Search for rare decays of Z and Higgs bosons to J/ψJ/ψ and a photon in proton-proton collisions at √s = 13TeV; European Physical Journal C; Vol. 79, iss. 2

書誌詳細
Parent link:European Physical Journal C
Vol. 79, iss. 2.— 2019.— [94, 27 p.]
団体著者: Национальный исследовательский Томский политехнический университет Исследовательская школа физики высокоэнергетических процессов
その他の著者: Sirunyan A. M., Tumasyan A. R., Adam W. Wolfgang, Ambrogi F. Federico, Babaev A. A. Anton Anatoljevich
要約:Title screen
A search is presented for decays of ZZ and Higgs bosons to a J/ψJ/ψ meson and a photon, with the subsequent decay of the J/ψJ/ψ to μ+μ−μ+μ−. The analysis uses data from proton-proton collisions with an integrated luminosity of 35.9fb−1fb−1 at s√=13TeVs=13TeV collected with the CMS detector at the LHC. The observed limit on the Z→J/ψγZ→J/ψγ decay branching fraction, assuming that the J/ψJ/ψ meson is produced unpolarized, is 1.4×10−61.4×10−6 at 95% confidence level, which corresponds to a rate higher than expected in the standard model by a factor of 15. For extreme-polarization scenarios, the observed limit changes from −13.6−13.6 to +8.6%+8.6% with respect to the unpolarized scenario. The observed upper limit on the branching fraction for H→J/ψγH→J/ψγ where the J/ψJ/ψ meson is assumed to be transversely polarized is 7.6×10−47.6×10−4, a factor of 260 larger than the standard model prediction. The results for the Higgs boson are combined with previous data from proton-proton collisions at s√=8TeVs=8TeV to produce an observed upper limit on the branching fraction for H→J/ψγH→J/ψγ that is a factor of 220 larger than the standard model value.
言語:英語
出版事項: 2019
主題:
オンライン・アクセス:https://doi.org/10.1140/epjc/s10052-019-6562-5
フォーマット: 電子媒体 図書の章
KOHA link:https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=662133

MARC

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200 1 |a Search for rare decays of Z and Higgs bosons to J/ψJ/ψ and a photon in proton-proton collisions at √s = 13TeV  |f A. M. Sirunyan, A. R. Tumasyan, W. Adam [et al.] 
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330 |a A search is presented for decays of ZZ and Higgs bosons to a J/ψJ/ψ meson and a photon, with the subsequent decay of the J/ψJ/ψ to μ+μ−μ+μ−. The analysis uses data from proton-proton collisions with an integrated luminosity of 35.9fb−1fb−1 at s√=13TeVs=13TeV collected with the CMS detector at the LHC. The observed limit on the Z→J/ψγZ→J/ψγ decay branching fraction, assuming that the J/ψJ/ψ meson is produced unpolarized, is 1.4×10−61.4×10−6 at 95% confidence level, which corresponds to a rate higher than expected in the standard model by a factor of 15. For extreme-polarization scenarios, the observed limit changes from −13.6−13.6 to +8.6%+8.6% with respect to the unpolarized scenario. The observed upper limit on the branching fraction for H→J/ψγH→J/ψγ where the J/ψJ/ψ meson is assumed to be transversely polarized is 7.6×10−47.6×10−4, a factor of 260 larger than the standard model prediction. The results for the Higgs boson are combined with previous data from proton-proton collisions at s√=8TeVs=8TeV to produce an observed upper limit on the branching fraction for H→J/ψγH→J/ψγ that is a factor of 220 larger than the standard model value. 
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