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Phys."],"abstract":"Abstract<\/jats:sc>\n <\/jats:title>\n The production cross sections of \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> and B+<\/jats:sup> mesons are reported in proton-proton (pp) collisions recorded by the CMS experiment at the CERN LHC with a center-of-mass energy of 5.02 TeV. The data sample corresponds to an integrated luminosity of 302 pb\n \u2212<\/jats:italic>1<\/jats:sup>. The cross sections are based on measurements of the \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n \u2192<\/jats:italic> J\/\u03c8<\/jats:italic>(\u03bc<\/jats:italic>\n +<\/jats:sup>\n \u03bc<\/jats:italic>\n \n \u2212<\/jats:italic>\n <\/jats:sup>)\u03d5<\/jats:italic>(1020)(K+<\/jats:sup>K\n \u2212<\/jats:italic>\n <\/jats:sup>) and B+<\/jats:sup>\n \u2192<\/jats:italic> J\/\u03c8<\/jats:italic>(\u03bc<\/jats:italic>\n +<\/jats:sup>\n \u03bc<\/jats:italic>\n \n \u2212<\/jats:italic>\n <\/jats:sup>)K+<\/jats:sup> decay channels. Results are presented in the transverse momentum (p<\/jats:italic>\n T<\/jats:sub>) range 7\u201350 GeV\/c<\/jats:italic> and the rapidity interval |y<\/jats:italic>| <<\/jats:italic> 2.<\/jats:italic>4 for the B mesons. The measured p<\/jats:italic>\n T<\/jats:sub>-differential cross sections of B+<\/jats:sup> and \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> in pp collisions are well described by fixed-order plus next-to-leading logarithm perturbative quantum chromodynamics calculations. Using previous PbPb collision measurements at the same nucleon-nucleon center-of-mass energy, the nuclear modification factors, R<\/jats:italic>\n AA<\/jats:sub>, of the B mesons are determined. For p<\/jats:italic>\n T<\/jats:sub>\n ><\/jats:italic> 10 GeV\/c<\/jats:italic>, both mesons are found to be suppressed in PbPb collisions (with R<\/jats:italic>\n AA<\/jats:sub> values significantly below unity), with less suppression observed for the \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> mesons. In this p<\/jats:italic>\n T<\/jats:sub> range, the R<\/jats:italic>\n AA<\/jats:sub> values for the B+<\/jats:sup> mesons are consistent with those for inclusive charged hadrons and D0<\/jats:sup> mesons. Below 10 GeV\/c<\/jats:italic>, both B+<\/jats:sup> and \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> are found to be less suppressed than either inclusive charged hadrons or D0<\/jats:sup> mesons, with the \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>\n R<\/jats:italic>\n AA<\/jats:sub> value consistent with unity. The R<\/jats:italic>\n AA<\/jats:sub> values found for the B+<\/jats:sup> and \n \n $$ {\\textrm{B}}_{\\textrm{s}}^0 $$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n s<\/mml:mi>\n 0<\/mml:mn>\n <\/mml:msubsup>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> are compared to theoretical calculations, providing constraints on the mechanism of bottom quark energy loss and hadronization in the quark-gluon plasma, the hot and dense matter created in ultrarelativistic heavy ion collisions.<\/jats:p>","DOI":"10.1007\/jhep02(2025)195","type":"journal-article","created":{"date-parts":[[2025,4,4]],"date-time":"2025-04-04T02:40:46Z","timestamp":1743734446000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":1,"title":["Bottom quark energy loss and hadronization with B+ and $$ {\\textrm{B}}_{\\textrm{s}}^0 $$ nuclear modification factors using pp and PbPb collisions at $$ \\sqrt{s_{\\textrm{NN}}} $$ = 5.02 TeV"],"prefix":"10.1007","volume":"2025","author":[{"name":"The CMS collaboration","sequence":"first","affiliation":[]},{"given":"A.","family":"Hayrapetyan","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/00ad27c73","id-type":"ROR","asserted-by":"publisher"}],"name":"Yerevan Physics Institute"}]},{"given":"A.","family":"Tumasyan","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/00ad27c73","id-type":"ROR","asserted-by":"publisher"}],"name":"Yerevan Physics Institute"},{"id":[{"id":"https:\/\/ror.org\/00s8vne50","id-type":"ROR","asserted-by":"publisher"}],"name":"Yerevan State University"}]},{"given":"W.","family":"Adam","sequence":"additional","affiliation":[{"id":[{"id":"https:\/\/ror.org\/039shy520","id-type":"ROR","asserted-by":"publisher"}],"name":"Institut f\u00fcr Hochenergiephysik"}]},{"given":"J. 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