Search for a light charged Higgs boson in the H±→cs channel in proton-proton collisions at √s=13  TeV / A. M. Sirunyan, A. R. Tumasyan, W. Adam [et al.]

Уровень набора: Physical Review D, particles, fields, gravitation, and cosmology = 1970-Альтернативный автор-лицо: Sirunyan, A. M.;Tumasyan, A. R.;Adam, W., Wolfgang;Ambrogi, F., Federico;Tyurin, N. E., Nikolay Evgenjevich;Babaev, A. A., physicist, engineer-issledovatelskogo Polytechnic University, candidate of physical and mathematical Sciences, 1981-, Anton Anatoljevich;Okhotnikov, V. V., physicist, engineer of Tomsk Polytechnic University, 1992-, Vitaly Vladimirovich;Sukhikh, L. G., physicist, Associate Professor of Tomsk Polytechnic University, Doctor of Sciences, 1984-, Leonid GrigorievichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет, Исследовательская школа физики высокоэнергетических процессов, (2017- )Язык: английский.Страна: .Резюме или реферат: A search is conducted for a low-mass charged Higgs boson produced in a top quark decay and subsequently decaying into a charm and a strange quark. The data sample was recorded in proton-proton collisions at √s=13  TeV by the CMS experiment at the LHC and corresponds to an integrated luminosity of 35.9  fb−1. The search is performed in the process of top quark pair production, where one top quark decays to a bottom quark and a charged Higgs boson and the other to a bottom quark and a W boson. With the W boson decaying to a charged lepton (electron or muon) and a neutrino, the final state comprises an isolated lepton, missing transverse momentum, and at least four jets, of which two are tagged as b jets. To enhance the search sensitivity, one of the jets originating from the charged Higgs boson is required to satisfy a charm tagging selection. No significant excess beyond standard model predictions is found in the dijet invariant mass distribution. An upper limit in the range 1.68%-0.25% is set on the branching fraction of the top quark decay to the charged Higgs boson and bottom quark for a charged Higgs boson mass between 80 and 160 GeV..Примечания о наличии в документе библиографии/указателя: [References: 66 tit.].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: 66 tit.]

A search is conducted for a low-mass charged Higgs boson produced in a top quark decay and subsequently decaying into a charm and a strange quark. The data sample was recorded in proton-proton collisions at √s=13  TeV by the CMS experiment at the LHC and corresponds to an integrated luminosity of 35.9  fb−1. The search is performed in the process of top quark pair production, where one top quark decays to a bottom quark and a charged Higgs boson and the other to a bottom quark and a W boson. With the W boson decaying to a charged lepton (electron or muon) and a neutrino, the final state comprises an isolated lepton, missing transverse momentum, and at least four jets, of which two are tagged as b jets. To enhance the search sensitivity, one of the jets originating from the charged Higgs boson is required to satisfy a charm tagging selection. No significant excess beyond standard model predictions is found in the dijet invariant mass distribution. An upper limit in the range 1.68%-0.25% is set on the branching fraction of the top quark decay to the charged Higgs boson and bottom quark for a charged Higgs boson mass between 80 and 160 GeV.

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