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C"],"abstract":"Abstract<\/jats:title>\n A search for a light charged Higgs boson produced in decays of the top quark, \n \n $$t \\rightarrow H^{\\pm } b$$<\/jats:tex-math>\n \n \n t<\/mml:mi>\n \u2192<\/mml:mo>\n \n H<\/mml:mi>\n \u00b1<\/mml:mo>\n <\/mml:msup>\n b<\/mml:mi>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> with \n \n $$H^{\\pm } \\rightarrow cs$$<\/jats:tex-math>\n \n \n \n H<\/mml:mi>\n \u00b1<\/mml:mo>\n <\/mml:msup>\n \u2192<\/mml:mo>\n c<\/mml:mi>\n s<\/mml:mi>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>, is presented. This search targets the production of top-quark pairs \n \n $$t\\bar{t} \\rightarrow Wb H^{\\pm } b$$<\/jats:tex-math>\n \n \n t<\/mml:mi>\n \n \n t<\/mml:mi>\n <\/mml:mrow>\n \n \u00af<\/mml:mo>\n <\/mml:mrow>\n <\/mml:mover>\n \u2192<\/mml:mo>\n W<\/mml:mi>\n b<\/mml:mi>\n \n H<\/mml:mi>\n \u00b1<\/mml:mo>\n <\/mml:msup>\n b<\/mml:mi>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>, with \n \n $$W \\rightarrow \\ell \\nu $$<\/jats:tex-math>\n \n \n W<\/mml:mi>\n \u2192<\/mml:mo>\n \u2113<\/mml:mi>\n \u03bd<\/mml:mi>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> (\n \n $$\\ell = e, \\mu $$<\/jats:tex-math>\n \n \n \u2113<\/mml:mi>\n =<\/mml:mo>\n e<\/mml:mi>\n ,<\/mml:mo>\n \u03bc<\/mml:mi>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>), resulting in a lepton-plus-jets final state characterised by an isolated electron or muon and at least four jets. The search exploits b<\/jats:italic>-quark and c<\/jats:italic>-quark identification techniques as well as multivariate methods to suppress the dominant \n \n $$t\\bar{t}$$<\/jats:tex-math>\n \n \n t<\/mml:mi>\n \n \n t<\/mml:mi>\n <\/mml:mrow>\n \n \u00af<\/mml:mo>\n <\/mml:mrow>\n <\/mml:mover>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> background. The data analysed correspond to \n \n $$140\\hbox { fb}^{-1}$$<\/jats:tex-math>\n \n \n 140<\/mml:mn>\n \n \n fb<\/mml:mtext>\n \n -<\/mml:mo>\n 1<\/mml:mn>\n <\/mml:mrow>\n <\/mml:msup>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> of \n \n $$pp$$<\/jats:tex-math>\n \n \n pp<\/mml:mi>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> collisions at \n \n $$\\sqrt{s} = 13\\hbox { TeV}$$<\/jats:tex-math>\n \n \n \n s<\/mml:mi>\n <\/mml:msqrt>\n =<\/mml:mo>\n 13<\/mml:mn>\n \n TeV<\/mml:mtext>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula> recorded with the ATLAS detector at the LHC between 2015 and 2018. Observed (expected) 95% confidence-level upper limits on the branching fraction \n \n $$\\mathscr {B}(t\\rightarrow H^{\\pm } b)$$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n (<\/mml:mo>\n t<\/mml:mi>\n \u2192<\/mml:mo>\n \n H<\/mml:mi>\n \u00b1<\/mml:mo>\n <\/mml:msup>\n b<\/mml:mi>\n )<\/mml:mo>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>, assuming \n \n $$\\mathscr {B}(t\\rightarrow Wb) + \\mathscr {B}(t \\rightarrow H^{\\pm } (\\rightarrow cs)b)=1.0$$<\/jats:tex-math>\n \n \n B<\/mml:mi>\n \n (<\/mml:mo>\n t<\/mml:mi>\n \u2192<\/mml:mo>\n W<\/mml:mi>\n b<\/mml:mi>\n )<\/mml:mo>\n <\/mml:mrow>\n +<\/mml:mo>\n B<\/mml:mi>\n (<\/mml:mo>\n t<\/mml:mi>\n \u2192<\/mml:mo>\n \n H<\/mml:mi>\n \u00b1<\/mml:mo>\n <\/mml:msup>\n \n (<\/mml:mo>\n \u2192<\/mml:mo>\n c<\/mml:mi>\n s<\/mml:mi>\n )<\/mml:mo>\n <\/mml:mrow>\n b<\/mml:mi>\n )<\/mml:mo>\n =<\/mml:mo>\n 1.0<\/mml:mn>\n <\/mml:mrow>\n <\/mml:math>\n <\/jats:alternatives>\n <\/jats:inline-formula>, are set between 0.066% (0.077%) and 3.6% (2.3%) for a charged Higgs boson with a mass between 60 and 168 GeV.<\/jats:p>","DOI":"10.1140\/epjc\/s10052-024-13715-4","type":"journal-article","created":{"date-parts":[[2025,2,6]],"date-time":"2025-02-06T13:35:49Z","timestamp":1738848949000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":8,"title":["Search for a light charged Higgs boson in $$t \\rightarrow H^{\\pm } b$$ decays, with $$H^{\\pm } \\rightarrow cs$$, in $$pp$$ collisions at $$\\sqrt{s}={13}\\hbox { TeV}$$ with the ATLAS detector"],"prefix":"10.1140","volume":"85","author":[{"name":"ATLAS 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