\eta] \\pi^+ \\right) =\\)<\/span><script type='math\/tex'>{\\cal B} \\left( D^0 \\to [K_2^*(1980)^- \\to K^- \\eta] \\pi^+ \\right) =<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(\\left( 2.2\\ ^{+1.7}_{-1.9} \\right) \\times 10^{-4}\\)<\/span><script type='math\/tex'>\\left( 2.2\\ ^{+1.7}_{-1.9} \\right) \\times 10^{-4}<\/script><\/nobr> is determined. In addition, the <nobr><span class='MathJax_Preview'>\\(\\pi \\eta^\\prime\\)<\/span><script type='math\/tex'>\\pi \\eta^\\prime<\/script><\/nobr> contribution to the <nobr><span class='MathJax_Preview'>\\(a_0(980)^\\pm\\)<\/span><script type='math\/tex'>a_0(980)^\\pm<\/script><\/nobr> resonance shape is confirmed with <nobr><span class='MathJax_Preview'>\\(10.1\\sigma\\)<\/span><script type='math\/tex'>10.1\\sigma<\/script><\/nobr> statistical significance using the three-channel Flatt\u00e9 model. We also measure <nobr><span class='MathJax_Preview'>\\({\\cal B}(D^0 \\to \\overline{K}{}^*(892)^0 \\eta) = \\left( 1.41\\ ^{+0.13}_{-0.12} \\right)\\%\\)<\/span><script type='math\/tex'>{\\cal B}(D^0 \\to \\overline{K}{}^*(892)^0 \\eta) = \\left( 1.41\\ ^{+0.13}_{-0.12} \\right)\\%<\/script>.<\/nobr> This is consistent with, and more precise than, the current world average <nobr><span class='MathJax_Preview'>\\((1.02 \\pm 0.30)\\%\\)<\/span><script type='math\/tex'>(1.02 \\pm 0.30)\\%<\/script>,<\/nobr> deviates with a significance of more than <nobr><span class='MathJax_Preview'>\\(3\\sigma\\)<\/span><script type='math\/tex'>3\\sigma<\/script><\/nobr> from the theoretical predictions of <nobr><span class='MathJax_Preview'>\\((0.51{-}0.92)\\%\\)<\/span><script type='math\/tex'>(0.51{-}0.92)\\%<\/script>.<\/nobr><\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the top quark forward-backward production asymmetry and the anomalous chromoelectric and chromomagnetic moments in <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2006 (2020) 146<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP06(2020)146\" target=\"_blank\">10.1007\/JHEP06(2020)146<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3683'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3683\" style=\"display: none;\">The parton-level top quark <nobr><span class='MathJax_Preview'>\\((t)\\)<\/span><script type='math\/tex'>(t)<\/script><\/nobr> forward-backward asymmetry and the anomalous chromoelectric <nobr><span class='MathJax_Preview'>\\((\\hat{d}_t)\\)<\/span><script type='math\/tex'>(\\hat{d}_t)<\/script><\/nobr> and chromomagnetic <nobr><span class='MathJax_Preview'>\\((\\hat{\\mu}_t)\\)<\/span><script type='math\/tex'>(\\hat{\\mu}_t)<\/script><\/nobr> moments have been measured using LHC <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions at a center-of-mass energy of 13&nbsp;TeV, collected in the CMS detector in a data sample corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The linearized variable <nobr><span class='MathJax_Preview'>\\(A_{FB}^{(1)}\\)<\/span><script type='math\/tex'>A_{FB}^{(1)}<\/script><\/nobr> is used to approximate the asymmetry. Candidate <nobr><span class='MathJax_Preview'>\\(t \\overline{t}\\)<\/span><script type='math\/tex'>t \\overline{t}<\/script><\/nobr> events decaying to a muon or electron and jets in final states with low and high Lorentz boosts are selected and reconstructed using a fit of the kinematic distributions of the decay products to those expected for <nobr><span class='MathJax_Preview'>\\(t \\overline{t}\\)<\/span><script type='math\/tex'>t \\overline{t}<\/script><\/nobr> final states. The values found for the parameters are <nobr><span class='MathJax_Preview'>\\(A_{FB}^{(1)} = 0.048\\ ^{+0.095}_{-0.087}\\)<\/span><script type='math\/tex'>A_{FB}^{(1)} = 0.048\\ ^{+0.095}_{-0.087}<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(^{+0.020}_{-0.029}\\)<\/span><script type='math\/tex'>^{+0.020}_{-0.029}<\/script>&nbsp;(syst),<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\hat{\\mu}_t = -0.024\\ ^{+0.013}_{-0.009}\\)<\/span><script type='math\/tex'>\\hat{\\mu}_t = -0.024\\ ^{+0.013}_{-0.009}<\/script>&nbsp;(stat)<\/nobr> <nobr><span class='MathJax_Preview'>\\(^{+0.016}_{-0.011}\\)<\/span><script type='math\/tex'>^{+0.016}_{-0.011}<\/script>&nbsp;(syst),<\/nobr> and a limit is placed on the magnitude of <nobr><span class='MathJax_Preview'>\\(|\\hat{d}_t| < 0.03\\)<\/span><script type='math\/tex'>|\\hat{d}_t| < 0.03<\/script><\/nobr> at 95% confidence level.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">[TRANSLATION] Detector Effects on the Response of a Highly Granular Hadron Calorimeter to Single Hadrons<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>S.&nbsp;Korpachev and M.&nbsp;Chadeeva<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Bulletin of the Lebedev Physics Institute 47 (2020) \u2116&nbsp;4, 110\u2013113<br \/>DOI: <a href=\"https:\/\/doi.org\/10.3103\/S1068335620040028\" target=\"_blank\">10.3103\/S1068335620040028<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4177'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4177\" style=\"display: none;\">In the detectors currently being developed for experiments on the next-generation lepton colliders, highly granular calorimeters are to be used. In particular, the hadron calorimeter is planned to be assembled from scintillation cells with direct readout of light by silicon photomultipliers. According to the results of experimental measurements of the light collection in a cell developed for the CALICE prototype hadron calorimeter, when detecting minimum ionizing particles, an estimate of the detector effects was obtained. The detector effect on the resolution of the ILD hadron calorimeter was studied by modeling the response of the detector to single neutral kaons. It was shown that the contribution of experimentally measured detector effects to the resolution for single particles is on the order of 0.5&ndash;1% in the range of hadron energy of 5&ndash;60&nbsp;GeV.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">\u0412\u043b\u0438\u044f\u043d\u0438\u0435 \u0434\u0435\u0442\u0435\u043a\u0442\u043e\u0440\u043d\u044b\u0445 \u044d\u0444\u0444\u0435\u043a\u0442\u043e\u0432 \u043d\u0430 \u043e\u0442\u043a\u043b\u0438\u043a \u0432\u044b\u0441\u043e\u043a\u043e\u0433\u0440\u0430\u043d\u0443\u043b\u044f\u0440\u043d\u043e\u0433\u043e \u0430\u0434\u0440\u043e\u043d\u043d\u043e\u0433\u043e \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u0430 \u043d\u0430 \u043e\u0434\u0438\u043d\u043e\u0447\u043d\u044b\u0435 \u0430\u0434\u0440\u043e\u043d\u044b<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>\u0421.\u0421.&nbsp;\u041a\u043e\u0440\u043f\u0430\u0447\u0435\u0432, \u041c.\u0412.&nbsp;\u0427\u0430\u0434\u0435\u0435\u0432\u0430<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">\u041a\u0440\u0430\u0442\u043a\u0438\u0435 \u0441\u043e\u043e\u0431\u0449\u0435\u043d\u0438\u044f \u043f\u043e \u0444\u0438\u0437\u0438\u043a\u0435 \u0424\u0418\u0410\u041d 47 (2020), \u2116&nbsp;4, \u0441.&nbsp;17\u201323<\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4186'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4186\" style=\"display: none;\">\u0412 \u0434\u0435\u0442\u0435\u043a\u0442\u043e\u0440\u0430\u0445, \u0440\u0430\u0437\u0440\u0430\u0431\u0430\u0442\u044b\u0432\u0430\u0435\u043c\u044b\u0445 \u0434\u043b\u044f \u044d\u043a\u0441\u043f\u0435\u0440\u0438\u043c\u0435\u043d\u0442\u043e\u0432 \u043d\u0430 \u043b\u0435\u043f\u0442\u043e\u043d\u043d\u044b\u0445 \u043a\u043e\u043b\u043b\u0430\u0439\u0434\u0435\u0440\u0430\u0445 \u0441\u043b\u0435\u0434\u0443\u044e\u0449\u0435\u0433\u043e \u043f\u043e\u043a\u043e\u043b\u0435\u043d\u0438\u044f, \u043f\u0440\u0435\u0434\u043f\u043e\u043b\u0430\u0433\u0430\u0435\u0442\u0441\u044f \u0438\u0441\u043f\u043e\u043b\u044c\u0437\u043e\u0432\u0430\u0442\u044c \u0432\u044b\u0441\u043e\u043a\u043e\u0433\u0440\u0430\u043d\u0443\u043b\u044f\u0440\u043d\u044b\u0435 \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u044b. \u0412 \u0447\u0430\u0441\u0442\u043d\u043e\u0441\u0442\u0438, \u0430\u0434\u0440\u043e\u043d\u043d\u044b\u0439 \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440 \u043f\u043b\u0430\u043d\u0438\u0440\u0443\u0435\u0442\u0441\u044f \u0441\u043e\u0431\u0440\u0430\u0442\u044c \u0438\u0437 \u0441\u0446\u0438\u043d\u0442\u0438\u043b\u043b\u044f\u0446\u0438\u043e\u043d\u043d\u044b\u0445 \u044f\u0447\u0435\u0435\u043a \u0441 \u043f\u0440\u044f\u043c\u044b\u043c \u0441\u0447\u0438\u0442\u044b\u0432\u0430\u043d\u0438\u0435\u043c \u0441\u0432\u0435\u0442\u0430 \u043a\u0440\u0435\u043c\u043d\u0438\u0435\u0432\u044b\u043c\u0438 \u0444\u043e\u0442\u043e\u0443\u043c\u043d\u043e\u0436\u0438\u0442\u0435\u043b\u044f\u043c\u0438. \u041f\u043e \u0440\u0435\u0437\u0443\u043b\u044c\u0442\u0430\u0442\u0430\u043c \u044d\u043a\u0441\u043f\u0435\u0440\u0438\u043c\u0435\u043d\u0442\u0430\u043b\u044c\u043d\u043e\u0433\u043e \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u044f \u0441\u0432\u0435\u0442\u043e\u0441\u0431\u043e\u0440\u0430 \u0432 \u044f\u0447\u0435\u0439\u043a\u0435, \u0440\u0430\u0437\u0440\u0430\u0431\u043e\u0442\u0430\u043d\u043d\u043e\u0439 \u0434\u043b\u044f \u043f\u0440\u043e\u0442\u043e\u0442\u0438\u043f\u0430 \u0430\u0434\u0440\u043e\u043d\u043d\u043e\u0433\u043e \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u0430 CALICE, \u043f\u0440\u0438 \u0440\u0435\u0433\u0438\u0441\u0442\u0440\u0430\u0446\u0438\u0438 \u043c\u0438\u043d\u0438\u043c\u0430\u043b\u044c\u043d\u043e \u0438\u043e\u043d\u0438\u0437\u0438\u0440\u0443\u044e\u0449\u0438\u0445 \u0447\u0430\u0441\u0442\u0438\u0446 \u0431\u044b\u043b\u0430 \u043f\u043e\u043b\u0443\u0447\u0435\u043d\u0430 \u043e\u0446\u0435\u043d\u043a\u0430 \u0434\u0435\u0442\u0435\u043a\u0442\u043e\u0440\u043d\u044b\u0445 \u044d\u0444\u0444\u0435\u043a\u0442\u043e\u0432. \u0412\u043b\u0438\u044f\u043d\u0438\u0435 \u044d\u0442\u0438\u0445 \u044d\u0444\u0444\u0435\u043a\u0442\u043e\u0432 \u043d\u0430 \u0440\u0430\u0437\u0440\u0435\u0448\u0435\u043d\u0438\u0435 \u0430\u0434\u0440\u043e\u043d\u043d\u043e\u0433\u043e \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u0430 ILD \u0431\u044b\u043b\u043e \u0438\u0441\u0441\u043b\u0435\u0434\u043e\u0432\u0430\u043d\u043e \u043f\u0443\u0442\u0435\u043c \u043c\u043e\u0434\u0435\u043b\u0438\u0440\u043e\u0432\u0430\u043d\u0438\u044f \u043e\u0442\u043a\u043b\u0438\u043a\u0430 \u0434\u0435\u0442\u0435\u043a\u0442\u043e\u0440\u0430 \u043d\u0430 \u043e\u0434\u0438\u043d\u043e\u0447\u043d\u044b\u0435 \u043d\u0435\u0439\u0442\u0440\u0430\u043b\u044c\u043d\u044b\u0435 \u043a\u0430\u043e\u043d\u044b. \u041f\u043e\u043a\u0430\u0437\u0430\u043d\u043e, \u0447\u0442\u043e \u0432\u043a\u043b\u0430\u0434 \u044d\u043a\u0441\u043f\u0435\u0440\u0438\u043c\u0435\u043d\u0442\u0430\u043b\u044c\u043d\u043e \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u043d\u044b\u0445 \u0434\u0435\u0442\u0435\u043a\u0442\u043e\u0440\u043d\u044b\u0445 \u044d\u0444\u0444\u0435\u043a\u0442\u043e\u0432 \u0432 \u0440\u0430\u0437\u0440\u0435\u0448\u0435\u043d\u0438\u0435 \u0434\u043b\u044f \u043e\u0434\u0438\u043d\u043e\u0447\u043d\u044b\u0445 \u0447\u0430\u0441\u0442\u0438\u0446 \u0441\u043e\u0441\u0442\u0430\u0432\u043b\u044f\u0435\u0442 \u043f\u043e\u0440\u044f\u0434\u043a\u0430 0.5&ndash;1% \u0432 \u0434\u0438\u0430\u043f\u0430\u0437\u043e\u043d\u0435 \u044d\u043d\u0435\u0440\u0433\u0438\u0439 \u0430\u0434\u0440\u043e\u043d\u043e\u0432 5&ndash;60&nbsp;\u0413\u044d\u0412.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the cross section for electroweak production of a <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson, a photon and two jets in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV and constraints on anomalous quartic couplings<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2006 (2020) 076<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP06(2020)076\" target=\"_blank\">10.1007\/JHEP06(2020)076<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3859'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3859\" style=\"display: none;\">A measurement is presented of the cross section for electroweak production of a <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson and a photon in association with two jets <nobr><span class='MathJax_Preview'>\\((Z \\gamma j j)\\)<\/span><script type='math\/tex'>(Z \\gamma j j)<\/script><\/nobr> in proton-proton collisions. The <nobr><span class='MathJax_Preview'>\\(Z\\)<\/span><script type='math\/tex'>Z<\/script><\/nobr> boson candidates are selected through their decay into a pair of electrons or muons. The process of interest, electroweak <nobr><span class='MathJax_Preview'>\\(Z \\gamma j j\\)<\/span><script type='math\/tex'>Z \\gamma j j<\/script><\/nobr> production, is isolated by selecting events with a large dijet mass and a large pseudorapidity gap between the two jets. The measurement is based on data collected at the CMS experiment at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script><\/nobr> = 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The observed significance of the signal is 3.9 standard deviations, where a significance of 5.2 standard deviations is expected in the standard model. These results are combined with published results by CMS at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 8&nbsp;TeV, which leads to observed and expected respective significances of 4.7 and 5.5 standard deviations. From the 13&nbsp;TeV data, a value is obtained for the signal strength of electroweak <nobr><span class='MathJax_Preview'>\\(Z \\gamma j j\\)<\/span><script type='math\/tex'>Z \\gamma j j<\/script><\/nobr> production and bounds are given on quartic vector boson interactions in the framework of dimension-eight effective field theory operators.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">A measurement of the Higgs boson mass in the diphoton decay channel<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 805 (2020) 135425<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2020.135425\" target=\"_blank\">10.1016\/j.physletb.2020.135425<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3836'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3836\" style=\"display: none;\">A measurement of the mass of the Higgs boson in the diphoton decay channel is presented. This analysis is based on <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> of proton-proton collision data collected during the 2016 LHC running period, with the CMS detector at a centre-of-mass energy of 13&nbsp;TeV. A refined detector calibration and new analysis techniques have been used to improve the precision of this measurement. The Higgs boson mass is measured to be <nobr><span class='MathJax_Preview'>\\(m_H = 125.78 \\pm 0.26\\)<\/span><script type='math\/tex'>m_H = 125.78 \\pm 0.26<\/script>&nbsp;GeV.<\/nobr> This is combined with a measurement of <nobr><span class='MathJax_Preview'>\\(m_H\\)<\/span><script type='math\/tex'>m_H<\/script><\/nobr> already performed in the <nobr><span class='MathJax_Preview'>\\(H \\to Z Z \\to 4{\\cal l}\\)<\/span><script type='math\/tex'>H \\to Z Z \\to 4{\\cal l}<\/script><\/nobr> decay channel using the same data set, giving <nobr><span class='MathJax_Preview'>\\(m_H = 125.46 \\pm 0.16\\)<\/span><script type='math\/tex'>m_H = 125.46 \\pm 0.16<\/script>&nbsp;GeV.<\/nobr> This result, when further combined with an earlier measurement of <nobr><span class='MathJax_Preview'>\\(m_H\\)<\/span><script type='math\/tex'>m_H<\/script><\/nobr> using data collected in 2011 and 2012 with the CMS detector, gives a value for the Higgs boson mass of <nobr><span class='MathJax_Preview'>\\(m_H = 125.38 \\pm 0.14\\)<\/span><script type='math\/tex'>m_H = 125.38 \\pm 0.14<\/script>&nbsp;GeV.<\/nobr> This is currently the most precise measurement of the mass of the Higgs boson.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurements with silicon photomultipliers of dose-rate effects in the radiation damage of plastic scintillator tiles in the CMS hadron endcap calorimeter<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of Instrumentation 15 (2020) P06009<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1748-0221\/15\/06\/P06009\" target=\"_blank\">10.1088\/1748-0221\/15\/06\/P06009<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3761'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3761\" style=\"display: none;\">Measurements are presented of the reduction of signal output due to radiation damage for two types of plastic scintillator tiles used in the hadron endcap (HE) calorimeter of the CMS detector. The tiles were exposed to particles produced in proton-proton <nobr>(<span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script>)<\/nobr> collisions at the CERN LHC with a center-of-mass energy of 13&nbsp;TeV, corresponding to a delivered luminosity of <nobr>50&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The measurements are based on readout channels of the HE that were instrumented with silicon photomultipliers, and are derived using data from several sources: a laser calibration system, a movable radioactive source, as well as hadrons and muons produced in <nobr><span class='MathJax_Preview'>\\(p p\\)<\/span><script type='math\/tex'>p p<\/script><\/nobr> collisions. Results from several irradiation campaigns using <nobr><span class='MathJax_Preview'>\\(^{60}{\\rm Co}\\)<\/span><script type='math\/tex'>^{60}{\\rm Co}<\/script><\/nobr> sources are also discussed. The damage is presented as a function of dose rate. Within the range of these measurements, for a fixed dose the damage increases with decreasing dose rate.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Identification of heavy, energetic, hadronically decaying particles using machine-learning techniques<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of Instrumentation 15 (2020) P06005<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1748-0221\/15\/06\/P06005\" target=\"_blank\">10.1088\/1748-0221\/15\/06\/P06005<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('4121'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"4121\" style=\"display: none;\">Machine-learning (ML) techniques are explored to identify and classify hadronic decays of highly Lorentz-boosted <nobr><span class='MathJax_Preview'>\\(W \/ Z \/\\)<\/span><script type='math\/tex'>W \/ Z \/<\/script>Higgs<\/nobr> bosons and top quarks. Techniques without ML have also been evaluated and are included for comparison. The identification performances of a variety of algorithms are characterized in simulated events and directly compared with data. The algorithms are validated using proton-proton collision data at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>35.9&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> Systematic uncertainties are assessed by comparing the results obtained using simulation and collision data. The new techniques studied in this paper provide significant performance improvements over non-ML techniques, reducing the background rate by up to an order of magnitude at the same signal efficiency.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Update of inclusive cross sections of single and pairs of identified light charged hadrons<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Belle Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 101 (2020) 092004<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.101.092004\" target=\"_blank\">10.1103\/PhysRevD.101.092004<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3772'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3772\" style=\"display: none;\">We report new measurements of the production cross sections of pairs of charged pions and kaons as a function of their fractional energies using various fractional-energy definitions. Two different fractional-energy definitions were used and compared to the conventional fractional-energy definition reported previously. The new variables aim at either identifying dihadron cross sections in terms of single-hadron fragmentation functions, or to provide a means of characterizing the transverse momentum created in the fragmentation process. The results were obtained applying the updated initial-state radiation correction used in other recent Belle publications on light-hadron production cross sections. In addition, production cross sections of single charged pions, kaons, and protons were also updated using this initial-state radiation correction. The cross sections are obtained from a <nobr>558&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> data sample collected at the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script><\/nobr> resonance with the Belle detector at the KEKB asymmetric-energy <nobr><span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script><\/nobr> collider.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for an excited lepton that decays via a contact interaction to a lepton and two jets in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2005 (2020) 052<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP05(2020)052\" target=\"_blank\">10.1007\/JHEP05(2020)052<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3730'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3730\" style=\"display: none;\">Results are presented from a search for events containing an excited lepton (electron or muon) produced in association with an ordinary lepton of the same flavor and decaying to a lepton and two hadronic jets. Both the production and the decay of the excited leptons are assumed to occur via a contact interaction with a characteristic energy scale <nobr><span class='MathJax_Preview'>\\(\\Lambda\\)<\/span><script type='math\/tex'>\\Lambda<\/script>.<\/nobr> The branching fraction for the decay mode under study increases with the mass of the excited lepton and is the most sensitive channel for very heavy excited leptons. The analysis uses a sample of proton-proton collisions collected by the CMS experiment at the LHC at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV, corresponding to an integrated luminosity of <nobr>77.4&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The four-body invariant mass of the two lepton plus two jet system is used as the primary discriminating variable. No significant excess of events beyond the expectation for standard model processes is observed. Assuming that <nobr><span class='MathJax_Preview'>\\(\\Lambda\\)<\/span><script type='math\/tex'>\\Lambda<\/script><\/nobr> is equal to the mass of the excited leptons, excited electrons and muons with masses below 5.6 and 5.7&nbsp;TeV, respectively, are excluded at 95% confidence level. These are the best limits to date.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for direct top squark pair production in events with one lepton, jets, and missing transverse momentum at 13&nbsp;TeV with the CMS experiment<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2005 (2020) 032<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP05(2020)032\" target=\"_blank\">10.1007\/JHEP05(2020)032<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3674'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3674\" style=\"display: none;\">A search for direct top squark pair production is presented. The search is based on proton-proton collision data at a center-of-mass energy of 13&nbsp;TeV recorded by the CMS experiment at the LHC during 2016, 2017, and 2018, corresponding to an integrated luminosity of <nobr>137&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The search is carried out using events with a single isolated electron or muon, multiple jets, and large transverse momentum imbalance. The observed data are consistent with the expectations from standard model processes. Exclusions are set in the context of simplified top squark pair production models. Depending on the model, exclusion limits at 95% confidence level for top squark masses up to 1.2&nbsp;TeV are set for a massless lightest supersymmetric particle, assumed to be the neutralino. For models with top squark masses of 1&nbsp;TeV, neutralino masses up to 600&nbsp;GeV are excluded.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Quark masses: N3LO bridge from <nobr><span class='MathJax_Preview'>\\(RI\/SMOM\\)<\/span><script type='math\/tex'>RI\/SMOM<\/script><\/nobr> to <nobr><span class='MathJax_Preview'>\\(\\overline{MS}\\)<\/span><script type='math\/tex'>\\overline{MS}<\/script><\/nobr> scheme<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.&nbsp;Bednyakov and A.&nbsp;Pikelner<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 101 (2020) 091501(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.101.091501\" target=\"_blank\">10.1103\/PhysRevD.101.091501<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3862'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3862\" style=\"display: none;\">We analytically compute the three-loop corrections to the relation between the renormalized quark masses defined in the minimal-subtraction <nobr><span class='MathJax_Preview'>\\((\\overline{MS})\\)<\/span><script type='math\/tex'>(\\overline{MS})<\/script><\/nobr> and the regularization-invariant symmetric momentum-subtraction <nobr><span class='MathJax_Preview'>\\((RI\/SMOM)\\)<\/span><script type='math\/tex'>(RI\/SMOM)<\/script><\/nobr> schemes. Our result is valid in the Landau gauge and can be used to reduce the uncertainty in a lattice determination of the <nobr><span class='MathJax_Preview'>\\(\\overline{MS}\\)<\/span><script type='math\/tex'>\\overline{MS}<\/script><\/nobr> quark masses.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of <nobr><span class='MathJax_Preview'>\\({\\cal R}(D)\\)<\/span><script type='math\/tex'>{\\cal R}(D)<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\({\\cal R}(D^*)\\)<\/span><script type='math\/tex'>{\\cal R}(D^*)<\/script><\/nobr> with a Semileptonic Tagging Method<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>G.&nbsp;Caria, P.&nbsp;Urquijo, ... , S.&nbsp;Eidelman et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 124 (2020) 161803<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.124.161803\" target=\"_blank\">10.1103\/PhysRevLett.124.161803<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3230'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3230\" style=\"display: none;\">The experimental results on the ratios of branching fractions <nobr><span class='MathJax_Preview'>\\({\\cal R}(D) =\\)<\/span><script type='math\/tex'>{\\cal R}(D) =<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\({\\cal B}(\\overline{B} \\to D \\tau^- \\overline{\\nu}_\\tau) \/ {\\cal B}(\\overline{B} \\to D {\\cal l}^- \\overline{\\nu}_{\\cal l})\\)<\/span><script type='math\/tex'>{\\cal B}(\\overline{B} \\to D \\tau^- \\overline{\\nu}_\\tau) \/ {\\cal B}(\\overline{B} \\to D {\\cal l}^- \\overline{\\nu}_{\\cal l})<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\({\\cal R}(D^*) = {\\cal B}(\\overline{B} \\to D^* \\tau^- \\overline{\\nu}_\\tau) \/ {\\cal B}(\\overline{B} \\to D^* {\\cal l}^- \\overline{\\nu}_{\\cal l})\\)<\/span><script type='math\/tex'>{\\cal R}(D^*) = {\\cal B}(\\overline{B} \\to D^* \\tau^- \\overline{\\nu}_\\tau) \/ {\\cal B}(\\overline{B} \\to D^* {\\cal l}^- \\overline{\\nu}_{\\cal l})<\/script>,<\/nobr> where <nobr><span class='MathJax_Preview'>\\({\\cal l}\\)<\/span><script type='math\/tex'>{\\cal l}<\/script><\/nobr> denotes an electron or a muon, show a long-standing discrepancy with the standard model predictions, and might hint at a violation of lepton flavor universality. We report a new simultaneous measurement of <nobr><span class='MathJax_Preview'>\\({\\cal R}(D)\\)<\/span><script type='math\/tex'>{\\cal R}(D)<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\({\\cal R}(D^*)\\)<\/span><script type='math\/tex'>{\\cal R}(D^*)<\/script>,<\/nobr> based on a data sample containing <nobr><span class='MathJax_Preview'>\\(772 \\times 10^6\\)<\/span><script type='math\/tex'>772 \\times 10^6<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(B \\overline{B}\\)<\/span><script type='math\/tex'>B \\overline{B}<\/script><\/nobr> events recorded at the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script><\/nobr> resonance with the Belle detector at the KEKB <nobr><span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script><\/nobr> collider. In this analysis the tag-side <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script><\/nobr> meson is reconstructed in a semileptonic decay mode and the signal-side <nobr><span class='MathJax_Preview'>\\(\\tau\\)<\/span><script type='math\/tex'>\\tau<\/script><\/nobr> is reconstructed in a purely leptonic decay. The measured values are <nobr><span class='MathJax_Preview'>\\({\\cal R}(D) = 0.307 \\pm 0.037 \\pm 0.016\\)<\/span><script type='math\/tex'>{\\cal R}(D) = 0.307 \\pm 0.037 \\pm 0.016<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\({\\cal R}(D^*) = 0.283 \\pm 0.018 \\pm 0.014\\)<\/span><script type='math\/tex'>{\\cal R}(D^*) = 0.283 \\pm 0.018 \\pm 0.014<\/script>,<\/nobr> where the first uncertainties are statistical and the second are systematic. These results are in agreement with the standard model predictions within 0.2, 1.1, and 0.8 standard deviations for <nobr><span class='MathJax_Preview'>\\({\\cal R}(D)\\)<\/span><script type='math\/tex'>{\\cal R}(D)<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\({\\cal R}(D^*)\\)<\/span><script type='math\/tex'>{\\cal R}(D^*)<\/script>,<\/nobr> and their combination, respectively. This work constitutes the most precise measurements of <nobr><span class='MathJax_Preview'>\\({\\cal R}(D)\\)<\/span><script type='math\/tex'>{\\cal R}(D)<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\({\\cal R}(D^*)\\)<\/span><script type='math\/tex'>{\\cal R}(D^*)<\/script><\/nobr> performed to date as well as the first result for <nobr><span class='MathJax_Preview'>\\({\\cal R}(D)\\)<\/span><script type='math\/tex'>{\\cal R}(D)<\/script><\/nobr> based on a semileptonic tagging method.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Study of excited <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0<\/script><\/nobr> states decaying to <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0 \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\Lambda_b^0 \\pi^+ \\pi^-<\/script><\/nobr> in proton-proton collisions at <nobr><span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> =<\/nobr> 13&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.M.&nbsp;Sirunyan, ... , S.&nbsp;Polikarpov et al. (CMS Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 803 (2020) 135345<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2020.135345\" target=\"_blank\">10.1016\/j.physletb.2020.135345<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3762'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3762\" style=\"display: none;\">A study of excited <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0<\/script><\/nobr> baryons is reported, based on a data sample collected in 2016&ndash;2018 with the CMS detector at the LHC in proton-proton collisions at a center-of-mass energy of 13&nbsp;TeV, corresponding to an integrated luminosity of up to <nobr>140&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The existence of four excited <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0<\/script><\/nobr> states: <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0(5912)^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0(5912)^0<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0(5920)^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0(5920)^0<\/script>,<\/nobr> <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0(6146)^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0(6146)^0<\/script>,<\/nobr> and <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0(6152)^0\\)<\/span><script type='math\/tex'>\\Lambda_b^0(6152)^0<\/script><\/nobr> in the <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0 \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\Lambda_b^0 \\pi^+ \\pi^-<\/script><\/nobr> mass spectrum is confirmed, and their masses are measured. The <nobr><span class='MathJax_Preview'>\\(\\Lambda_b^0 \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\Lambda_b^0 \\pi^+ \\pi^-<\/script><\/nobr> mass distribution exhibits a broad excess of events in the region of 6040&ndash;6100&nbsp;MeV, whose origin cannot be discerned with the present data.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Four-loop QCD MOM beta functions from the three-loop vertices at the symmetric point<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.&nbsp;Bednyakov and A.&nbsp;Pikelner<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 101 (2020) 071502(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.101.071502\" target=\"_blank\">10.1103\/PhysRevD.101.071502<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3815'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3815\" style=\"display: none;\">For the first time, we compute three-loop contributions to all triple vertices in QCD at the symmetric point. The analytic results are obtained in massless QCD with an arbitrary color group in the Landau gauge. All new loop integrals are expressed in terms of harmonic polylogarithms at the sixth root of unity. These corrections allow us to derive expressions for the four-loop QCD beta function in a set of momentum-subtraction schemes.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for an Invisibly Decaying <nobr><span class='MathJax_Preview'>\\(Z^\\prime\\)<\/span><script type='math\/tex'>Z^\\prime<\/script><\/nobr> Boson at Belle&nbsp;II in <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\mu^+ \\mu^- (e^\\pm \\mu^\\mp)\\)<\/span><script type='math\/tex'>e^+e^- \\to \\mu^+ \\mu^- (e^\\pm \\mu^\\mp)<\/script><\/nobr> Plus Missing Energy Final States<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Belle&nbsp;II Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 124 (2020) 141801<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.124.141801\" target=\"_blank\">10.1103\/PhysRevLett.124.141801<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3685'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3685\" style=\"display: none;\">Theories beyond the standard model often predict the existence of an additional neutral boson, the <nobr><span class='MathJax_Preview'>\\(Z^\\prime\\)<\/span><script type='math\/tex'>Z^\\prime<\/script>.<\/nobr> Using data collected by the Belle&nbsp;II experiment during 2018 at the SuperKEKB collider, we perform the first searches for the invisible decay of a <nobr><span class='MathJax_Preview'>\\(Z^\\prime\\)<\/span><script type='math\/tex'>Z^\\prime<\/script><\/nobr> in the process <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\mu^+ \\mu^- Z^\\prime\\)<\/span><script type='math\/tex'>e^+e^- \\to \\mu^+ \\mu^- Z^\\prime<\/script><\/nobr> and of a lepton-flavor-violating <nobr><span class='MathJax_Preview'>\\(Z^\\prime\\)<\/span><script type='math\/tex'>Z^\\prime<\/script><\/nobr> in <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to e^\\pm \\mu^\\mp Z^\\prime\\)<\/span><script type='math\/tex'>e^+e^- \\to e^\\pm \\mu^\\mp Z^\\prime<\/script>.<\/nobr> We do not find any excess of events and set 90% credibility level upper limits on the cross sections of these processes. We translate the former, in the framework of an <nobr><span class='MathJax_Preview'>\\(L_\\mu - L_\\tau\\)<\/span><script type='math\/tex'>L_\\mu - L_\\tau<\/script><\/nobr> theory, into upper limits on the <nobr><span class='MathJax_Preview'>\\(Z^\\prime\\)<\/span><script type='math\/tex'>Z^\\prime<\/script><\/nobr> coupling constant at the level of <nobr><span class='MathJax_Preview'>\\(5 \\times 10^{-2} - 1\\)<\/span><script type='math\/tex'>5 \\times 10^{-2} - 1<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(M_{Z^\\prime} \\leq 6\\)<\/span><script type='math\/tex'>M_{Z^\\prime} \\leq 6<\/script>&nbsp;GeV<\/nobr><nobr><span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script>.<\/nobr><\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Future Physics Programme of BESIII<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Ablikim, ... , S.I.&nbsp;Eidelman et al.<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Chinese Physics C 44 (2020) 040001<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1674-1137\/44\/4\/040001\" target=\"_blank\">10.1088\/1674-1137\/44\/4\/040001<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3661'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3661\" style=\"display: none;\">There has recently been a dramatic renewal of interest in hadron spectroscopy and charm physics. This renaissance has been driven in part by the discovery of a plethora of charmonium-like <nobr><span class='MathJax_Preview'>\\(XYZ\\)<\/span><script type='math\/tex'>XYZ<\/script><\/nobr> states at BESIII and <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script><\/nobr> factories, and the observation of an intriguing proton-antiproton threshold enhancement and the possibly related <nobr><span class='MathJax_Preview'>\\(X(1835)\\)<\/span><script type='math\/tex'>X(1835)<\/script><\/nobr> meson state at BESIII, as well as the threshold measurements of charm mesons and charm baryons. We present a detailed survey of the important topics in tau-charm physics and hadron physics that can be further explored at BESIII during the remaining operation period of BEPCII. This survey will help in the optimization of the data-taking plan over the coming years, and provides physics motivation for the possible upgrade of BEPCII to higher luminosity.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Study of <nobr><span class='MathJax_Preview'>\\(B \\to p \\overline{p} \\pi \\pi\\)<\/span><script type='math\/tex'>B \\to p \\overline{p} \\pi \\pi<\/script><\/nobr><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Belle Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 101 (2020) 052012<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.101.052012\" target=\"_blank\">10.1103\/PhysRevD.101.052012<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3660'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3660\" style=\"display: none;\">Using a data sample of <nobr><span class='MathJax_Preview'>\\(772 \\times 10^6\\)<\/span><script type='math\/tex'>772 \\times 10^6<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\(B \\overline{B}\\)<\/span><script type='math\/tex'>B \\overline{B}<\/script><\/nobr> pairs collected on the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script><\/nobr> resonance with the Belle detector at the KEKB asymmetric energy <nobr><span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script><\/nobr> collider, we report the observation of <nobr><span class='MathJax_Preview'>\\(B^0 \\to p \\overline{p} \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>B^0 \\to p \\overline{p} \\pi^+ \\pi^-<\/script><\/nobr> and the first observation of <nobr><span class='MathJax_Preview'>\\(B^+ \\to p \\overline{p} \\pi^+ \\pi^0\\)<\/span><script type='math\/tex'>B^+ \\to p \\overline{p} \\pi^+ \\pi^0<\/script>.<\/nobr> We measure a decay branching fraction of <nobr><span class='MathJax_Preview'>\\((0.83 \\pm 0.17 \\pm 0.7) \\times 10^{-6}\\)<\/span><script type='math\/tex'>(0.83 \\pm 0.17 \\pm 0.7) \\times 10^{-6}<\/script><\/nobr> in <nobr><span class='MathJax_Preview'>\\(B^0 \\to p \\overline{p} \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>B^0 \\to p \\overline{p} \\pi^+ \\pi^-<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(M_{\\pi^+ \\pi^-} < 1.22\\)<\/span><script type='math\/tex'>M_{\\pi^+ \\pi^-} < 1.22<\/script>&nbsp;GeV<\/nobr><nobr><span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script><\/nobr> with a significance of 5.5 standard deviations. The contribution from <nobr><span class='MathJax_Preview'>\\(B^0 \\to p \\overline{p} K^0\\)<\/span><script type='math\/tex'>B^0 \\to p \\overline{p} K^0<\/script><\/nobr> is excluded. We measure a decay branching fraction of <nobr><span class='MathJax_Preview'>\\((4.58 \\pm 1.17 \\pm 0.67) \\times 10^{-6}\\)<\/span><script type='math\/tex'>(4.58 \\pm 1.17 \\pm 0.67) \\times 10^{-6}<\/script><\/nobr> for <nobr><span class='MathJax_Preview'>\\(B^+ \\to p \\overline{p} \\pi^+ \\pi^0\\)<\/span><script type='math\/tex'>B^+ \\to p \\overline{p} \\pi^+ \\pi^0<\/script><\/nobr> with <nobr><span class='MathJax_Preview'>\\(M_{\\pi^+ \\pi^0} < 1.3\\)<\/span><script type='math\/tex'>M_{\\pi^+ \\pi^0} < 1.3<\/script>&nbsp;GeV<\/nobr><nobr><span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script><\/nobr> with a significance of 5.4 standard deviations. We study the difference of the <nobr><span class='MathJax_Preview'>\\(M_{p \\overline{p}}\\)<\/span><script type='math\/tex'>M_{p \\overline{p}}<\/script><\/nobr> distributions in <nobr><span class='MathJax_Preview'>\\(B^0 \\to p \\overline{p} \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>B^0 \\to p \\overline{p} \\pi^+ \\pi^-<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(B^+ \\to p \\overline{p} \\pi^+ \\pi^0\\)<\/span><script type='math\/tex'>B^+ \\to p \\overline{p} \\pi^+ \\pi^0<\/script>.<\/nobr><\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">On the Scalar-Sensitive Angular Observables for <nobr><span class='MathJax_Preview'>\\(B \\to K^* l l\\)<\/span><script type='math\/tex'>B \\to K^* l l<\/script><\/nobr> in the SM<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.V.&nbsp;Bednyakov and A.I.&nbsp;Mukhaeva<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics of Particles and Nuclei Letters 17 (2020) \u2116&nbsp;1, 1\u201312<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1134\/S1547477120010045\" target=\"_blank\">10.1134\/S1547477120010045<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3871'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3871\" style=\"display: none;\">The angular analysis of rare decays <nobr><span class='MathJax_Preview'>\\(B \\to K^* l l\\)<\/span><script type='math\/tex'>B \\to K^* l l<\/script><\/nobr> deserves much attention in literature due to rich structure and great potential to discover New Physics. There are several <nobr><span class='MathJax_Preview'>\\(2-3\\sigma\\)<\/span><script type='math\/tex'>2-3\\sigma<\/script><\/nobr> discrepancies with the SM predictions, which can be accounted for by the introduction of New Physics. In this paper we will not address these issues, but concentrate on the SM predictions. The aim of the present letter is to consider scalar-sensitive observables and review the SM result for the latter. It is a well-known fact that the corresponding contributions are heavily suppressed in the SM and usually neglected. Nevertheless, we present the explicit result for the leading contribution, which can be of interest when comparing with possible NP predictions. In addition, we briefly discuss possible prospects of experimental study of the corresponding observables.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">A study of the corrections to factorization in <nobr><span class='MathJax_Preview'>\\(\\overline{B}{}^0 \\to D^{*+} \\omega \\pi^-\\)<\/span><script type='math\/tex'>\\overline{B}{}^0 \\to D^{*+} \\omega \\pi^-<\/script><\/nobr><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>S.I.&nbsp;Eidelman, L.V.&nbsp;Kardapoltsev and D.V.&nbsp;Matvienko<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2002 (2020) 168<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP02(2020)168\" target=\"_blank\">10.1007\/JHEP02(2020)168<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3867'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3867\" style=\"display: none;\">A factorization hypothesis is tested by examining a form factor of the to <nobr><span class='MathJax_Preview'>\\(\\omega \\pi\\)<\/span><script type='math\/tex'>\\omega \\pi<\/script><\/nobr> production in hadronic <nobr><span class='MathJax_Preview'>\\(B^0 \\to D^{*\\pm} \\omega \\pi^\\mp\\)<\/span><script type='math\/tex'>B^0 \\to D^{*\\pm} \\omega \\pi^\\mp<\/script><\/nobr> decays. The form factor is compared to that from available <nobr><span class='MathJax_Preview'>\\(\\tau\\)<\/span><script type='math\/tex'>\\tau<\/script>-lepton<\/nobr> as well as <nobr><span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script><\/nobr> data using the conserved vector current hypothesis. The difference of normalizations of form factor shapes from <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(\\tau\\)<\/span><script type='math\/tex'>\\tau<\/script><\/nobr> <nobr><span class='MathJax_Preview'>\\((e^+e^-)\\)<\/span><script type='math\/tex'>(e^+e^-)<\/script><\/nobr> data indicates the important role of the large <nobr><span class='MathJax_Preview'>\\(N_c\\)<\/span><script type='math\/tex'>N_c<\/script><\/nobr> limit in QCD. Moreover, the growth of the difference between the form factors with the <nobr><span class='MathJax_Preview'>\\(\\omega \\pi\\)<\/span><script type='math\/tex'>\\omega \\pi<\/script><\/nobr> invariant mass is related to the perturbative QCD corrections of factorization. The current precision of <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script><\/nobr> data does not allow one to find any evidence of corrections to factorization. A promising study could be performed with the Belle&nbsp;II and LHCb data sets.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of <nobr><span class='MathJax_Preview'>\\(D^0\\)<\/span><script type='math\/tex'>D^0<\/script>-<\/nobr><nobr><span class='MathJax_Preview'>\\(\\overline{D}{}^0\\)<\/span><script type='math\/tex'>\\overline{D}{}^0<\/script><\/nobr> mixing parameters using semileptonic decays of neutral kaon<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>P.&nbsp;Pakhlov and V.&nbsp;Popov<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2002 (2020) 160<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP02(2020)160\" target=\"_blank\">10.1007\/JHEP02(2020)160<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3649'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3649\" style=\"display: none;\">We propose a new method to extract <nobr><span class='MathJax_Preview'>\\(D^0\\)<\/span><script type='math\/tex'>D^0<\/script>-<\/nobr><nobr><span class='MathJax_Preview'>\\(\\overline{D}{}^0\\)<\/span><script type='math\/tex'>\\overline{D}{}^0<\/script><\/nobr> mixing parameters using the <nobr><span class='MathJax_Preview'>\\(D^0 \\to \\overline{K}{}^0 \\pi^0\\)<\/span><script type='math\/tex'>D^0 \\to \\overline{K}{}^0 \\pi^0<\/script><\/nobr> decay with the <nobr><span class='MathJax_Preview'>\\(\\overline{K}{}^0\\)<\/span><script type='math\/tex'>\\overline{K}{}^0<\/script><\/nobr> reconstructed in the semileptonic mode. Although a <nobr><span class='MathJax_Preview'>\\(K^0 \\to \\pi^\\pm {\\cal l}^\\mp \\nu_{\\cal l}\\)<\/span><script type='math\/tex'>K^0 \\to \\pi^\\pm {\\cal l}^\\mp \\nu_{\\cal l}<\/script><\/nobr> decay suffers from low statistics and complexity of the secondary vertex reconstruction in comparison to the standard <nobr><span class='MathJax_Preview'>\\(K_S^0 \\to \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>K_S^0 \\to \\pi^+ \\pi^-<\/script><\/nobr> vertex, it provides much richer, sometimes unique information about the initial state of a <nobr><span class='MathJax_Preview'>\\(K^0\\)<\/span><script type='math\/tex'>K^0<\/script>-meson<\/nobr> produced in a heavy-flavor hadron decay. In this paper it is shown that the reconstruction of the chain <nobr><span class='MathJax_Preview'>\\(D^0 \\to K^0 (\\pi^\\pm {\\cal l}^\\mp \\nu_{\\cal l}) \\pi^0\\)<\/span><script type='math\/tex'>D^0 \\to K^0 (\\pi^\\pm {\\cal l}^\\mp \\nu_{\\cal l}) \\pi^0<\/script><\/nobr> allows one to extract the strong phase difference between the doubly Cabibbo-suppressed and Cabibbo-favored decay amplitudes, which is of key importance for determination of the <nobr><span class='MathJax_Preview'>\\(D^0\\)<\/span><script type='math\/tex'>D^0<\/script>-<\/nobr><nobr><span class='MathJax_Preview'>\\(\\overline{D}{}^0\\)<\/span><script type='math\/tex'>\\overline{D}{}^0<\/script>-mixing<\/nobr> parameters.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for <nobr><span class='MathJax_Preview'>\\(B^+ \\to \\mu^+ \\nu_\\mu\\)<\/span><script type='math\/tex'>B^+ \\to \\mu^+ \\nu_\\mu<\/script><\/nobr> and <nobr><span class='MathJax_Preview'>\\(B^+ \\to \\mu^+ N\\)<\/span><script type='math\/tex'>B^+ \\to \\mu^+ N<\/script><\/nobr> with inclusive tagging<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Belle Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 101 (2020) 032007<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.101.032007\" target=\"_blank\">10.1103\/PhysRevD.101.032007<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('3478'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"3478\" style=\"display: none;\">We report the result for a search for the leptonic decay of <nobr><span class='MathJax_Preview'>\\(B^+ \\to \\mu^+ \\nu_\\mu\\)<\/span><script type='math\/tex'>B^+ \\to \\mu^+ \\nu_\\mu<\/script><\/nobr> using the full Belle dataset of <nobr>711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script><\/nobr> of integrated luminosity at the <nobr><span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script><\/nobr> resonance. In the Standard Model leptonic <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script>-meson<\/nobr> decays are helicity and Cabibbo-Kobayashi-Maskawa suppressed. To maximize sensitivity an inclusive tagging approach is used to reconstruct the second <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script><\/nobr> meson produced in the collision. The directional information from this second <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script><\/nobr> meson is used to boost the observed <nobr><span class='MathJax_Preview'>\\(\\mu\\)<\/span><script type='math\/tex'>\\mu<\/script><\/nobr> into the signal <nobr><span class='MathJax_Preview'>\\(B\\)<\/span><script type='math\/tex'>B<\/script>-meson<\/nobr> rest frame, in which the <nobr><span class='MathJax_Preview'>\\(\\mu\\)<\/span><script type='math\/tex'>\\mu<\/script><\/nobr> has a monochromatic momentum spectrum. Though its momentum is smeared by the experimental resolution, this technique improves the analysis sensitivity considerably. Analyzing the <nobr><span class='MathJax_Preview'>\\(\\mu\\)<\/span><script type='math\/tex'>\\mu<\/script><\/nobr> momentum spectrum in this frame we find <nobr><span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to \\mu^+ \\nu_\\mu) = (5.3 \\pm 2.0 \\pm 0.9) \\times 10^{-7}\\)<\/span><script type='math\/tex'>{\\cal B}(B^+ \\to \\mu^+ \\nu_\\mu) = (5.3 \\pm 2.0 \\pm 0.9) \\times 10^{-7}<\/script><\/nobr> with a one-sided significance of 2.8 standard deviations over the background-only hypothesis. This translates to a frequentist upper limit of <nobr><span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to \\mu^+ \\nu_\\mu) < 8.6 \\times 10^{-7}\\)<\/span><script type='math\/tex'>{\\cal B}(B^+ \\to \\mu^+ \\nu_\\mu) < 8.6 \\times 10^{-7}<\/script><\/nobr> at 90% confidence level. The experimental spectrum is then used to search for a massive sterile neutrino, <nobr><span class='MathJax_Preview'>\\(B^+ \\to \\mu^+ N\\)<\/span><script type='math\/tex'>B^+ \\to \\mu^+ N<\/script>,<\/nobr> but no evidence is observed for a sterile neutrino with a mass in a range of 0&mdash;1.5&nbsp;GeV. The determined <nobr><span class='MathJax_Preview'>\\(B^+ \\to \\mu^+ \\nu_\\mu\\)<\/span><script type='math\/tex'>B^+ \\to \\mu^+ \\nu_\\mu<\/script><\/nobr> branching fraction limit is further used to constrain the mass and coupling space of the type II and type III two-Higgs-doublet models.<\/span><\/div>\n<\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\pi^+ \\pi^-<\/script><\/nobr> cross section with the CMD-3 detector at the VEPP-2000 collider<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>CMD-3 Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 2001 (2020) 112<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1007\/JHEP01(2020)112\" target=\"_blank\">10.1007\/JHEP01(2020)112<\/a><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2933'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2933\" style=\"display: none;\">The cross section of the process <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\pi^+ \\pi^-<\/script><\/nobr> is measured using the data collected with the CMD-3 detector at the VEPP-2000 collider in the center-of-mass energy range from 1.1 to 2.0&nbsp;GeV. The decay mode <nobr><span class='MathJax_Preview'>\\(\\eta \\to \\gamma \\gamma\\)<\/span><script type='math\/tex'>\\eta \\to \\gamma \\gamma<\/script><\/nobr> is used for <nobr><span class='MathJax_Preview'>\\(\\eta\\)<\/span><script type='math\/tex'>\\eta<\/script><\/nobr> meson reconstruction in the data sample corresponding to an integrated luminosity of <nobr>78.3&nbsp;pb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>.<\/nobr> The energy dependence of the <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\pi^+ \\pi^-<\/script><\/nobr> cross section is fitted within the framework of vector meson dominance in order to extract the <nobr><span class='MathJax_Preview'>\\(\\Gamma(\\rho(1450) \\to e^+e^-)\\ \\times\\)<\/span><script type='math\/tex'>\\Gamma(\\rho(1450) \\to e^+e^-)\\ \\times<\/script><\/nobr><wbr><nobr><span class='MathJax_Preview'>\\({\\cal B}(\\rho(1450) \\to \\eta \\pi^+ \\pi^-)\\)<\/span><script type='math\/tex'>{\\cal B}(\\rho(1450) \\to \\eta \\pi^+ \\pi^-)<\/script><\/nobr> and the <nobr><span class='MathJax_Preview'>\\(\\Gamma(\\rho(1700) \\to e^+e^-)\\ \\times\\)<\/span><script type='math\/tex'>\\Gamma(\\rho(1700) \\to e^+e^-)\\ \\times<\/script><\/nobr><wbr><nobr><span class='MathJax_Preview'>\\({\\cal B}(\\rho(1700) \\to \\eta \\pi^+\\pi^-)\\)<\/span><script type='math\/tex'>{\\cal B}(\\rho(1700) \\to \\eta \\pi^+\\pi^-)<\/script><\/nobr> products. Based on conservation of vector current, the analyzed data are used to test the relationship between the <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\pi^+ \\pi^-<\/script><\/nobr> cross section and the spectral function in <nobr><span class='MathJax_Preview'>\\(\\tau^- \\to \\eta \\pi^- \\pi^0 \\nu_\\tau\\)<\/span><script type='math\/tex'>\\tau^- \\to \\eta \\pi^- \\pi^0 \\nu_\\tau<\/script><\/nobr> decay. The <nobr><span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\pi^+ \\pi^-<\/script><\/nobr> cross section obtained with the CMD-3 detector is in good agreement with the previous measurements.<\/span><\/div>\n<\/div>\n<\/li>\n<\/ol>\n<\/div>\n<h3 align=\"center\">2019 \u0433\u043e\u0434<\/h3>\n<div class=\"publication-archive\">\n<ol style=\"padding: 0; padding-left: 18pt;\">\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Observation of <span class='MathJax_Preview'>\\(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-\\)<script type='math\/tex'>\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-<\/script> and search for <span class='MathJax_Preview'>\\(\\tau^- \\to \\pi^- \\nu_\\tau \\mu^+ \\mu^-\\)<script type='math\/tex'>\\tau^- \\to \\pi^- \\nu_\\tau \\mu^+ \\mu^-<\/script><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Y.&nbsp;Jin, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 100 (2019) 071101(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.100.071101\" target=\"_blank\">10.1103\/PhysRevD.100.071101<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2982'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2982\" style=\"display: none;\">e present the first measurements of branching fractions of rare tau-lepton decays, <span class='MathJax_Preview'>\\(\\tau^- \\to \\pi^- \\nu_\\tau {\\cal l}^+ {\\cal l}^-\\)<script type='math\/tex'>\\tau^- \\to \\pi^- \\nu_\\tau {\\cal l}^+ {\\cal l}^-<\/script> <span class='MathJax_Preview'>\\(({\\cal l} = e)\\)<script type='math\/tex'>({\\cal l} = e<\/script> or <span class='MathJax_Preview'>\\(\\mu\\)<script type='math\/tex'>\\mu)<\/script>, using a data sample corresponding to 562&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> collected at a center-of-mass energy of 10.58&nbsp;GeV with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. The <span class='MathJax_Preview'>\\(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-\\)<script type='math\/tex'>\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-<\/script> decay is observed for the first time with <span class='MathJax_Preview'>\\(7.0\\sigma\\)<script type='math\/tex'>7.0\\sigma<\/script> significance. The partial branching fraction determined by the structure-dependent mechanisms mediated by either a vector or an axial-vector current for the mass region <span class='MathJax_Preview'>\\(M_{\\pi e e} > 1.05\\)<script type='math\/tex'>M_{\\pi e e} > 1.05<\/script>&nbsp;GeV<span class='MathJax_Preview'>\\(\/c^2\\)<script type='math\/tex'>\/c^2<\/script> is measured to be <span class='MathJax_Preview'>\\({\\cal B}(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-)[M_{\\pi^- e^+ e^-} > 1.05\\)<script type='math\/tex'>{\\cal B}(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-)[M_{\\pi^- e^+ e^-} > 1.05<\/script>&nbsp;GeV<span class='MathJax_Preview'>\\(\/c^2] = (5.90 \\pm 0.53 \\pm 0.85 \\pm 0.11) \\times 10^{-6}\\)<script type='math\/tex'>\/c^2] = (5.90 \\pm 0.53 \\pm 0.85 \\pm 0.11) \\times 10^{-6}<\/script>, where the first uncertainty is statistical, the second is systematic, and the third is due to model dependence. In the full phase space, due to the different detection efficiencies for the structure-dependent mechanisms mediated by axial-vector and vector currents, the branching fraction varies from <span class='MathJax_Preview'>\\({\\cal B}_A(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-) = (1.46 \\pm 0.13 \\pm 0.21) \\times 10^{-5}\\)<script type='math\/tex'>{\\cal B}_A(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-) = (1.46 \\pm 0.13 \\pm 0.21) \\times 10^{-5}<\/script> to <span class='MathJax_Preview'>\\({\\cal B}_V(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-) = (3.01 \\pm 0.27 \\pm 0.43) \\times 10^{-5}\\)<script type='math\/tex'>{\\cal B}_V(\\tau^- \\to \\pi^- \\nu_\\tau e^+ e^-) = (3.01 \\pm 0.27 \\pm 0.43) \\times 10^{-5}<\/script>, respectively. An upper limit is set on the branching fraction of the <span class='MathJax_Preview'>\\(\\tau^- \\to \\pi^- \\nu_\\tau \\mu^+ \\mu^-\\)<script type='math\/tex'>\\tau^- \\to \\pi^- \\nu_\\tau \\mu^+ \\mu^-<\/script> decay, <span class='MathJax_Preview'>\\({\\cal B}(\\tau^- \\to \\pi^- \\nu_\\tau \\mu^+ \\mu^-) < 1.14 \\times 10^{-5}\\)<script type='math\/tex'>{\\cal B}(\\tau^- \\to \\pi^- \\nu_\\tau \\mu^+ \\mu^-) < 1.14 \\times 10^{-5}<\/script>, at the 90% confidence level.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of the CKM matrix element <span class='MathJax_Preview'>\\(|V_{cb}|\\)<script type='math\/tex'>|V_{cb}|<\/script> from <span class='MathJax_Preview'>\\(B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}\\)<script type='math\/tex'>B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}<\/script> at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i> E.&nbsp;Waheed, P.&nbsp;Urquijo, D.&nbsp;Ferlewicz ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 100 (2019) 052007<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.100.052007\" target=\"_blank\">10.1103\/PhysRevD.100.052007<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2529'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2529\" style=\"display: none;\">We present a new measurement of the Cabibbo-Kobayashi-Maskawa matrix element <span class='MathJax_Preview'><\\(|V_{cb}|\\)<script type='math\/tex'>|V_{cb}|<\/script> from <span class='MathJax_Preview'>\\(B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}\\)<\/span><script type='math\/tex'>B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}<\/script> decays, reconstructed with the full Belle data set of 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> integrated luminosity. Two form factor parametrizations, originally conceived by the Caprini-Lellouch-Neubert (CLN) and the Boyd, Grinstein and Lebed (BGL) groups, are used to extract the product <span class='MathJax_Preview'>\\({\\cal F}(1) \\eta_{EW} |V_{cb}|\\)<\/span><script type='math\/tex'>{\\cal F}(1) \\eta_{EW} |V_{cb}|<\/script> and the decay form factors, where <span class='MathJax_Preview'>\\({\\cal F}(1)\\)<script type='math\/tex'>{\\cal F}(1)<\/script> is the normalization factor and <span class='MathJax_Preview'>\\(\\eta_{EW}\\)<script type='math\/tex'>\\eta_{EW}<\/script> is a small electroweak correction. In the CLN parametrization we find <span class='MathJax_Preview'>\\({\\cal F}(1) \\eta_{EW} |V_{cb}| = (35.06 \\pm 0.15 \\pm 0.56) \\times 10^{-3}\\)<script type='math\/tex'>{\\cal F}(1) \\eta_{EW} |V_{cb}| = (35.06 \\pm 0.15 \\pm 0.56) \\times 10^{-3}<\/script>, <span class='MathJax_Preview'>\\(\\rho^2 = 1.106 \\pm 0.031 \\pm 0.007\\)<script type='math\/tex'>\\rho^2 = 1.106 \\pm 0.031 \\pm 0.007<\/script>, <span class='MathJax_Preview'>\\(R_1(1) = 1.229 \\pm 0.028 \\pm 0.009\\)<script type='math\/tex'>R_1(1) = 1.229 \\pm 0.028 \\pm 0.009<\/script>, <span class='MathJax_Preview'>\\(R_2(1) = 0.852 \\pm 0.021 \\pm 0.006\\)<script type='math\/tex'>R_2(1) = 0.852 \\pm 0.021 \\pm 0.006<\/script>. For the BGL parametrization we obtain <span class='MathJax_Preview'>\\({\\cal F}(1) \\eta_{EW} |V_{cb}| = (34.93 \\pm 0.23 \\pm 0.59) \\times 10^{-3}\\)<script type='math\/tex'>{\\cal F}(1) \\eta_{EW} |V_{cb}| = (34.93 \\pm 0.23 \\pm 0.59) \\times 10^{-3}<\/script>, which is consistent with the world average when correcting for <span class='MathJax_Preview'>\\({\\cal F}(1) \\eta_{EW}\\)<script type='math\/tex'>{\\cal F}(1) \\eta_{EW}<\/script>. The branching fraction of <span class='MathJax_Preview'>\\(B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}\\)<script type='math\/tex'>B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}<\/script> is measured to be <span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}) = (4.90 \\pm 0.02 \\pm 0.16)\\%\\)<script type='math\/tex'>{\\cal B}(B^0 \\to D^{*-} {\\cal l}^+ \\nu_{\\cal l}) = (4.90 \\pm 0.02 \\pm 0.16)\\%<\/script>. We also present a new test of lepton flavor universality violation in semileptonic <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> decays, <span class='MathJax_Preview'>\\(\\frac{{\\cal B}(B^0 \\to D^{*-} e^+ \\nu)}{{\\cal B}(B^0 \\to D^{*-} \\mu^+ \\nu)} = 1.01 \\pm 0.01 \\pm 0.03\\)<script type='math\/tex'>\\frac{{\\cal B}(B^0 \\to D^{*-} e^+ \\nu)}{{\\cal B}(B^0 \\to D^{*-} \\mu^+ \\nu)} = 1.01 \\pm 0.01 \\pm 0.03<\/script>. The errors quoted correspond to the statistical and systematic uncertainties, respectively. This is the most precise measurement of <span class='MathJax_Preview'>\\({\\cal F}(1) \\eta_{EW} |V_{cb}|\\)<script type='math\/tex'>{\\cal F}(1) \\eta_{EW} |V_{cb}|<\/script> and form factors to date and the first experimental study of the BGL form factor parametrization in an experimental measurement.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for <span class='MathJax_Preview'>\\(\\Omega(2012) \\to K \\Xi(1530) \\to K \\pi \\Xi\\)<script type='math\/tex'>\\Omega(2012) \\to K \\Xi(1530) \\to K \\pi \\Xi<\/script> at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>S.&nbsp;Jia, C.&nbsp;P.&nbsp;Shen, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration) <\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 100 (2019) 032006<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.100.032006\" target=\"_blank\">10.1103\/PhysRevD.100.032006<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2573'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2573\" style=\"display: none;\">Using data samples of <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collisions collected at the <span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<script type='math\/tex'>\\Upsilon(1S)<\/script>, <span class='MathJax_Preview'>\\(\\Upsilon(2S)\\)<script type='math\/tex'>\\Upsilon(2S)<\/script>, and <span class='MathJax_Preview'>\\(\\Upsilon(3S)\\)<script type='math\/tex'>\\Upsilon(3S)<\/script> resonances with the Belle detector, we search for the three-body decay of the <span class='MathJax_Preview'>\\(\\Omega(2012)\\)<script type='math\/tex'>\\Omega(2012)<\/script> baryon to <span class='MathJax_Preview'>\\(K \\pi \\Xi\\)<script type='math\/tex'>K \\pi \\Xi<\/script>. This decay is predicted to dominate for models describing the <span class='MathJax_Preview'>\\(\\Omega(2012)\\)<script type='math\/tex'>\\Omega(2012)<\/script> as a <span class='MathJax_Preview'>\\(K \\Xi(1530)\\)<script type='math\/tex'>K \\Xi(1530)<\/script> molecule. No significant <span class='MathJax_Preview'>\\(\\Omega(2012)\\)<script type='math\/tex'>\\Omega(2012)<\/script> signals are observed in the studied channels, and 90% credibility level upper limits on the ratios of the branching fractions relative to <span class='MathJax_Preview'>\\(K \\Xi\\)<script type='math\/tex'>K \\Xi<\/script> decay modes are obtained.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">First measurements of absolute branching fractions of the <span class='MathJax_Preview'>\\(\\Xi_c^+\\)<script type='math\/tex'>\\Xi_c^+<\/script> baryon at Belle<\/div>\n<p><!--\t\t\n\n<div class=\"publication_authors\"><span class=\"author-list\" style=\"font-style: italic;\">LPI, MEPhI, MIPT<\/span><span class=\"date\">(August 12, 2019)<\/span><\/div>\n\n --><\/p>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Y.&nbsp;B.&nbsp;Li, C.&nbsp;P.&nbsp;Shen, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 100 (2019) 031101(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.100.031101\" target=\"_blank\">10.1103\/PhysRevD.100.031101<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2065'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2065\" style=\"display: none;\">We present the first measurements of absolute branching fractions of <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> decays into <span class='MathJax_Preview'>\\(\\Xi^- \\pi^+\\)<script type='math\/tex'>\\Xi^- \\pi^+<\/script>, <span class='MathJax_Preview'>\\(\\Lambda K^- \\pi^+\\)<script type='math\/tex'>\\Lambda K^- \\pi^+<\/script>, and <span class='MathJax_Preview'>\\(p K^- K^- \\pi^+\\)<script type='math\/tex'>p K^- K^- \\pi^+<\/script> final states. The measurements are made using a dataset comprising <span class='MathJax_Preview'>\\((772 \\pm 11) \\times 10^6\\)<script type='math\/tex'>(772 \\pm 11) \\times 10^6<\/script> <span class='MathJax_Preview'>\\(B \\overline{B}\\)<script type='math\/tex'>B \\overline{B}<\/script> pairs collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. We first measure the absolute branching fraction for <span class='MathJax_Preview'>\\(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0\\)<script type='math\/tex'>B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0<\/script> using a missing-mass technique; the result is <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0) = (9.51 \\pm 2.10 \\pm 0.88) \\times 10^{-4}\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0) = (9.51 \\pm 2.10 \\pm 0.88) \\times 10^{-4}<\/script>. We subsequently measure the product branching fractions <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)<\/script>, <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+)<\/script>, and <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+)<\/script> with improved precision. Dividing these product branching fractions by the result for <span class='MathJax_Preview'>\\(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0\\)<script type='math\/tex'>B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0<\/script> yields the following branching fractions: <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+) = (1.80 \\pm 0.50 \\pm 0.14)\\%\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+) = (1.80 \\pm 0.50 \\pm 0.14)\\%<\/script>, <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+) = (1.17 \\pm 0.37 \\pm 0.09)\\%\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+) = (1.17 \\pm 0.37 \\pm 0.09)\\%<\/script>, and <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+) = (0.58 \\pm 0.23 \\pm 0.05)\\%\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+) = (0.58 \\pm 0.23 \\pm 0.05)\\%<\/script>. For the above branching fractions, the first uncertainties are statistical and the second are systematic. Our result for <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)<\/script> can be combined with <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> branching fractions measured relative to <span class='MathJax_Preview'>\\(\\Xi_c^0 \\to \\Xi^- \\pi^+\\)<script type='math\/tex'>\\Xi_c^0 \\to \\Xi^- \\pi^+<\/script> to yield other absolute <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> branching fractions.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurement of branching fraction and final-state asymmetry for the <span class='MathJax_Preview'>\\(\\overline{B}{}^0 \\to K_S^0 K^\\mp \\pi^\\pm\\)<script type='math\/tex'>\\overline{B}{}^0 \\to K_S^0 K^\\mp \\pi^\\pm<\/script> decay<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Y.-T.&nbsp;Lai, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 100 (2019) 011101(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.100.011101\" target=\"_blank\">10.1103\/PhysRevD.100.011101<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2518'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2518\" style=\"display: none;\">We report a measurement of the branching fraction and final-state asymmetry for the <span class='MathJax_Preview'>\\(\\overline{B}{}^0 \\to K_S^0 K^\\mp \\pi^\\pm\\)<script type='math\/tex'>\\overline{B}{}^0 \\to K_S^0 K^\\mp \\pi^\\pm<\/script> decays. The analysis is based on a data sample of 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. We obtain a branching fraction of <span class='MathJax_Preview'>\\((3.60 \\pm 0.33 \\pm 0.15) \\times 10^{-6}\\)<script type='math\/tex'>(3.60 \\pm 0.33 \\pm 0.15) \\times 10^{-6}<\/script> and a final-state asymmetry of <span class='MathJax_Preview'>\\((-8.5 \\pm 8.9 \\pm 0.2)\\%\\)<script type='math\/tex'>(-8.5 \\pm 8.9 \\pm 0.2)\\%<\/script>, where the first uncertainties are statistical and the second are systematic. Hints of peaking structures are found in the differential branching fractions measured as functions of Dalitz variables.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for the process <span class='MathJax_Preview'>\\(e^+e^- \\to D^*(2007)\\)<script type='math\/tex'>e^+e^- \\to D^*(2007)<\/script> with the CMD-3 detector<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>D.N.&nbsp;Shemyakin, ...&nbsp;, S.I.&nbsp;Eidelman et al.<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">EPJ Web of Conferences 212 (2019) 02011<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1051\/epjconf\/201921202011\" target=\"_blank\">10.1051\/epjconf\/201921202011<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2711'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2711\" style=\"display: none;\">A search for the process <span class='MathJax_Preview'>\\(e^+e^- \\to D^{*0}(2007)\\)<script type='math\/tex'>e^+e^- \\to D^{*0}(2007)<\/script> has been performed with the CMD-3 detector at the VEPP-2000 <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script>-collider. Two main decay modes of the <span class='MathJax_Preview'>\\(D^{*0}(2007)\\)<script type='math\/tex'>D^{*0}(2007)<\/script> decay, <span class='MathJax_Preview'>\\(D^0 \\pi^0\\)<script type='math\/tex'>D^0 \\pi^0<\/script> and <span class='MathJax_Preview'>\\(D^0 \\gamma\\)<script type='math\/tex'>D^0 \\gamma<\/script>, followed by <span class='MathJax_Preview'>\\(D^0 \\to K^+ \\pi^- \\pi^+ \\pi^-\\)<script type='math\/tex'>D^0 \\to K^+ \\pi^- \\pi^+ \\pi^-<\/script> are used in this analysis. With an integrated luminosity of 3.7&nbsp;pb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> collected at the center-of-mass energy <span class='MathJax_Preview'>\\(E_{\\rm c.m.} =\\)<script type='math\/tex'>E_{\\rm c.m.} =<\/script> <span class='MathJax_Preview'>\\(2006.62\\)<script type='math\/tex'>2006.62<\/script>&nbsp;MeV our preliminary upper limit is <span class='MathJax_Preview'>\\({\\cal B}_{D^{*0} \\to e^+e^-} < 1.6 \\times 10^{-6}\\)<script type='math\/tex'>{\\cal B}_{D^{*0} \\to e^+e^-} < 1.6 \\times 10^{-6}<\/script> at 90%C.L.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\"><span class='MathJax_Preview'>\\(X(3872)\\)<script type='math\/tex'>X(3872)<\/script> \u0432 \u043c\u043e\u043b\u0435\u043a\u0443\u043b\u044f\u0440\u043d\u043e\u0439 \u043c\u043e\u0434\u0435\u043b\u0438<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>\u042e.\u0421.&nbsp;\u041a\u0430\u043b\u0430\u0448\u043d\u0438\u043a\u043e\u0432\u0430, \u0410.\u0412.&nbsp;\u041d\u0435\u0444\u0435\u0434\u044c\u0435\u0432<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">\u0423\u0441\u043f\u0435\u0445\u0438 \u0444\u0438\u0437\u0438\u0447\u0435\u0441\u043a\u0438\u0445 \u043d\u0430\u0443\u043a 189 (2019), \u2116&nbsp;6, \u0441.&nbsp;603\u2013634<br \/>DOI: <a href=\"https:\/\/doi.org\/10.3367\/UFNr.2018.08.038411\" target=\"_blank\">10.3367\/UFNr.2018.08.038411<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1903'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1903\" style=\"display: none;\">\u041e\u0431\u0441\u0443\u0436\u0434\u0430\u044e\u0442\u0441\u044f \u043c\u0435\u0442\u043e\u0434\u044b \u0438 \u043f\u043e\u0434\u0445\u043e\u0434\u044b \u043a \u043e\u043f\u0438\u0441\u0430\u043d\u0438\u044e \u043c\u043e\u043b\u0435\u043a\u0443\u043b\u044f\u0440\u043d\u044b\u0445 \u0441\u043e\u0441\u0442\u043e\u044f\u043d\u0438\u0439 \u0432 \u0441\u043f\u0435\u043a\u0442\u0440\u0435 \u0442\u044f\u0436\u0451\u043b\u044b\u0445 \u043a\u0432\u0430\u0440\u043a\u043e\u0432, \u0430 \u0442\u0430\u043a\u0436\u0435 \u043f\u043e\u0434\u0440\u043e\u0431\u043d\u043e \u0438\u0437\u0443\u0447\u0430\u044e\u0442\u0441\u044f \u0441\u0432\u043e\u0439\u0441\u0442\u0432\u0430 \u044d\u043a\u0437\u043e\u0442\u0438\u0447\u0435\u0441\u043a\u043e\u0433\u043e \u0441\u043e\u0441\u0442\u043e\u044f\u043d\u0438\u044f \u0447\u0430\u0440\u043c\u043e\u043d\u0438\u044f <span class='MathJax_Preview'>\\(X(3872)\\)<script type='math\/tex'>X(3872)<\/script> \u0432 \u0440\u0430\u043c\u043a\u0430\u0445 \u043c\u043e\u0434\u0435\u043b\u0438 \u043c\u0435\u0437\u043e\u043d\u043d\u043e\u0439 \u043c\u043e\u043b\u0435\u043a\u0443\u043b\u044b. <\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Transverse momentum dependent production cross sections of charged pions, kaons and protons produced in inclusive <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> annihilation at <span class='MathJax_Preview'>\\(\\sqrt{s}\\)<script type='math\/tex'>\\sqrt{s}<\/script> = 10.58&nbsp;GeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Belle Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 112006<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.112006\" target=\"_blank\">10.1103\/PhysRevD.99.112006<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2311'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2311\" style=\"display: none;\">We report measurements of the production cross sections of charged pions, kaons, and protons as a function of fractional energy, the event-shape variable called thrust, and the transverse momentum with respect to the thrust axis. These measurements access the transverse momenta created in the fragmentation process, which are of critical importance to the understanding of any transverse-momentum-dependent distribution and fragmentation functions. The low transverse-momentum part of the cross sections can be well described by Gaussians in transverse momentum as is generally assumed but the fractional-energy dependence is nontrivial and different hadron types have varying Gaussian widths. The width of these Gaussians decreases with thrust and shows an initially rising, then decreasing fractional-energy dependence. The widths for pions and kaons are comparable within uncertainties, while those for protons are significantly narrower. These single-hadron cross sections and Gaussian widths are obtained from a 558&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> data sample collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for <span class='MathJax_Preview'>\\(X(3872)\\)<script type='math\/tex'>X(3872)<\/script> and <span class='MathJax_Preview'>\\(X(3915)\\)<script type='math\/tex'>X(3915)<\/script> decay into <span class='MathJax_Preview'>\\(\\chi_{c1} \\pi^0\\)<script type='math\/tex'>\\chi_{c1} \\pi^0<\/script> in <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> decays at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>V.&nbsp;Bhardwaj, S.&nbsp;Jia, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 111101(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.111101\" target=\"_blank\">10.1103\/PhysRevD.99.111101<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2517'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2517\" style=\"display: none;\">We report a search for <span class='MathJax_Preview'>\\(X(3872)\\)<script type='math\/tex'>X(3872)<\/script> and <span class='MathJax_Preview'>\\(X(3915)\\)<script type='math\/tex'>X(3915)<\/script> in <span class='MathJax_Preview'>\\(B^+ \\to \\chi_{c1} \\pi^0 K^+\\)<script type='math\/tex'>B^+ \\to \\chi_{c1} \\pi^0 K^+<\/script> decays. We set an upper limit of <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to X(3872) K^+) \\times {\\cal B}(X(3872) \\to \\chi_{c1} \\pi^0) < 8.1 \\times 10^{-6}\\)<script type='math\/tex'>{\\cal B}(B^+ \\to X(3872) K^+) \\times {\\cal B}(X(3872) \\to \\chi_{c1} \\pi^0) < 8.1 \\times 10^{-6}<\/script> and <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to X(3915) K^+) \\times\\)<script type='math\/tex'>{\\cal B}(B^+ \\to X(3915) K^+) \\times<\/script> <span class='MathJax_Preview'>\\({\\cal B}(X(3915) \\to \\chi_{c1} \\pi^0) < 3.8 \\times 10^{-5}\\)<script type='math\/tex'>{\\cal B}(X(3915) \\to \\chi_{c1} \\pi^0) < 3.8 \\times 10^{-5}<\/script> at 90% confidence level. We also measure <span class='MathJax_Preview'>\\({\\cal B}(X(3872) \\to \\chi_{c1} \\pi^0) \/ {\\cal B}(X(3872) \\to J\/\\psi \\pi^+ \\pi^-) < 0.97\\)<script type='math\/tex'>{\\cal B}(X(3872) \\to \\chi_{c1} \\pi^0) \/ {\\cal B}(X(3872) \\to J\/\\psi \\pi^+ \\pi^-) < 0.97<\/script> at 90% confidence level. The results reported here are obtained from <span class='MathJax_Preview'>\\(772 \\times 10^6\\)<script type='math\/tex'>772 \\times 10^6<\/script> <span class='MathJax_Preview'>\\(B \\overline{B}\\)<script type='math\/tex'>B \\overline{B}<\/script> events collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">A new approach for measuring the muon anomalous magnetic moment and electric dipole moment<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Abe, ...&nbsp;, S.&nbsp;Eidelman et al.<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Progress of Theoretical and Experimental Physics 2019 (2019) 053C02<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1093\/ptep\/ptz030\" target=\"_blank\">10.1093\/ptep\/ptz030<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2224'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2224\" style=\"display: none;\">This paper introduces a new approach to measure the muon magnetic moment anomaly <span class='MathJax_Preview'>\\(a_\\mu = (g - 2)\/2\\)<script type='math\/tex'>a_\\mu = (g - 2)\/2<\/script> and the muon electric dipole moment (EDM) <span class='MathJax_Preview'>\\(d_\\mu\\)<script type='math\/tex'>d_\\mu<\/script> at the J-PARC muon facility. The goal of our experiment is to measure <span class='MathJax_Preview'>\\(a_\\mu\\)<script type='math\/tex'>a_\\mu<\/script> and <span class='MathJax_Preview'>\\(d_\\mu\\)<script type='math\/tex'>d_\\mu<\/script> using an independent method with a factor of 10 lower muon momentum, and a factor of 20 smaller diameter storage-ring solenoid compared with previous and ongoing muon <span class='MathJax_Preview'>\\(g - 2\\)<script type='math\/tex'>g - 2<\/script> experiments with unprecedented quality of the storage magnetic field. Additional significant differences from the present experimental method include a factor of 1000 smaller transverse emittance of the muon beam (reaccelerated thermal muon beam), its efficient vertical injection into the solenoid, and tracking each decay positron from muon decay to obtain its momentum vector. The precision goal for <span class='MathJax_Preview'>\\(a_\\mu\\)<script type='math\/tex'>a_\\mu<\/script> is a statistical uncertainty of 450 parts per billion (ppb), similar to the present experimental uncertainty, and a systematic uncertainty less than 70&nbsp;ppb. The goal for EDM is a sensitivity of <span class='MathJax_Preview'>\\(1.5 \\times 10^{-21}~e\\cdot\\)<script type='math\/tex'>1.5 \\times 10^{-21}~e\\cdot<\/script>cm.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Evidence for the decay <span class='MathJax_Preview'>\\(B^0 \\to p \\overline{p} \\pi^0\\)<script type='math\/tex'>B^0 \\to p \\overline{p} \\pi^0<\/script><\/div>\n<p><!--\t\t\n\n<div class=\"publication_authors\"><span class=\"author-list\" style=\"font-style: italic;\">LPI, MEPhI, MIPT<\/span><span class=\"date\">(May 28, 2019)<\/span><\/div>\n\n --><\/p>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>B.&nbsp;Pal, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Vorobyev, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 091104(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.091104\" target=\"_blank\">10.1103\/PhysRevD.99.091104<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2488'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2488\" style=\"display: none;\">We report a search for the charmless baryonic decay <span class='MathJax_Preview'>\\(B^0 \\to p \\overline{p} \\pi^0\\)<script type='math\/tex'>B^0 \\to p \\overline{p} \\pi^0<\/script> with a data sample corresponding to an integrated luminosity of 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> containing <span class='MathJax_Preview'>\\((772 \\pm 10) \\times 10^6\\)<script type='math\/tex'>(772 \\pm 10) \\times 10^6<\/script> <span class='MathJax_Preview'>\\(B \\overline{B}\\)<script type='math\/tex'>B \\overline{B}<\/script> pairs. The data were collected by the Belle experiment running on the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance at the KEKB <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. We measure a branching fraction <span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to p \\overline{p} \\pi^0) = (5.0 \\pm 1.8 \\pm 0.6) \\times 10^{-7}\\)<script type='math\/tex'>{\\cal B}(B^0 \\to p \\overline{p} \\pi^0) = (5.0 \\pm 1.8 \\pm 0.6) \\times 10^{-7}<\/script>, where the first uncertainty is statistical and the second is systematic. The signal has a significance of 3.1 standard deviations and constitutes the first evidence for this decay mode. We also search for the intermediate two-body decays <span class='MathJax_Preview'>\\(B^0 \\to \\Delta^+ \\overline{p}\\)<script type='math\/tex'>B^0 \\to \\Delta^+ \\overline{p}<\/script> and <span class='MathJax_Preview'>\\(B^0 \\to \\overline{\\Delta}{}^- p\\)<script type='math\/tex'>B^0 \\to \\overline{\\Delta}{}^- p<\/script>, and set an upper limit on the branching fraction, <span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to \\Delta^+ \\overline{p}) + {\\cal B}(B^0 \\to \\overline{\\Delta}{}^- p) < 1.6 \\times 10^{-6}\\)<script type='math\/tex'>{\\cal B}(B^0 \\to \\Delta^+ \\overline{p}) + {\\cal B}(B^0 \\to \\overline{\\Delta}{}^- p) < 1.6 \\times 10^{-6}<\/script> at 90% confidence level.<\/span><\/div>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Observation of a fine structure in <span class='MathJax_Preview'>\\(e^+e^- \\to hadrons\\)<script type='math\/tex'>e^+e^- \\to hadrons<\/script> production at the nucleon-antinucleon threshold<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>R.R.&nbsp;Akhmetshin, ... , S.&nbsp;Eidelman,  et al. (CMD-3 Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physics Letters B 794 (2019) 64\u201368<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1016\/j.physletb.2019.05.032\" target=\"_blank\">10.1016\/j.physletb.2019.05.032<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2063'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2063\" style=\"display: none;\">A study of hadron production at the nucleon-antinucleon threshold has been performed with the CMD-3 detector at the VEPP-2000 <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. The very fast rise with about 1&nbsp;MeV width has been observed in the <span class='MathJax_Preview'>\\(e^+e^- \\to p \\overline{p}\\)<script type='math\/tex'>e^+e^- \\to p \\overline{p}<\/script> cross section. A sharp drop in the <span class='MathJax_Preview'>\\(e^+e^- \\to 3(\\pi^+ \\pi^-)\\)<script type='math\/tex'>e^+e^- \\to 3(\\pi^+ \\pi^-)<\/script> cross section has been confirmed and found to have a less than 2&nbsp;MeV width, in agreement with the observed fast rise of the <span class='MathJax_Preview'>\\(e^+e^- \\to p \\overline{p}\\)<script type='math\/tex'>e^+e^- \\to p \\overline{p}<\/script> cross section. For the first time a similar sharp drop is demonstrated in the <span class='MathJax_Preview'>\\(e^+e^- \\to K^+ K^- \\pi^+ \\pi^-\\)<script type='math\/tex'>e^+e^- \\to K^+ K^- \\pi^+ \\pi^-<\/script> cross section. The behavior of the <span class='MathJax_Preview'>\\(e^+e^- \\to 3(\\pi^+ \\pi^-)\\)<script type='math\/tex'>e^+e^- \\to 3(\\pi^+ \\pi^-)<\/script>, <span class='MathJax_Preview'>\\(K^+ K^- \\pi^+ \\pi^-\\)<script type='math\/tex'>K^+ K^- \\pi^+ \\pi^-<\/script> cross sections cannot be explained by an interference of any resonance amplitude with continuum, therefore this phenomenon cannot be due to a narrow near-threshold resonance. No such structure has been observed in the <span class='MathJax_Preview'>\\(e^+e^- \\to 2(\\pi^+ \\pi^-)\\)<script type='math\/tex'>e^+e^- \\to 2(\\pi^+ \\pi^-)<\/script> cross section.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">\u042d\u043a\u0441\u043f\u0435\u0440\u0438\u043c\u0435\u043d\u0442\u044b \u043d\u0430 \u043b\u0438\u043d\u0435\u0439\u043d\u043e\u043c \u043a\u043e\u043b\u043b\u0430\u0439\u0434\u0435\u0440\u0435 ILC: \u043e\u0436\u0438\u0434\u0430\u0435\u043c\u044b\u0435 \u0440\u0435\u0437\u0443\u043b\u044c\u0442\u0430\u0442\u044b \u0444\u0438\u0437\u0438\u0447\u0435\u0441\u043a\u0438\u0445 \u0438\u0441\u0441\u043b\u0435\u0434\u043e\u0432\u0430\u043d\u0438\u0439<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>\u0410.\u0413.&nbsp;\u0414\u0440\u0443\u0446\u043a\u043e\u0439<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">\u0423\u0441\u043f\u0435\u0445\u0438 \u0444\u0438\u0437\u0438\u0447\u0435\u0441\u043a\u0438\u0445 \u043d\u0430\u0443\u043a 189 (2019), \u2116&nbsp;5, \u0441.&nbsp;478\u2013493<br \/>DOI: <a href=\"https:\/\/doi.org\/10.3367\/UFNr.2018.07.038394\" target=\"_blank\">10.3367\/UFNr.2018.07.038394<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2039'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2039\" style=\"display: none;\">\u041f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u043e \u0441\u043e\u0432\u0440\u0435\u043c\u0435\u043d\u043d\u043e\u0435 \u0441\u043e\u0441\u0442\u043e\u044f\u043d\u0438\u0435 \u043f\u0440\u043e\u0435\u043a\u0442\u0430 \u043f\u043b\u0430\u043d\u0438\u0440\u0443\u0435\u043c\u043e\u0433\u043e \u0432 \u042f\u043f\u043e\u043d\u0438\u0438 \u041c\u0435\u0436\u0434\u0443\u043d\u0430\u0440\u043e\u0434\u043d\u043e\u0433\u043e \u043b\u0438\u043d\u0435\u0439\u043d\u043e\u0433\u043e <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script>-\u043a\u043e\u043b\u043b\u0430\u0439\u0434\u0435\u0440\u0430 (International Liner Collider, ILC). \u041e\u0431\u0441\u0443\u0436\u0434\u0430\u0435\u0442\u0441\u044f \u043f\u0440\u043e\u0433\u0440\u0430\u043c\u043c\u0430 \u0444\u0438\u0437\u0438\u0447\u0435\u0441\u043a\u0438\u0445 \u0438\u0441\u0441\u043b\u0435\u0434\u043e\u0432\u0430\u043d\u0438\u0439, \u043f\u0440\u0435\u0434\u043b\u0430\u0433\u0430\u0435\u043c\u044b\u0445 \u043d\u0430 ILC, \u043f\u0440\u0438 \u044d\u0442\u043e\u043c \u0431\u043e\u043b\u044c\u0448\u0435 \u0432\u043d\u0438\u043c\u0430\u043d\u0438\u044f \u0443\u0434\u0435\u043b\u0435\u043d\u043e \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u044f\u043c, \u0432\u043e\u0437\u043c\u043e\u0436\u043d\u044b\u043c \u043f\u0440\u0438 \u043f\u043e\u043b\u043d\u043e\u0439 \u044d\u043d\u0435\u0440\u0433\u0438\u0438 \u0441\u0442\u043e\u043b\u043a\u043d\u043e\u0432\u0435\u043d\u0438\u0439 250&nbsp;\u0413\u044d\u0412 \u0438 \u043e\u0436\u0438\u0434\u0430\u0435\u043c\u043e\u0439 \u0438\u043d\u0442\u0435\u0433\u0440\u0430\u043b\u044c\u043d\u043e\u0439 \u0441\u0432\u0435\u0442\u0438\u043c\u043e\u0441\u0442\u0438 ~&thinsp;2&nbsp;\u0430\u0431<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script>. \u042d\u0442\u043e \u0441\u0432\u044f\u0437\u0430\u043d\u043e \u0441 \u0442\u0435\u043c, \u0447\u0442\u043e \u043d\u0430 \u043f\u0435\u0440\u0432\u043e\u0439 \u0441\u0442\u0430\u0434\u0438\u0438 \u0441\u0442\u0440\u043e\u0438\u0442\u0435\u043b\u044c\u0441\u0442\u0432\u0430 \u043a\u043e\u043b\u043b\u0430\u0439\u0434\u0435\u0440\u0430 \u0431\u044b\u043b\u043e \u043f\u0440\u0435\u0434\u043b\u043e\u0436\u0435\u043d\u043e \u043e\u0433\u0440\u0430\u043d\u0438\u0447\u0438\u0442\u044c\u0441\u044f \u044d\u043d\u0435\u0440\u0433\u0438\u0435\u0439 250&nbsp;\u0413\u044d\u0412. \u041a\u0440\u0430\u0442\u043a\u043e \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u044b \u0442\u0435\u0445\u043d\u0438\u0447\u0435\u0441\u043a\u0438\u0435 \u0445\u0430\u0440\u0430\u043a\u0442\u0435\u0440\u0438\u0441\u0442\u0438\u043a\u0438 \u043f\u0440\u043e\u0435\u043a\u0442\u0430 \u0443\u0441\u043a\u043e\u0440\u0438\u0442\u0435\u043b\u044c\u043d\u043e\u0433\u043e \u043a\u043e\u043c\u043f\u043b\u0435\u043a\u0441\u0430 ILC \u0438 \u043f\u043b\u0430\u043d\u0438\u0440\u0443\u0435\u043c\u043e\u0433\u043e \u0434\u0435\u0442\u0435\u043a\u0442\u043e\u0440\u0430 ILD (International Large Detector).<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for the <span class='MathJax_Preview'>\\(B \\to Y(4260) K\\)<script type='math\/tex'>B \\to Y(4260) K<\/script>, <span class='MathJax_Preview'>\\(Y(4260) \\to J\/\\psi \\pi^+ \\pi^-\\)<script type='math\/tex'>Y(4260) \\to J\/\\psi \\pi^+ \\pi^-<\/script> decays<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>R.&nbsp;Garg, V.&nbsp;Bhardwaj, J.B.&nbsp;Singh, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 071102(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.071102\" target=\"_blank\">10.1103\/PhysRevD.99.071102<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2254'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2254\" style=\"display: none;\">We report the results of a search for the <span class='MathJax_Preview'>\\(B \\to Y(4260) K\\)<script type='math\/tex'>B \\to Y(4260) K<\/script>, <span class='MathJax_Preview'>\\(Y(4260) \\to J\/\\psi \\pi^+ \\pi^-\\)<script type='math\/tex'>Y(4260) \\to J\/\\psi \\pi^+ \\pi^-<\/script> decays. This study is based on a data sample corresponding to an integrated luminosity of 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script>, collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. We investigate the <span class='MathJax_Preview'>\\(J\/\\psi \\pi^+ \\pi^-\\)<script type='math\/tex'>J\/\\psi \\pi^+ \\pi^-<\/script> invariant mass distribution in the range 4.0 to 4.6&nbsp;GeV<span class='MathJax_Preview'>\\(\/c^2\\)<script type='math\/tex'>\/c^2<\/script> using both <span class='MathJax_Preview'>\\(B^+ \\to J\/\\psi \\pi^+ \\pi^- K^+\\)<script type='math\/tex'>B^+ \\to J\/\\psi \\pi^+ \\pi^- K^+<\/script> and <span class='MathJax_Preview'>\\(B^0 \\to J\/\\psi \\pi^+ \\pi^- K_S^0\\)<script type='math\/tex'>B^0 \\to J\/\\psi \\pi^+ \\pi^- K_S^0<\/script> decays. We find excesses of events above the background levels, with significances of 2.1 and 0.9 standard deviations for charged and neutral <span class='MathJax_Preview'>\\(B \\to Y(4260) K\\)<script type='math\/tex'>B \\to Y(4260) K<\/script> decays, respectively, taking into account the systematic uncertainties. These correspond to upper limits on the product of branching fractions, <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to Y(4260) K^+) \\times {\\cal B}(Y(4260) \\to J\/\\psi \\pi^+ \\pi^-) < 1.4 \\times 10^{-5}\\)<script type='math\/tex'>{\\cal B}(B^+ \\to Y(4260) K^+) \\times {\\cal B}(Y(4260) \\to J\/\\psi \\pi^+ \\pi^-) < 1.4 \\times 10^{-5}<\/script> and <span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to Y(4260) K^0) \\times {\\cal B}(Y(4260) \\to J\/\\psi \\pi^+ \\pi^-) < 1.7 \\times 10^{-5}\\)<script type='math\/tex'>{\\cal B}(B^0 \\to Y(4260) K^0) \\times {\\cal B}(Y(4260) \\to J\/\\psi \\pi^+ \\pi^-) < 1.7 \\times 10^{-5}<\/script> at the 90% confidence level.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Determination of the <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation parameters at Belle&nbsp;II<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>P.&nbsp;Pakhlov<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of Physics: Conference Series 1137 (2019) 012058<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1742-6596\/1137\/1\/012058\" target=\"_blank\">10.1088\/1742-6596\/1137\/1\/012058<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2422'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2422\" style=\"display: none;\">This paper briefly describes some prospects for new physics searches related to <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation studies in <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> decays with the Belle&nbsp;II experiment. With a design luminosity of <span class='MathJax_Preview'>\\(8 \\cdot 10^{35}\\)<script type='math\/tex'>8 \\cdot 10^{35}<\/script>&nbsp;cm<span class='MathJax_Preview'>\\(^{-2}\\)<script type='math\/tex'>^{-2}<\/script>s<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script>, and an integrated luminosity above 50&nbsp;ab<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script>, the new <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script>-factory SuperKEKB will exceed the record instantaneous luminosity of its predecessor KEKB by a factor of 40. The new Belle&nbsp;II detector with most subsystems upgraded will allow to measure the parameters of <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation even more precisely in spite of increased backgrounds and radiation loads. The CKM mechanism is expected to be tested at 1% level at Belle&nbsp;II.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">First Measurements of Absolute Branching Fractions of the <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> Baryon at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Y.B.&nbsp;Li, C.P.&nbsp;Shen, C.Z.&nbsp;Yuan, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 122 (2019) 082001<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.082001\" target=\"_blank\">10.1103\/PhysRevLett.122.082001<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2065'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2065\" style=\"display: none;\">We present the first measurements of absolute branching fractions of <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> decays into <span class='MathJax_Preview'>\\(\\Xi^- \\pi^+\\)<script type='math\/tex'>\\Xi^- \\pi^+<\/script>, <span class='MathJax_Preview'>\\(\\Lambda K^- \\pi^+\\)<script type='math\/tex'>\\Lambda K^- \\pi^+<\/script>, and <span class='MathJax_Preview'>\\(p K^- K^- \\pi^+\\)<script type='math\/tex'>p K^- K^- \\pi^+<\/script> final states. The measurements are made using a dataset comprising <span class='MathJax_Preview'>\\((772 \\pm 11) \\times 10^6\\)<script type='math\/tex'>(772 \\pm 11) \\times 10^6<\/script> <span class='MathJax_Preview'>\\(B \\overline{B}\\)<script type='math\/tex'>B \\overline{B}<\/script> pairs collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. We first measure the absolute branching fraction for <span class='MathJax_Preview'>\\(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0\\)<script type='math\/tex'>B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0<\/script> using a missing-mass technique; the result is <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0) = (9.51 \\pm 2.10 \\pm 0.88) \\times 10^{-4}\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0) = (9.51 \\pm 2.10 \\pm 0.88) \\times 10^{-4}<\/script>. We subsequently measure the product branching fractions <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)<\/script>, <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+)<\/script>, and <span class='MathJax_Preview'>\\({\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0){\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+)<\/script> with improved precision. Dividing these product branching fractions by the result for <span class='MathJax_Preview'>\\(B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0\\)<script type='math\/tex'>B^- \\to \\overline{\\Lambda_c}{}^- \\Xi_c^0<\/script> yields the following branching fractions: <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+) = (1.80 \\pm 0.50 \\pm 0.14)\\%\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+) = (1.80 \\pm 0.50 \\pm 0.14)\\%<\/script>, <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+) = (1.17 \\pm 0.37 \\pm 0.09)\\%\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to \\Lambda K^- \\pi^+) = (1.17 \\pm 0.37 \\pm 0.09)\\%<\/script>, and <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+) = (0.58 \\pm 0.23 \\pm 0.05)\\%\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to p K^- K^- \\pi^+) = (0.58 \\pm 0.23 \\pm 0.05)\\%<\/script>. For the above branching fractions, the first uncertainties are statistical and the second are systematic. Our result for <span class='MathJax_Preview'>\\({\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)\\)<script type='math\/tex'>{\\cal B}(\\Xi_c^0 \\to \\Xi^- \\pi^+)<\/script> can be combined with <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> branching fractions measured relative to <span class='MathJax_Preview'>\\(\\Xi_c^0 \\to \\Xi^- \\pi^+\\)<script type='math\/tex'>\\Xi_c^0 \\to \\Xi^- \\pi^+<\/script> to yield other absolute <span class='MathJax_Preview'>\\(\\Xi_c^0\\)<script type='math\/tex'>\\Xi_c^0<\/script> branching fractions.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Observation of <span class='MathJax_Preview'>\\(\\Xi(1620)^0\\)<script type='math\/tex'>\\Xi(1620)^0<\/script> and Evidence for <span class='MathJax_Preview'>\\(\\Xi(1690)^0\\)<script type='math\/tex'>\\Xi(1690)^0<\/script> in <span class='MathJax_Preview'>\\(\\Xi_c^+ \\to \\Xi^- \\pi^+ \\pi^+\\)<script type='math\/tex'>\\Xi_c^+ \\to \\Xi^- \\pi^+ \\pi^+<\/script> Decays<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Sumihama, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 122 (2019) 072501<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.072501\" target=\"_blank\">10.1103\/PhysRevLett.122.072501<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1970'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1970\" style=\"display: none;\">We report the first observation of the double strange baryon <span class='MathJax_Preview'>\\(\\Xi(1620)^0\\)<script type='math\/tex'>\\Xi(1620)^0<\/script> in its decay to <span class='MathJax_Preview'>\\(\\Xi^- \\pi^+\\)<script type='math\/tex'>\\Xi^- \\pi^+<\/script> via <span class='MathJax_Preview'>\\(\\Xi_c^+ \\to \\Xi^- \\pi^+ \\pi^+\\)<script type='math\/tex'>\\Xi_c^+ \\to \\Xi^- \\pi^+ \\pi^+<\/script> decays based on a 980&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> data sample collected with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. The mass and width are measured to be <span class='MathJax_Preview'>\\(1610.4 \\pm 6.0\\)<script type='math\/tex'>1610.4 \\pm 6.0<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(^{+6.1}_{-4.2}\\)<script type='math\/tex'>^{+6.1}_{-4.2}<\/script>&nbsp;(syst)&nbsp;MeV<span class='MathJax_Preview'>\\(\/c^2\\)<script type='math\/tex'>\/c^2<\/script> and <span class='MathJax_Preview'>\\(59.9 \\pm 4.8\\)<script type='math\/tex'>59.9 \\pm 4.8<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(^{+2.8}_{-7.1}\\)<script type='math\/tex'>^{+2.8}_{-7.1}<\/script>&nbsp;(syst)&nbsp;MeV, respectively. We obtain <span class='MathJax_Preview'>\\(4.0\\sigma\\)<script type='math\/tex'>4.0\\sigma<\/script> evidence of the <span class='MathJax_Preview'>\\(\\Xi(1690)^0\\)<script type='math\/tex'>\\Xi(1690)^0<\/script> with the same data sample. These results shed light on the structure of hyperon resonances with strangeness <span class='MathJax_Preview'>\\(S = -2\\)<script type='math\/tex'>S = -2<\/script>.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Measurements of branching fraction and direct <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> asymmetry in <span class='MathJax_Preview'>\\(B^\\pm \\to K_S^0 K_S^0 K^\\pm\\)<script type='math\/tex'>B^\\pm \\to K_S^0 K_S^0 K^\\pm<\/script> and a search for <span class='MathJax_Preview'>\\(B^\\pm \\to K_S^0 K_S^0 \\pi^\\pm\\)<script type='math\/tex'>B^\\pm \\to K_S^0 K_S^0 \\pi^\\pm<\/script><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.B.&nbsp;Kaliyar, P.&nbsp;Behera, G.B.&nbsp;Mohanty, V.&nbsp;Gaur, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 031102(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.031102\" target=\"_blank\">10.1103\/PhysRevD.99.031102<\/a><span class=\"title\"> <\/span><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2190'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2190\" style=\"display: none;\">We study charmless hadronic decays of charged <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> mesons to the final states <span class='MathJax_Preview'>\\(K_S^0 K_S^0 K^\\pm\\)<script type='math\/tex'>K_S^0 K_S^0 K^\\pm<\/script> and <span class='MathJax_Preview'>\\(K_S^0 K_S^0 \\pi^\\pm\\)<script type='math\/tex'>K_S^0 K_S^0 \\pi^\\pm<\/script> using a 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> data sample that contains <span class='MathJax_Preview'>\\(772 \\times 10^6\\)<script type='math\/tex'>772 \\times 10^6<\/script> <span class='MathJax_Preview'>\\(B \\overline{B}\\)<script type='math\/tex'>B \\overline{B}<\/script> pairs and was collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. For <span class='MathJax_Preview'><\\(B^\\pm \\to K_S^0 K_S^0 K^\\pm\\)<script type='math\/tex'>B^\\pm \\to K_S^0 K_S^0 K^\\pm<\/script>, the measured branching fraction and direct <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> asymmetry are <span class='MathJax_Preview'>\\([10.42 \\pm 0.43\\)<script type='math\/tex'>[10.42 \\pm 0.43<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;0.22\\)<script type='math\/tex'>\\pm\\;0.22<\/script>&nbsp;(syst)<span class='MathJax_Preview'>\\(] \\times 10^{-6}\\)<script type='math\/tex'>] \\times 10^{-6}<\/script> and <span class='MathJax_Preview'>\\([+1.6 \\pm 3.9\\)<script type='math\/tex'>[+1.6 \\pm 3.9<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;0.9\\)<script type='math\/tex'>\\pm\\;0.9<\/script>&nbsp;(syst)<span class='MathJax_Preview'>\\(]\\%\\)<script type='math\/tex'>]\\%<\/script>, respectively. In the absence of a statistically significant signal for <span class='MathJax_Preview'>\\(B^\\pm \\to K_S^0 K_S^0 \\pi^\\pm\\)<script type='math\/tex'>B^\\pm \\to K_S^0 K_S^0 \\pi^\\pm<\/script>, we obtain a 90% confidence-level upper limit on its branching fraction as <span class='MathJax_Preview'>\\(8.7 \\times 10^{-7}\\)<script type='math\/tex'>8.7 \\times 10^{-7}<\/script>.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Recent results of the DANSS experiment<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Danilov on behalf of the DANSS Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Il Nuovo Cimento C 41 (2018) 162<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1393\/ncc\/i2018-18162-0\" target=\"_blank\">10.1393\/ncc\/i2018-18162-0<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2055'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2055\" style=\"display: none;\">DANSS is a highly segmented 1&nbsp;m<span class='MathJax_Preview'>\\(^3\\)<script type='math\/tex'>^3<\/script> plastic scintillator detector. Its 2500 one meter long scintillator strips have a Gd-loaded reflective cover. The DANSS detector is placed under an industrial 3.1&nbsp;GW<sub>th<\/sub> reactor of the Kalinin Nuclear Power Plant 350&nbsp;km NW from Moscow. The distance to the core is varied on-line from 10.7&nbsp;m to 12.7&nbsp;m. Recent results on searches for a sterile neutrino are presented as well as measurements of the antneutrino spectrum dependence on the fuel composition. All results are preliminary.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Observation of <span class='MathJax_Preview'>\\(B^+ \\to p \\overline{\\Lambda} K^+ K^-\\)<script type='math\/tex'>B^+ \\to p \\overline{\\Lambda} K^+ K^-<\/script> and <span class='MathJax_Preview'>\\(B^+ \\to \\overline{p} \\Lambda K^+ K^+\\)<script type='math\/tex'>B^+ \\to \\overline{p} \\Lambda K^+ K^+<\/script><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>P.-C.&nbsp;Lu, M.-Z.&nbsp;Wang, R.&nbsp;Chistov, P.&nbsp;Chang et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 032003<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.032003\" target=\"_blank\">10.1103\/PhysRevD.99.032003<\/a><span class=\"title\"> <\/span><\/p>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2011'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2011\" style=\"display: none;\">We report the study of <span class='MathJax_Preview'>\\(B^+ \\to p \\overline{\\Lambda} K^+ K^-\\)<script type='math\/tex'>B^+ \\to p \\overline{\\Lambda} K^+ K^-<\/script> and <span class='MathJax_Preview'>\\(B^+ \\to \\overline{p} \\Lambda K^+ K^+\\)<script type='math\/tex'>B^+ \\to \\overline{p} \\Lambda K^+ K^+<\/script> decays using a <span class='MathJax_Preview'>\\(772 \\times 10^6\\)<script type='math\/tex'>772 \\times 10^6<\/script> <span class='MathJax_Preview'><\\(B \\overline{B}\\)<script type='math\/tex'>B \\overline{B}<\/script> pair data sample recorded on the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at KEKB. The following branching fractions are measured: <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to p \\overline{\\Lambda} K^+ K^-) = (4.10\\,^{+0.45}_{-0.43} \\pm 0.50) \\times 10^{-6}\\)<script type='math\/tex'>{\\cal B}(B^+ \\to p \\overline{\\Lambda} K^+ K^-) = (4.10\\,^{+0.45}_{-0.43} \\pm 0.50) \\times 10^{-6}<\/script>, <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to \\overline{p} \\Lambda K^+ K^+) = (3.70\\,^{+0.39}_{-0.37} \\pm 0.44) \\times 10^{-6}\\)<script type='math\/tex'>{\\cal B}(B^+ \\to \\overline{p} \\Lambda K^+ K^+) = (3.70\\,^{+0.39}_{-0.37} \\pm 0.44) \\times 10^{-6}<\/script>, <span class='MathJax_Preview'>\\({\\cal B}(\\eta_c \\to p \\overline{\\Lambda} K^- + c.c.) = (2.83\\,^{+0.36}_{-0.34} \\pm 0.35) \\times 10^{-3}\\)<script type='math\/tex'>{\\cal B}(\\eta_c \\to p \\overline{\\Lambda} K^- + c.c.) = (2.83\\,^{+0.36}_{-0.34} \\pm 0.35) \\times 10^{-3}<\/script> and <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to p \\overline{\\Lambda} \\phi) =(7.95 \\pm 2.09 \\pm 0.77) \\times 10^{-7}\\)<script type='math\/tex'>{\\cal B}(B^+ \\to p \\overline{\\Lambda} \\phi) =(7.95 \\pm 2.09 \\pm 0.77) \\times 10^{-7}<\/script>, where <span class='MathJax_Preview'>\\(c.c.\\)<script type='math\/tex'>c.c.<\/script> denotes the corresponding charge-conjugation process. The intermediate resonance decays are excluded in the four-body decay measurements. We also find evidence for <span class='MathJax_Preview'>\\({\\cal B}(\\eta_c \\to \\Lambda(1520) \\overline{\\Lambda} + c.c.) = (3.48 \\pm 1.48 \\pm 0.46) \\times 10^{-3}\\)<script type='math\/tex'>{\\cal B}(\\eta_c \\to \\Lambda(1520) \\overline{\\Lambda} + c.c.) = (3.48 \\pm 1.48 \\pm 0.46) \\times 10^{-3}<\/script> and <span class='MathJax_Preview'>\\({\\cal B}(B^+ \\to \\Lambda(1520) \\overline{\\Lambda} K^+) =\\)<script type='math\/tex'>{\\cal B}(B^+ \\to \\Lambda(1520) \\overline{\\Lambda} K^+) =<\/script> <span class='MathJax_Preview'>\\((2.23 \\pm 0.63 \\pm 0.25) \\times 10^{-6}\\)<script type='math\/tex'>(2.23 \\pm 0.63 \\pm 0.25) \\times 10^{-6}<\/script>. No significant signals are found for <span class='MathJax_Preview'>\\(J\/\\psi \\to \\Lambda(1520) \\overline{\\Lambda} + c.c.\\)<script type='math\/tex'>J\/\\psi \\to \\Lambda(1520) \\overline{\\Lambda} + c.c.<\/script> and <span class='MathJax_Preview'>\\(B^+ \\to  \\overline{\\Lambda}(1520) \\Lambda K^+\\)<script type='math\/tex'>B^+ \\to  \\overline{\\Lambda}(1520) \\Lambda K^+<\/script>; we set the 90% confidence level upper limits on their decay branching fractions as <span class='MathJax_Preview'>\\(< 1.80 \\times 10^{-3}\\)<script type='math\/tex'>< 1.80 \\times 10^{-3}<\/script> and <span class='MathJax_Preview'>\\(< 2.08 \\times 10^{-6}\\)<script type='math\/tex'>< 2.08 \\times 10^{-6}<\/script>, respectively.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Hadronic transitions in bottomonia at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>S.&nbsp;Eidelman for the Belle Collaboration<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">EPJ Web of Conferences 199 (2019) 01001<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1051\/epjconf\/201919901001\" target=\"_blank\">10.1051\/epjconf\/201919901001<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2312'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2312\" style=\"display: none;\">Recent Belle results on various hadronic transitions among bottomonia are presented. We observe transitions with the <span class='MathJax_Preview'>\\(\\eta\\)<script type='math\/tex'>\\eta<\/script> and <span class='MathJax_Preview'>\\(\\eta^\\prime\\)<script type='math\/tex'>\\eta^\\prime<\/script> meson at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script>. Bottomonium production together with the <span class='MathJax_Preview'>\\(\\eta\\)<script type='math\/tex'>\\eta<\/script> meson is also reported at the <span class='MathJax_Preview'>\\(\\Upsilon(10860)\\)<script type='math\/tex'>\\Upsilon(10860)<\/script>. We study <span class='MathJax_Preview'>\\(\\pi^+ \\pi^- \\pi^0\\)<script type='math\/tex'>\\pi^+ \\pi^- \\pi^0<\/script> transitions at the <span class='MathJax_Preview'>\\(\\Upsilon(10860)\\)<script type='math\/tex'>\\Upsilon(10860)<\/script> and <span class='MathJax_Preview'>\\(\\Upsilon(11020)\\)<script type='math\/tex'>\\Upsilon(11020)<\/script>.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Constraints on Hidden Photons Produced in Nuclear Reactors<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Danilov, S.&nbsp;Demidov, and D.&nbsp;Gorbunov<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 122 (2019) 041801<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.041801\" target=\"_blank\">10.1103\/PhysRevLett.122.041801<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1856'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1856\" style=\"display: none;\">New light vector particles&nbsp;&mdash; hidden photons&nbsp;&mdash; are present in many extensions of the standard model of particle physics. They can be produced in nuclear reactors and registered by neutrino detectors. We obtain new limits on the models with the hidden photons from an analysis of published results of the TEXONO neutrino experiment. Accounting for oscillations between the visible and hidden photons, we find that the neutrino experiments are generally insensitive to the hidden photons lighter than \u223c0.1&nbsp;eV.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Observation of Transverse <span class='MathJax_Preview'>\\(\\Lambda \/ \\overline{\\Lambda}\\)<script type='math\/tex'>\\Lambda \/ \\overline{\\Lambda}<\/script> Hyperon Polarization in <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> Annihilation at Belle<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Y.&nbsp;Guan, A.&nbsp;Vossen, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 122 (2019) 042001<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.042001\" target=\"_blank\">10.1103\/PhysRevLett.122.042001<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2302'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2302\" style=\"display: none;\">We report the first observation of the spontaneous polarization of <span class='MathJax_Preview'>\\(\\Lambda\\)<script type='math\/tex'>\\Lambda<\/script> and <span class='MathJax_Preview'>\\(\\overline{\\Lambda}\\)<script type='math\/tex'>\\overline{\\Lambda}<\/script> hyperons transverse to the production plane in <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> annihilation, which is attributed to the effect arising from a polarizing fragmentation function. For inclusive <span class='MathJax_Preview'>\\(\\Lambda \/ \\overline{\\Lambda}\\)<script type='math\/tex'>\\Lambda \/ \\overline{\\Lambda}<\/script> production, we also report results with subtracted feed-down contributions from <span class='MathJax_Preview'>\\(\\Sigma^0\\)<script type='math\/tex'>\\Sigma^0<\/script> and charm. This measurement uses a dataset of 800.4&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> collected by the Belle experiment at or near a center-of-mass energy of 10.58&nbsp;GeV. We observe a significant polarization that rises with the fractional energy carried by the <span class='MathJax_Preview'>\\(\\Lambda \/ \\overline{\\Lambda}\\)<script type='math\/tex'>\\Lambda \/ \\overline{\\Lambda}<\/script> hyperon.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation with kinematic asymmetries in the <span class='MathJax_Preview'>\\(D^0 \\to K^+ K^- \\pi^+ \\pi^-\\)<script type='math\/tex'>D^0 \\to K^+ K^- \\pi^+ \\pi^-<\/script> decay<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>J.B.&nbsp;Kim, E.&nbsp;Won, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 99 (2019) 011104(R)<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.99.011104\" target=\"_blank\">10.1103\/PhysRevD.99.011104<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1971'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1971\" style=\"display: none;\">We search for <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation in the singly-Cabibbo-suppressed decay <span class='MathJax_Preview'>\\(D^0 \\to K^+ K^- \\pi^+ \\pi^-\\)<script type='math\/tex'>D^0 \\to K^+ K^- \\pi^+ \\pi^-<\/script> using data corresponding to an integrated luminosity of 988&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> collected by the Belle detector at the KEKB <span class='MathJax_Preview'>\\(e^+e^-\\)<script type='math\/tex'>e^+e^-<\/script> collider. We measure a set of five kinematically dependent <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> asymmetries, of which four asymmetries are measured for the first time. The set of asymmetry measurements can be sensitive to <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation via interference between the different partial-wave contributions to the decay and performed on other pseudoscalar decays. We find no evidence of <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script> violation.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\" >\n<div class=\"publication_title\">Search for a Light <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script>-odd Higgs Boson and Low-Mass Dark Matter at the Belle Experiment<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>I.S.&nbsp;Seong, S.E.&nbsp;Vahsen, ...&nbsp;, S.&nbsp;Eidelman et al.&nbsp;(Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 122 (2019) 011801<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.122.011801\" target=\"_blank\">10.1103\/PhysRevLett.122.011801<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1946'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1946\" style=\"display: none;\">We report on the first Belle search for a light <span class='MathJax_Preview'>\\(CP\\)<script type='math\/tex'>CP<\/script>-odd Higgs boson, <span class='MathJax_Preview'>\\(A^0\\)<script type='math\/tex'>A^0<\/script>, that decays into low mass dark matter, <span class='MathJax_Preview'>\\(\\chi\\)<script type='math\/tex'>\\chi<\/script>, in final states with a single photon and missing energy. We search for events produced via the dipion transition <span class='MathJax_Preview'>\\(\\Upsilon(2S) \\to \\Upsilon(1S) \\pi^+ \\pi^-\\)<script type='math\/tex'>\\Upsilon(2S) \\to \\Upsilon(1S) \\pi^+ \\pi^-<\/script>, followed by the on-shell process <span class='MathJax_Preview'>\\(\\Upsilon(1S) \\to \\gamma A^0\\)<script type='math\/tex'>\\Upsilon(1S) \\to \\gamma A^0<\/script> with <span class='MathJax_Preview'>\\(A^0 \\to \\chi \\chi\\)<script type='math\/tex'>A^0 \\to \\chi \\chi<\/script>, or by the off-shell process <span class='MathJax_Preview'>\\(\\Upsilon(1S) \\to \\gamma \\chi \\chi\\)<script type='math\/tex'>\\Upsilon(1S) \\to \\gamma \\chi \\chi<\/script>. Utilizing a data sample of <span class='MathJax_Preview'>\\(157.3 \\times 10^6\\)<script type='math\/tex'>157.3 \\times 10^6<\/script> <span class='MathJax_Preview'>\\(\\Upsilon(2S)\\)<script type='math\/tex'>\\Upsilon(2S)<\/script> decays, we find no evidence for a signal. We set limits on the branching fractions of such processes in the mass ranges <span class='MathJax_Preview'>\\(M_{A^0} <\\)<script type='math\/tex'>M_{A^0} <<\/script> 8.97&nbsp;GeV<span class='MathJax_Preview'>\\(\/c^2\\)<script type='math\/tex'>\/c^2<\/script> and <span class='MathJax_Preview'>\\(M_\\chi <\\)<script type='math\/tex'>M_\\chi <<\/script> 4.44&nbsp;GeV<span class='MathJax_Preview'>\\(\/c^2\\)<script type='math\/tex'>\/c^2<\/script>. We then use the limits on the off-shell process to set competitive limits on WIMP-nucleon scattering in the WIMP mass range below 5&nbsp;GeV<span class='MathJax_Preview'>\\(\/c^2\\)<script type='math\/tex'>\/c^2<\/script>.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<\/ol>\n<\/div>\n<h3 align=\"center\">2018 \u0433\u043e\u0434<\/h3>\n<div class=\"publication-archive\">\n<ol style=\"padding: 0; padding-left: 18pt;\">\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Search for the rare decay of <span class='MathJax_Preview'>\\(B^+ \\to {\\cal l}^+ \\nu_{\\cal l} \\gamma\\)<script type='math\/tex'>B^+ \\to {\\cal l}^+ \\nu_{\\cal l} \\gamma<\/script> with improved hadronic tagging<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>M.&nbsp;Gelb, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 98 (2018) 112016<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevD.98.112016\" target=\"_blank\">10.1103\/PhysRevD.98.112016<\/a><span class=\"title\"><\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2046'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2046\" style=\"display: none;\">We present the result of the search for the rare <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> meson decay of <span class='MathJax_Preview'>\\(B^+ \\to {\\cal l}^+ \\nu_{\\cal l} \\gamma\\)<script type='math\/tex'>B^+ \\to {\\cal l}^+ \\nu_{\\cal l} \\gamma<\/script> with <span class='MathJax_Preview'>\\({\\cal l} = e, \\mu\\)<script type='math\/tex'>{\\cal l} = e, \\mu<\/script>. For the search the full data set recorded by the Belle experiment of 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<script type='math\/tex'>^{-1}<\/script> integrated luminosity near the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<script type='math\/tex'>\\Upsilon(4S)<\/script> resonance is used. Signal candidates are reconstructed for photon energies <span class='MathJax_Preview'>\\(E_\\gamma\\)<script type='math\/tex'>E_\\gamma<\/script> larger than 1&nbsp;GeV using a novel multivariate tagging algorithm. The novel algorithm fully reconstructs the second <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> meson produced in the collision using hadronic modes and was specifically trained to recognize the signal signature in combination with hadronic tag-side <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> meson decays. This approach greatly enhances the performance. Background processes that can mimic this signature, mainly charmless semileptonic decays and continuum processes, are suppressed using multivariate methods. The number of signal candidates is determined by analyzing the missing mass squared distribution as inferred from the signal side particles and the kinematic properties of the tag-side <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> meson. No significant excess over the background-only hypothesis is observed and upper limits on the partial branching fraction <span class='MathJax_Preview'>\\(\\Delta {\\cal B}\\)<script type='math\/tex'>\\Delta {\\cal B}<\/script> with <span class='MathJax_Preview'>\\(E_\\gamma\\)<script type='math\/tex'>E_\\gamma<\/script> > 1&nbsp;GeV individually for electron and muon final states as well as for the average branching fraction of both lepton final states are reported. We find a Bayesian upper limit of <span class='MathJax_Preview'>\\(\\Delta {\\cal B}(B^+ \\to {\\cal l}^+ \\nu_{\\cal l} \\gamma) < 3.0 \\times 10^{-6}\\)<script type='math\/tex'>\\Delta {\\cal B}(B^+ \\to {\\cal l}^+ \\nu_{\\cal l} \\gamma) < 3.0 \\times 10^{-6}<\/script> at 90% CL and also report an upper limit on the first inverse moment of the light-cone distribution amplitude of the <span class='MathJax_Preview'>\\(B\\)<script type='math\/tex'>B<\/script> meson of <span class='MathJax_Preview'>\\(\\lambda_B > 0.24\\)<script type='math\/tex'>\\lambda_B > 0.24<\/script>&nbsp; GeV at 90% CL.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Hadronic energy resolution of a combined high granularity scintillator calorimeter system<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>J.&nbsp;Repond, ... , M.&nbsp;Chadeeva, M.&nbsp;Danilov, A.&nbsp;Drutskoy et al. (CALICE Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of Instrumentation 13 (2018) P12022<br \/>DOI: <a href=\"https:\/\/doi.org\/10.1088\/1748-0221\/13\/12\/P12022\" target=\"_blank\">10.1088\/1748-0221\/13\/12\/P12022<\/a><span class=\"title\"><\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1948'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1948\" style=\"display: none;\">This paper presents results obtained with the combined CALICE Scintillator Electromagnetic Calorimeter, Analogue Hadronic Calorimeter and Tail Catcher & Muon Tracker, three high granularity scintillator-silicon photomultiplier calorimeter prototypes. The response of the system to pions with momenta between 4&nbsp;GeV<span class='MathJax_Preview'>\\(\/c\\)<script type='math\/tex'>\/c<\/script> and 32&nbsp;GeV<span class='MathJax_Preview'>\\(\/c\\)<script type='math\/tex'>\/c<\/script> is analysed, including the average energy response, resolution, and longitudinal shower profiles. Two techniques are applied to reconstruct the initial particle energy from the measured energy depositions; a standard energy reconstruction which is linear in the measured depositions and a software compensation technique based on reweighting individually measured depositions according to their hit energy. The results are compared to predictions of the G<span style=\"font-variant: small-caps;\">eant<\/span>4 physics lists QGSP_BERT_HP and FTFP_BERT_HP.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Measurement of the branching fraction and time-dependent <span class='MathJax_Preview'>\\(CP\\)<\/span><script type='math\/tex'>CP<\/script> asymmetry for <span class='MathJax_Preview'>\\(B^0 \\to J\/\\psi \\pi^0\\)<\/span><script type='math\/tex'>B^0 \\to J\/\\psi \\pi^0<\/script> decays<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>B.&nbsp;Pal, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Vorobyev, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 98 (2018) 112008<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1103\/PhysRevD.98.112008\" target=\"_blank\">10.1103\/PhysRevD.98.112008<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1961'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1961\" style=\"display: none;\">We measure the branching fraction and time-dependent <span class='MathJax_Preview'>\\(CP\\)<\/span><script type='math\/tex'>CP<\/script>-violating asymmetry for <span class='MathJax_Preview'>\\(B^0 \\to J\/\\psi \\pi^0\\)<\/span><script type='math\/tex'>B^0 \\to J\/\\psi \\pi^0<\/script> decays using a data sample of 711&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script> collected on the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script> resonance by the Belle experiment running at the KEKB <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> collider. The branching fraction is measured to be <span class='MathJax_Preview'>\\({\\cal B}(B^0 \\to J\/\\psi \\pi^0) = \\left[1.62  \\pm 0.11\\right.\\)<\/span><script type='math\/tex'>{\\cal B}(B^0 \\to J\/\\psi \\pi^0) = \\left[1.62  \\pm 0.11\\right.<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;0.06\\)<\/span><script type='math\/tex'>\\pm\\;0.06<\/script>&nbsp;(syst)<span class='MathJax_Preview'>\\(\\left.\\right] \\times 10^{-5}\\)<\/span><script type='math\/tex'>\\left.\\right] \\times 10^{-5}<\/script>, which is the most precise measurement to date. The measured <span class='MathJax_Preview'>\\(CP\\)<\/span><script type='math\/tex'>CP<\/script> asymmetry parameters are <span class='MathJax_Preview'>\\({\\cal S} = -0.59 \\pm 0.19\\)<\/span><script type='math\/tex'>{\\cal S} = -0.59 \\pm 0.19<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;0.03\\)<\/span><script type='math\/tex'>\\pm\\;0.03<\/script>&nbsp;(syst) and <span class='MathJax_Preview'>\\({\\cal A} = -0.15 \\pm 0.14\\)<\/span><script type='math\/tex'>{\\cal A} = -0.15 \\pm 0.14<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(^{+0.04}_{-0.03}\\)<\/span><script type='math\/tex'>^{+0.04}_{-0.03}<\/script>&nbsp;(syst). The mixing-induced <span class='MathJax_Preview'>\\(CP\\)<\/span><script type='math\/tex'>CP<\/script> asymmetry <span class='MathJax_Preview'>\\(({\\cal S})\\)<\/span><script type='math\/tex'>({\\cal S})<\/script> differs from the case of no <span class='MathJax_Preview'>\\(CP\\)<\/span><script type='math\/tex'>CP<\/script> violation by 3.0 standard deviations, and the direct <span class='MathJax_Preview'>\\(CP\\)<\/span><script type='math\/tex'>CP<\/script> asymmetry <span class='MathJax_Preview'>\\(({\\cal A})\\)<\/span><script type='math\/tex'>({\\cal A})<\/script> is consistent with zero.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Observation of <span class='MathJax_Preview'>\\(\\Upsilon(2S) \\to \\gamma \\eta_b(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(2S) \\to \\gamma \\eta_b(1S)<\/script> Decay<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>B.G.&nbsp;Fulsom, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, P.&nbsp;Pakhlov, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Vorobyev, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 121 (2018) 232001<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1103\/PhysRevLett.121.232001\" target=\"_blank\">10.1103\/PhysRevLett.121.232001<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2103'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2103\" style=\"display: none;\">We report the observation of <span class='MathJax_Preview'>\\(\\Upsilon(2S) \\to \\gamma \\eta_b(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(2S) \\to \\gamma \\eta_b(1S)<\/script> decay based on an analysis of the inclusive photon spectrum of 24.7&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script> of <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> collisions at the <span class='MathJax_Preview'>\\(\\Upsilon(2S)\\)<\/span><script type='math\/tex'>\\Upsilon(2S)<\/script> center-of-mass energy collected with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> collider. We measure a branching fraction of <span class='MathJax_Preview'>\\(B\\left[\\Upsilon(2S) \\to \\gamma \\eta_b(1S)\\right] = \\left(6.1^{+0.6}_{-0.7}{}^{+0.9}_{-0.6}\\right) \\times 10^{-4}\\)<\/span><script type='math\/tex'>B\\left[\\Upsilon(2S) \\to \\gamma \\eta_b(1S)\\right] = \\left(6.1^{+0.6}_{-0.7}{}^{+0.9}_{-0.6}\\right) \\times 10^{-4}<\/script> and derive an <span class='MathJax_Preview'>\\(\\eta_b(1S)\\)<\/span><script type='math\/tex'>\\eta_b(1S)<\/script> mass of <span class='MathJax_Preview'>\\(9394.8^{+2.7}_{-3.1}{}^{+4.5}_{-2.7}\\)<\/span><script type='math\/tex'>9394.8^{+2.7}_{-3.1}{}^{+4.5}_{-2.7}<\/script>&nbsp;MeV<span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script>, where the uncertainties are statistical and systematic, respectively. The significance of our measurement is greater than 7 standard deviations, constituting the first observation of this decay mode.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Studies of <span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0<\/script> and <span class='MathJax_Preview'>\\(B_{s1}(5830)^0\\)<\/span><script type='math\/tex'>B_{s1}(5830)^0<\/script> mesons including the observation of the <span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0 \\to B^0 K_S^0\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0 \\to B^0 K_S^0<\/script> decay in proton-proton collisions at <span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> = 8&nbsp;TeV<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.M.&nbsp;Sirunyan, ... , R.&nbsp;Chistov, M.&nbsp;Danilov, P.&nbsp;Parygin, D.&nbsp;Philippov et al. (CMS Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">European Physical Journal C 78 (2018) 939<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1140\/epjc\/s10052-018-6390-z\" target=\"_blank\">10.1140\/epjc\/s10052-018-6390-z<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1949'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1949\" style=\"display: none;\">Measurements of <span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0<\/script> and <span class='MathJax_Preview'>\\(B_{s1}(5830)^0\\)<\/span><script type='math\/tex'>B_{s1}(5830)^0<\/script> mesons are performed using a data sample of proton-proton collisions corresponding to an integrated luminosity of 19.6&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>, collected with the CMS detector at the LHC at a centre-of-mass energy of 8&nbsp;TeV. The analysis studies <span class='MathJax_Preview'>\\(P\\)<\/span><script type='math\/tex'>P<\/script>-wave <span class='MathJax_Preview'>\\(B_s^0\\)<\/span><script type='math\/tex'>B_s^0<\/script> meson decays into <span class='MathJax_Preview'>\\(B^{(*)+} K^-\\)<\/span><script type='math\/tex'>B^{(*)+} K^-<\/script> and <span class='MathJax_Preview'>\\(B^{(*)0} K_S^0\\)<\/span><script type='math\/tex'>B^{(*)0} K_S^0<\/script>, where the <span class='MathJax_Preview'>\\(B^+\\)<\/span><script type='math\/tex'>B^+<\/script> and <span class='MathJax_Preview'>\\(B^0\\)<\/span><script type='math\/tex'>B^0<\/script> mesons are identified using the decays <span class='MathJax_Preview'>\\(B^+ \\to J\/\\psi K^+\\)<\/span><script type='math\/tex'>B^+ \\to J\/\\psi K^+<\/script> and <span class='MathJax_Preview'>\\(B^0 \\to J\/\\psi K^*(892)^0\\)<\/span><script type='math\/tex'>B^0 \\to J\/\\psi K^*(892)^0<\/script>. The masses of the <span class='MathJax_Preview'>\\(P\\)<\/span><script type='math\/tex'>P<\/script>-wave <span class='MathJax_Preview'>\\(B_s^0\\)<\/span><script type='math\/tex'>B_s^0<\/script> meson states are measured and the natural width of the <span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0<\/script> state is determined. The first measurement of the mass difference between the charged and neutral <span class='MathJax_Preview'>\\(B^*\\)<\/span><script type='math\/tex'>B^*<\/script> mesons is also presented. The <span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0<\/script> decay to <span class='MathJax_Preview'>\\(B^0 K_S^0\\)<\/span><script type='math\/tex'>B^0 K_S^0<\/script> is observed, together with a measurement of its branching fraction relative to the <span class='MathJax_Preview'>\\(B_{s2}^*(5840)^0 \\to B^+ K^-\\)<\/span><script type='math\/tex'>B_{s2}^*(5840)^0 \\to B^+ K^-<\/script> decay.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<p><!--\t        \n\n<li style=\"line-height: 1.4;\">\n\n<div class=\"single-publication\">\n\t\n\n<div class=\"publication_title\">[TRANSLATION] Study of the Response Uniformity of Scintillator Tiles for Highly Granular Calorimeters<\/div>\n\n\n\t\t\n\n<div class=\"publication_authors\"><span class=\"author-list\"><i>S.S.&nbsp;Korpachev and M.V.&nbsp;Chadeeva<\/i><\/span><\/div>\n\n\n\t\t\n\n<div class=\"publication_download\" align=\"justify\">Bulletin of the Lebedev Physics Institute 45 (2018) \u2116&nbsp;10, 322\u2013324\n<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.3103\/S1068335618100093\" target=\"_blank\">10.3103\/S1068335618100093<\/a><span class=\"title\"> <\/span><\/div>\n\n\t\t\n\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2152'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2152\" style=\"display: none;\">A modern trend in calorimetry is an increase in calorimeter granularity. A high-granularity hadron calorimeter assembled from scintillator tiles with signal readout by silicon photomultipliers is developed and tested by the CALICE collaboration. The uniformity of the tile response to minimum ionizing particles is studied, and these experimental measurements are compared with simulation based on the Geant4 package.<\/span><\/div>\n\n\n\t<\/div>\n\n<\/li>\n\n --><\/p>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">\u0418\u0437\u0443\u0447\u0435\u043d\u0438\u0435 \u043e\u0434\u043d\u043e\u0440\u043e\u0434\u043d\u043e\u0441\u0442\u0438 \u043e\u0442\u043a\u043b\u0438\u043a\u0430 \u0441\u0446\u0438\u043d\u0442\u0438\u043b\u043b\u044f\u0446\u0438\u043e\u043d\u043d\u044b\u0445 \u0442\u0430\u0439\u043b\u043e\u0432 \u0434\u043b\u044f \u0432\u044b\u0441\u043e\u043a\u043e\u0433\u0440\u0430\u043d\u0443\u043b\u044f\u0440\u043d\u044b\u0445 \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u043e\u0432<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>\u0421.\u0421.&nbsp;\u041a\u043e\u0440\u043f\u0430\u0447\u0435\u0432, \u041c.\u0412.&nbsp;\u0427\u0430\u0434\u0435\u0435\u0432\u0430<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">\u041a\u0440\u0430\u0442\u043a\u0438\u0435 \u0441\u043e\u043e\u0431\u0449\u0435\u043d\u0438\u044f \u043f\u043e \u0444\u0438\u0437\u0438\u043a\u0435 \u0424\u0418\u0410\u041d 45 (2018), \u2116&nbsp;10, \u0441.&nbsp;52\u201356<span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1892'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1892\" style=\"display: none;\">\u0421\u043e\u0432\u0440\u0435\u043c\u0435\u043d\u043d\u043e\u0439 \u0442\u0435\u043d\u0434\u0435\u043d\u0446\u0438\u0435\u0439 \u0432 \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u0438\u0438 \u044f\u0432\u043b\u044f\u0435\u0442\u0441\u044f \u043f\u043e\u0432\u044b\u0448\u0435\u043d\u0438\u0435 \u0433\u0440\u0430\u043d\u0443\u043b\u044f\u0440\u043d\u043e\u0441\u0442\u0438 \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440\u043e\u0432. \u0412\u044b\u0441\u043e\u043a\u043e\u0433\u0440\u0430\u043d\u0443\u043b\u044f\u0440\u043d\u044b\u0439 \u0430\u0434\u0440\u043e\u043d\u043d\u044b\u0439 \u043a\u0430\u043b\u043e\u0440\u0438\u043c\u0435\u0442\u0440, \u0441\u043e\u0431\u0440\u0430\u043d\u043d\u044b\u0439 \u0438\u0437 \u0441\u0446\u0438\u043d\u0442\u0438\u043b\u043b\u044f\u0446\u0438\u043e\u043d\u043d\u044b\u0445 \u0442\u0430\u0439\u043b\u043e\u0432 (\u044f\u0447\u0435\u0435\u043a) \u0441\u043e \u0441\u0447\u0438\u0442\u044b\u0432\u0430\u043d\u0438\u0435\u043c \u0441\u0438\u0433\u043d\u0430\u043b\u0430 \u043a\u0440\u0435\u043c\u043d\u0438\u0435\u0432\u044b\u043c\u0438 \u0444\u043e\u0442\u043e\u0443\u043c\u043d\u043e\u0436\u0438\u0442\u0435\u043b\u044f\u043c\u0438, \u0440\u0430\u0437\u0440\u0430\u0431\u043e\u0442\u0430\u043d \u0438 \u0442\u0435\u0441\u0442\u0438\u0440\u0443\u0435\u0442\u0441\u044f \u043a\u043e\u043b\u043b\u0430\u0431\u043e\u0440\u0430\u0446\u0438\u0435\u0439 CALICE. \u0412 \u0440\u0430\u0431\u043e\u0442\u0435 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u043e \u0438\u0441\u0441\u043b\u0435\u0434\u043e\u0432\u0430\u043d\u0438\u0435 \u043e\u0434\u043d\u043e\u0440\u043e\u0434\u043d\u043e\u0441\u0442\u0438 \u043e\u0442\u043a\u043b\u0438\u043a\u0430 \u0442\u0430\u0439\u043b\u0430 \u043d\u0430 \u043c\u0438\u043d\u0438\u043c\u0430\u043b\u044c\u043d\u043e \u0438\u043e\u043d\u0438\u0437\u0438\u0440\u0443\u044e\u0449\u0438\u0435 \u0447\u0430\u0441\u0442\u0438\u0446\u044b, \u0430 \u0442\u0430\u043a\u0436\u0435 \u0441\u0440\u0430\u0432\u043d\u0435\u043d\u0438\u0435 \u044d\u0442\u0438\u0445 \u044d\u043a\u0441\u00ad\u043f\u0435\u0440\u0438\u043c\u0435\u043d\u0442\u0430\u043b\u044c\u043d\u044b\u0445 \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u0439 \u0441 \u043c\u043e\u0434\u0435\u043b\u0438\u0440\u043e\u0432\u0430\u043d\u0438\u0435\u043c \u043d\u0430 \u043e\u0441\u043d\u043e\u0432\u0435 \u043f\u0430\u043a\u0435\u0442\u0430 Geant4.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Recent developments in charmed baryon spectroscopy<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>E.&nbsp;Solovieva<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">EPJ Web of Conferences 191 (2018) 02013<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1051\/epjconf\/201819102013\" target=\"_blank\">10.1051\/epjconf\/201819102013<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1887'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1887\" style=\"display: none;\">An overview of recent developments in charmed baryon spectroscopy is given. The classification of charmed baryons is presented, a quark model for ground states is briefly described, and the energy levels of excited<br \/>\nstates are analyzed.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">The Belle&nbsp;II experiment: status and physics program<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>D.&nbsp;Matvienko<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">EPJ Web of Conferences 191 (2018) 02010<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1051\/epjconf\/201819102010\" target=\"_blank\">10.1051\/epjconf\/201819102010<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('2025'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"2025\" style=\"display: none;\">The Belle&nbsp;II experiment at the SuperKEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> collider in Japan aims to search for new physics in the flavour transitions in the quark and lepton sectors. The SuperKEKB accelerator will operate at the target instantaneous luminosity of <span class='MathJax_Preview'>\\(8 \\times 10^{35}\\)<\/span><script type='math\/tex'>8 \\times 10^{35}<\/script>&nbsp;s<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script>cm<span class='MathJax_Preview'>\\(^2\\)<\/span><script type='math\/tex'>^2<\/script>. It requires a substantial upgrade of the detector subsystems which are expected to record 50&nbsp;ab<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script> of data. Such a huge data sample in clean background environment allows for probing signatures of new physics through suppressed flavour physics reactions and cross checks for deviations from the Standard Model measured at the LHCb experiment. Physics data taking at the Belle&nbsp;II experiment successfully started in April 2018.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Measurement of <span class='MathJax_Preview'>\\(\\eta_c(1S)\\)<\/span><script type='math\/tex'>\\eta_c(1S)<\/script>, <span class='MathJax_Preview'>\\(\\eta_c(2S)\\)<\/span><script type='math\/tex'>\\eta_c(2S)<\/script>, and nonresonant <span class='MathJax_Preview'>\\(\\eta^\\prime \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\eta^\\prime \\pi^+ \\pi^-<\/script> production via two-photon collisions<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>Q.N.&nbsp;Xu, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, P.&nbsp;Pakhlov, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Vorobyev, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review D 98 (2018) 072001<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1103\/PhysRevD.98.072001\" target=\"_blank\">10.1103\/PhysRevD.98.072001<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1972'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1972\" style=\"display: none;\">We report the measurement of <span class='MathJax_Preview'>\\(\\gamma \\gamma \\to \\eta_c(1S), \\eta_c(2S) \\to \\eta^\\prime \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\gamma \\gamma \\to \\eta_c(1S), \\eta_c(2S) \\to \\eta^\\prime \\pi^+ \\pi^-<\/script> with <span class='MathJax_Preview'>\\(\\eta^\\prime\\)<\/span><script type='math\/tex'>\\eta^\\prime<\/script> decays to <span class='MathJax_Preview'>\\(\\gamma \\rho\\)<\/span><script type='math\/tex'>\\gamma \\rho<\/script> and <span class='MathJax_Preview'>\\(\\eta \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\eta \\pi^+ \\pi^-<\/script> using 941&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script> of data collected with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> collider. The <span class='MathJax_Preview'>\\(\\eta_c(1S)\\)<\/span><script type='math\/tex'>\\eta_c(1S)<\/script> mass and width are measured to be <span class='MathJax_Preview'>\\(M = \\left[2984.6 \\pm 0.7\\right.\\)<\/span><script type='math\/tex'>M = \\left[2984.6 \\pm 0.7\\right.<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;2.2\\)<\/span><script type='math\/tex'>\\pm\\;2.2<\/script>&nbsp;(syst) <span class='MathJax_Preview'>\\(\\pm\\;0.3\\)<\/span><script type='math\/tex'>\\pm\\;0.3<\/script>&nbsp;(model)<span class='MathJax_Preview'>\\(\\left.\\right]\\)<\/span><script type='math\/tex'>\\left.\\right]<\/script>&nbsp;MeV<span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script> and <span class='MathJax_Preview'>\\(\\Gamma = 30.8^{+2.3}_{-2.2}\\)<\/span><script type='math\/tex'>\\Gamma = 30.8^{+2.3}_{-2.2}<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;2.5\\)<\/span><script type='math\/tex'>\\pm\\;2.5<\/script>&nbsp;(syst) <span class='MathJax_Preview'>\\(\\pm\\;1.4\\)<\/span><script type='math\/tex'>\\pm\\;1.4<\/script>&nbsp;(model)&nbsp;MeV, respectively. First observation of <span class='MathJax_Preview'>\\(\\eta_c(2S) \\to \\eta^\\prime \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\eta_c(2S) \\to \\eta^\\prime \\pi^+ \\pi^-<\/script> with a significance of <span class='MathJax_Preview'>\\(5.5\\sigma\\)<\/span><script type='math\/tex'>5.5\\sigma<\/script> including systematic error is obtained, and the <span class='MathJax_Preview'>\\(\\eta_c(2S)\\)<\/span><script type='math\/tex'>\\eta_c(2S)<\/script> mass is measured to be <span class='MathJax_Preview'>\\(M = \\left[3635.1 \\pm 3.7\\right.\\)<\/span><script type='math\/tex'>M = \\left[3635.1 \\pm 3.7\\right.<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;2.9\\)<\/span><script type='math\/tex'>\\pm\\;2.9<\/script>&nbsp;(syst) <span class='MathJax_Preview'>\\(\\pm\\;0.4\\)<\/span><script type='math\/tex'>\\pm\\;0.4<\/script>&nbsp;(model)<span class='MathJax_Preview'>\\(\\left.\\right]\\)<\/span><script type='math\/tex'>\\left.\\right]<\/script>&nbsp;MeV<span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script>. The products of the two-photon decay width and branching fraction <span class='MathJax_Preview'>\\(\\left({\\cal B}\\right)\\)<\/span><script type='math\/tex'>\\left({\\cal B}\\right)<\/script> of decays to <span class='MathJax_Preview'>\\(\\eta^\\prime \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\eta^\\prime \\pi^+ \\pi^-<\/script> are determined to be <span class='MathJax_Preview'>\\(\\Gamma_{\\gamma \\gamma} \\Gamma_{\\gamma \\gamma} {\\cal B} = \\left[65.4 \\pm 2.6\\right.\\)<\/span><script type='math\/tex'>\\Gamma_{\\gamma \\gamma} \\Gamma_{\\gamma \\gamma} {\\cal B} = \\left[65.4 \\pm 2.6\\right.<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;7.8\\)<\/span><script type='math\/tex'>\\pm\\;7.8<\/script>&nbsp;(syst)<span class='MathJax_Preview'>\\(\\left.\\right]\\)<\/span><script type='math\/tex'>\\left.\\right]<\/script>&nbsp;eV for <span class='MathJax_Preview'>\\(\\eta_c(1S)\\)<\/span><script type='math\/tex'>\\eta_c(1S)<\/script> and <span class='MathJax_Preview'>\\(\\left[5.6^{+1.2}_{-1.1}\\right.\\)<\/span><script type='math\/tex'>\\left[5.6^{+1.2}_{-1.1}\\right.<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;1.1\\)<\/span><script type='math\/tex'>\\pm\\;1.1<\/script>&nbsp;(syst)<span class='MathJax_Preview'>\\(\\big]\\)<\/span><script type='math\/tex'>\\big]<\/script>&nbsp;eV for <span class='MathJax_Preview'>\\(\\eta_c(2S)\\)<\/span><script type='math\/tex'>\\eta_c(2S)<\/script>. The cross sections for <span class='MathJax_Preview'>\\(\\gamma \\gamma \\to \\eta^\\prime \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>\\gamma \\gamma \\to \\eta^\\prime \\pi^+ \\pi^-<\/script> and <span class='MathJax_Preview'>\\(\\eta^\\prime f_2(1270)\\)<\/span><script type='math\/tex'>\\eta^\\prime f_2(1270)<\/script> are measured for the first time.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Inclusive study of bottomonium production in association with an <span class='MathJax_Preview'>\\(\\eta\\)<\/span><script type='math\/tex'>\\eta<\/script> meson in <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> annihilations near <span class='MathJax_Preview'>\\(\\Upsilon(5S)\\)<\/span><script type='math\/tex'>\\Upsilon(5S)<\/script><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>U.&nbsp;Tamponi, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, P.&nbsp;Pakhlov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Vorobyev, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">European Physical Journal C 78 (2018) 633<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1140\/epjc\/s10052-018-6086-4\" target=\"_blank\">10.1140\/epjc\/s10052-018-6086-4<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1574'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1574\" style=\"display: none;\">We study bottomonium production in association with an <span class='MathJax_Preview'>\\(\\eta\\)<\/span><script type='math\/tex'>\\eta<\/script> meson in <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> annihilations near the <span class='MathJax_Preview'>\\(\\Upsilon(5S)\\)<\/span><script type='math\/tex'>\\Upsilon(5S)<\/script>,at a centre-of-mass energy of <span class='MathJax_Preview'>\\(\\sqrt{s}\\)<\/span><script type='math\/tex'>\\sqrt{s}<\/script> = 10.866&nbsp;GeV. The results are based on the 121.4&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script> data sample collected by the Belle experiment at the asymmetric-energy KEKB collider. Only the <span class='MathJax_Preview'>\\(\\eta\\)<\/span><script type='math\/tex'>\\eta<\/script> meson is reconstructed and the missing-mass spectrum of <span class='MathJax_Preview'>\\(\\eta\\)<\/span><script type='math\/tex'>\\eta<\/script> candidates is investigated. We observe the <span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\Upsilon_J(1D)\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\Upsilon_J(1D)<\/script> process and find evidence for the <span class='MathJax_Preview'>\\(e^+e^- \\to \\eta \\Upsilon(2S)\\)<\/span><script type='math\/tex'>e^+e^- \\to \\eta \\Upsilon(2S)<\/script> process, while no significant signals of <span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script>, <span class='MathJax_Preview'>\\(h_b(1P)\\)<\/span><script type='math\/tex'>h_b(1P)<\/script>, nor <span class='MathJax_Preview'>\\(h_b(2P)\\)<\/span><script type='math\/tex'>h_b(2P)<\/script> are found. Cross sections for the studied processes are reported.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Observation of <span class='MathJax_Preview'>\\(\\Upsilon(4S) \\to \\eta^\\prime \\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S) \\to \\eta^\\prime \\Upsilon(1S)<\/script><\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>E.&nbsp;Guido, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, V.&nbsp;Popov, T.&nbsp;Uglov, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 121 (2018) 062001<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1103\/PhysRevLett.121.062001\" target=\"_blank\">10.1103\/PhysRevLett.121.062001<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1588'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1588\" style=\"display: none;\">We report the first observation of the hadronic transition <span class='MathJax_Preview'>\\(\\Upsilon(4S) \\to \\eta^\\prime \\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S) \\to \\eta^\\prime \\Upsilon(1S)<\/script>, using 496&nbsp;fb<span class='MathJax_Preview'>\\(^{-1}\\)<\/span><script type='math\/tex'>^{-1}<\/script> data collected at the <span class='MathJax_Preview'>\\(\\Upsilon(4S)\\)<\/span><script type='math\/tex'>\\Upsilon(4S)<\/script> resonance with the Belle detector at the KEKB asymmetric-energy <span class='MathJax_Preview'>\\(e^+e^-\\)<\/span><script type='math\/tex'>e^+e^-<\/script> collider. We reconstruct the <span class='MathJax_Preview'>\\(\\eta^\\prime\\)<\/span><script type='math\/tex'>\\eta^\\prime<\/script> meson through its decays to <span class='MathJax_Preview'>\\(\\rho^0 \\gamma\\)<\/span><script type='math\/tex'>\\rho^0 \\gamma<\/script> and to <span class='MathJax_Preview'>\\(\\pi^+ \\pi^- \\eta\\)<\/span><script type='math\/tex'>\\pi^+ \\pi^- \\eta<\/script>, with <span class='MathJax_Preview'>\\(\\eta \\to \\gamma \\gamma\\)<\/span><script type='math\/tex'>\\eta \\to \\gamma \\gamma<\/script>. We measure <span class='MathJax_Preview'>\\({\\cal B}(\\Upsilon(4S) \\to \\eta^\\prime \\Upsilon(1S)) = [3.43 \\pm 0.88\\)<\/span><script type='math\/tex'>{\\cal B}(\\Upsilon(4S) \\to \\eta^\\prime \\Upsilon(1S)) = [3.43 \\pm 0.88<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm\\;0.21\\)<\/span><script type='math\/tex'>\\pm\\;0.21<\/script>&nbsp;(syst)<span class='MathJax_Preview'>\\(] \\times 10^{-5}\\)<\/span><script type='math\/tex'>] \\times 10^{-5}<\/script>, with a significance of <span class='MathJax_Preview'>\\(5.7\\sigma\\)<\/span><script type='math\/tex'>5.7\\sigma<\/script>.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">Observation of an Excited <span class='MathJax_Preview'>\\(\\Omega^-\\)<\/span><script type='math\/tex'>\\Omega^-<\/script> Baryon<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>J.&nbsp;Yelton, ... , K.&nbsp;Chilikin, S.&nbsp;Eidelman, D.&nbsp;Matvienko, R.&nbsp;Mizuk, P.&nbsp;Pakhlov, V.&nbsp;Popov, E.&nbsp;Solovieva, T.&nbsp;Uglov, V.&nbsp;Vorobyev, V.&nbsp;Zhukova et al. (Belle Collaboration)<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Physical Review Letters 121 (2018) 052003<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1103\/PhysRevLett.121.052003\" target=\"_blank\">10.1103\/PhysRevLett.121.052003<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1760'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1760\" style=\"display: none;\">Using data recorded with the Belle detector, we observe a new excited hyperon, an <span class='MathJax_Preview'>\\(\\Omega^{*-}\\)<\/span><script type='math\/tex'>\\Omega^{*-}<\/script> candidate decaying into <span class='MathJax_Preview'>\\(\\Xi^0 K^-\\)<\/span><script type='math\/tex'>\\Xi^0 K^-<\/script> and <span class='MathJax_Preview'>\\(\\Xi^- K_S^0\\)<\/span><script type='math\/tex'>\\Xi^- K_S^0<\/script> with a mass of <span class='MathJax_Preview'>\\(2012.4 \\pm 0.7\\)<\/span><script type='math\/tex'>2012.4 \\pm 0.7<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm 0.6\\)<\/span><script type='math\/tex'>\\pm 0.6<\/script>&nbsp;(syst)&nbsp;MeV<span class='MathJax_Preview'>\\(\/c^2\\)<\/span><script type='math\/tex'>\/c^2<\/script> and a width of <span class='MathJax_Preview'>\\(\\Gamma = 6.4^{+2.5}_{-2.0}\\)<\/span><script type='math\/tex'>\\Gamma = 6.4^{+2.5}_{-2.0}<\/script>&nbsp;(stat) <span class='MathJax_Preview'>\\(\\pm 1.6\\)<\/span><script type='math\/tex'>\\pm 1.6<\/script>&nbsp;(syst)&nbsp;MeV. The <span class='MathJax_Preview'>\\(\\Omega^{*-}\\)<\/span><script type='math\/tex'>\\Omega^{*-}<\/script> is seen primarily in <span class='MathJax_Preview'>\\(\\Upsilon(1S)\\)<\/span><script type='math\/tex'>\\Upsilon(1S)<\/script>, <span class='MathJax_Preview'>\\(\\Upsilon(2S)\\)<\/span><script type='math\/tex'>\\Upsilon(2S)<\/script>, and <span class='MathJax_Preview'>\\(\\Upsilon(3S)\\)<\/span><script type='math\/tex'>\\Upsilon(3S)<\/script> decays.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<p><!--\t        \n\n<li style=\"line-height: 1.4;\">\n\n<div class=\"single-publication\">\n\t\n\n<div class=\"publication_title\">[TRANSLATION] Anomalous magnetic moment of the muon<\/div>\n\n\n\t\t\n\n<div class=\"publication_authors\"><span class=\"author-list\"><i>I.B.&nbsp;Logashenko, S.I.&nbsp;Eidelman<\/i><\/span><\/div>\n\n\n\t\t\n\n<div class=\"publication_download\" align=\"justify\">Physics&hairsp;&ndash;&hairsp;Uspekhi 61 (2018) \u2116&nbsp;5, 480\u2013510<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.3367\/UFNe.2018.02.038312\" target=\"_blank\">10.3367\/UFNe.2018.02.038312<\/a><span class=\"title\"> <\/span><\/div>\n\n\t\t\n\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1885'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1885\" style=\"display: none;\">The anomalous magnetic moment of the muon, <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script>, is a unique quantity that allows high-precision tests of the Standard Model. Currently, a difference of 3 to 4 standard deviations is observed between the prediction of the Standard Model and the most precise measurement performed. We present a review of the Standard Model calculations of <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script>. The principles and history of <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script> experiments are presented, and the recent measurement at the Brookhaven National Laboratory, USA, is described in detail. Prospects for further improving the accuracy of both calculations and measurements of <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script> are discussed.<\/span><\/div>\n\n\n\t<\/div>\n\n<\/li>\n\n --><\/p>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">\u0410\u043d\u043e\u043c\u0430\u043b\u044c\u043d\u044b\u0439 \u043c\u0430\u0433\u043d\u0438\u0442\u043d\u044b\u0439 \u043c\u043e\u043c\u0435\u043d\u0442 \u043c\u044e\u043e\u043d\u0430<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>\u0418.\u0411.&nbsp;\u041b\u043e\u0433\u0430\u0448\u0435\u043d\u043a\u043e, \u0421.\u0418.&nbsp;\u042d\u0439\u0434\u0435\u043b\u044c\u043c\u0430\u043d<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">\u0423\u0441\u043f\u0435\u0445\u0438 \u0444\u0438\u0437\u0438\u0447\u0435\u0441\u043a\u0438\u0445 \u043d\u0430\u0443\u043a 188 (2018), \u2116&nbsp;5, \u0441.&nbsp;540\u2013573<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.3367\/UFNr.2018.02.038312\" target=\"_blank\">10.3367\/UFNr.2018.02.038312<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1867'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1867\" style=\"display: none;\">\u0410\u043d\u043e\u043c\u0430\u043b\u044c\u043d\u044b\u0439 \u043c\u0430\u0433\u043d\u0438\u0442\u043d\u044b\u0439 \u043c\u043e\u043c\u0435\u043d\u0442 \u043c\u044e\u043e\u043d\u0430 <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script> \u044f\u0432\u043b\u044f\u0435\u0442\u0441\u044f \u0443\u043d\u0438\u043a\u0430\u043b\u044c\u043d\u044b\u043c \u043e\u0431\u044a\u0435\u043a\u0442\u043e\u043c, \u043f\u043e\u0437\u0432\u043e\u043b\u044f\u044e\u0449\u0438\u043c \u0441 \u043e\u0447\u0435\u043d\u044c \u0432\u044b\u0441\u043e\u043a\u043e\u0439 \u0442\u043e\u0447\u043d\u043e\u0441\u0442\u044c\u044e \u043f\u0440\u043e\u0432\u0435\u0440\u0438\u0442\u044c \u0421\u0442\u0430\u043d\u0434\u0430\u0440\u0442\u043d\u0443\u044e \u043c\u043e\u0434\u0435\u043b\u044c. \u041d\u0430 \u0441\u0435\u0433\u043e\u0434\u043d\u044f\u0448\u043d\u0438\u0439 \u0434\u0435\u043d\u044c \u043d\u0430\u0431\u043b\u044e\u0434\u0430\u0435\u0442\u0441\u044f \u043e\u0442\u043b\u0438\u0447\u0438\u0435 \u0432 3&ndash;4 \u0441\u0442\u0430\u043d\u0434\u0430\u0440\u0442\u043d\u044b\u0445 \u043e\u0442\u043a\u043b\u043e\u043d\u0435\u043d\u0438\u044f \u043c\u0435\u0436\u0434\u0443 \u043f\u0440\u0435\u0434\u0441\u043a\u0430\u0437\u0430\u043d\u0438\u0435\u043c \u0421\u0442\u0430\u043d\u0434\u0430\u0440\u0442\u043d\u043e\u0439 \u043c\u043e\u0434\u0435\u043b\u0438 \u0438 \u043d\u0430\u0438\u0431\u043e\u043b\u0435\u0435 \u0442\u043e\u0447\u043d\u044b\u043c \u0440\u0435\u0437\u0443\u043b\u044c\u0442\u0430\u0442\u043e\u043c \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u044f. \u041f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d \u043e\u0431\u0437\u043e\u0440 \u0441\u043e\u0432\u0440\u0435\u043c\u0435\u043d\u043d\u043e\u0433\u043e \u0441\u043e\u0441\u0442\u043e\u044f\u043d\u0438\u044f \u0434\u0435\u043b \u043f\u043e \u0432\u044b\u0447\u0438\u0441\u043b\u0435\u043d\u0438\u044e <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script> \u0432 \u0440\u0430\u043c\u043a\u0430\u0445 \u0421\u0442\u0430\u043d\u0434\u0430\u0440\u0442\u043d\u043e\u0439 \u043c\u043e\u0434\u0435\u043b\u0438. \u041f\u0440\u0438\u0432\u0435\u0434\u0435\u043d\u044b \u043f\u0440\u0438\u043d\u0446\u0438\u043f\u044b \u0438 \u0438\u0441\u0442\u043e\u0440\u0438\u044f \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u0439 <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script>, \u043f\u043e\u0434\u0440\u043e\u0431\u043d\u043e \u043e\u043f\u0438\u0441\u0430\u043d\u043e \u043d\u0430\u0438\u0431\u043e\u043b\u0435\u0435 \u0442\u043e\u0447\u043d\u043e\u0435 \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u0435, \u043f\u0440\u043e\u0432\u0435\u0434\u0451\u043d\u043d\u043e\u0435 \u0432 \u0411\u0440\u0443\u043a\u0445\u0435\u0439\u0432\u0435\u043d\u0441\u043a\u043e\u0439 \u043d\u0430\u0446\u0438\u043e\u043d\u0430\u043b\u044c\u043d\u043e\u0439 \u043b\u0430\u0431\u043e\u0440\u0430\u0442\u043e\u0440\u0438\u0438 (\u0421\u0428\u0410). \u041e\u0431\u0441\u0443\u0436\u0434\u0430\u044e\u0442\u0441\u044f \u043f\u0435\u0440\u0441\u043f\u0435\u043a\u0442\u0438\u0432\u044b \u0434\u0430\u043b\u044c\u043d\u0435\u0439\u0448\u0435\u0433\u043e \u0443\u043b\u0443\u0447\u0448\u0435\u043d\u0438\u044f \u0442\u043e\u0447\u043d\u043e\u0441\u0442\u0438 \u043a\u0430\u043a \u0440\u0430\u0441\u0447\u0451\u0442\u043e\u0432, \u0442\u0430\u043a \u0438 \u0438\u0437\u043c\u0435\u0440\u0435\u043d\u0438\u0439 <span class='MathJax_Preview'>\\(a_\\mu\\)<\/span><script type='math\/tex'>a_\\mu<\/script>.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<li style=\"line-height: 1.4;\">\n<div class=\"single-publication\">\n<div class=\"publication_title\">A method for model-independent measurement of the CKM angle <span class='MathJax_Preview'>\\(\\beta\\)<\/span><script type='math\/tex'>\\beta<\/script> via time-dependent analysis of the <span class='MathJax_Preview'>\\(B^0 \\to D \\pi^+\\pi^-\\)<\/span><script type='math\/tex'>B^0 \\to D \\pi^+\\pi^-<\/script>, <span class='MathJax_Preview'>\\(D \\to K_S^0 \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>D \\to K_S^0 \\pi^+ \\pi^-<\/script> decays<\/div>\n<div class=\"publication_authors\"><span class=\"author-list\"><i>A.&nbsp;Bondar, A.&nbsp;Kuzmin and V.&nbsp;Vorobyev<\/i><\/span><\/div>\n<div class=\"publication_download\" align=\"justify\">Journal of High Energy Physics 1803 (2018) 195<br \/>DOI: <a href=\"https:\/\/dx.doi.org\/10.1007\/JHEP03(2018)195\" target=\"_blank\">10.1007\/JHEP03(2018)195<\/a><span class=\"title\"> <\/span><\/div>\n<div class=\"publication_summary\" align=\"justify\"><span class=\"title\">\u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: <\/span><span class=\"description\" onclick=\"javascript: {style.display = 'none'; var div = document.getElementById('1643'); div.style.display = '';}\"> ... \u043a\u043b\u0438\u043a\u043d\u0438\u0442\u0435, \u0447\u0442\u043e\u0431\u044b \u043f\u0440\u043e\u0447\u0438\u0442\u0430\u0442\u044c ...<\/span><span class=\"description\" id=\"1643\" style=\"display: none;\">A new method for model-independent measurement of the CKM angle <span class='MathJax_Preview'>\\(\\beta\\)<\/span><script type='math\/tex'>\\beta<\/script> is proposed, that employs time-dependent analysis of flavour-tagged <span class='MathJax_Preview'>\\(B^0 \\to D \\pi^+\\pi^-\\)<\/span><script type='math\/tex'>B^0 \\to D \\pi^+\\pi^-<\/script> decays with <span class='MathJax_Preview'>\\(D\\)<\/span><script type='math\/tex'>D<\/script> meson decays into <span class='MathJax_Preview'>\\(\\cal{CP}\\)<\/span><script type='math\/tex'>\\cal{CP}<\/script>-specific and <span class='MathJax_Preview'>\\(K_S^0 \\pi^+ \\pi^-\\)<\/span><script type='math\/tex'>K_S^0 \\pi^+ \\pi^-<\/script> final states. This method can be used to measure the angle <span class='MathJax_Preview'>\\(\\beta\\)<\/span><script type='math\/tex'>\\beta<\/script> with future data from the BelleII and LHCb experiments with the precision level of one degree.<\/span><\/div>\n<\/p><\/div>\n<\/li>\n<\/ol>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>2020 \u0433\u043e\u0434 Measurements of production cross sections of \\(W Z\\) and same-sign \\(W W\\) boson pairs in association with two jets in proton-proton collisions at \\(\\sqrt{s}\\) = 13&nbsp;TeV CMS Collaboration Physics Letters B 809 (2020) 135710DOI: 10.1016\/j.physletb.2020.135710 \u041a\u0440\u0430\u0442\u043a\u043e\u0435 \u0441\u043e\u0434\u0435\u0440\u0436\u0430\u043d\u0438\u0435: &#8230; <a href=\"https:\/\/belle.lebedev.ru\/bsm\/publications\/\" class=\"read-more\">\u0427\u0438\u0442\u0430\u0442\u044c \u0434\u0430\u043b\u044c\u0448\u0435 &#8230;<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"_links":{"self":[{"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/pages\/2"}],"collection":[{"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/comments?post=2"}],"version-history":[{"count":99,"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/pages\/2\/revisions"}],"predecessor-version":[{"id":765,"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/pages\/2\/revisions\/765"}],"wp:attachment":[{"href":"https:\/\/belle.lebedev.ru\/bsm\/wp-json\/wp\/v2\/media?parent=2"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}