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Электронный каталог: Hayrapetyan, A. - Search for Rare Decays of the Z and Higgs Bosons to a J∕*q or *q(2S) Meson and a Photon in Proton...
Hayrapetyan, A. - Search for Rare Decays of the Z and Higgs Bosons to a J∕*q or *q(2S) Meson and a Photon in Proton...

Статья
Автор: Hayrapetyan, A.
Physics Letters B: Search for Rare Decays of the Z and Higgs Bosons to a J∕*q or *q(2S) Meson and a Photon in Proton...
б.г.
ISBN отсутствует
Автор: Hayrapetyan, A.
Physics Letters B: Search for Rare Decays of the Z and Higgs Bosons to a J∕*q or *q(2S) Meson and a Photon in Proton...
б.г.
ISBN отсутствует
Статья
Hayrapetyan, A.
Search for Rare Decays of the Z and Higgs Bosons to a J∕*q or *q(2S) Meson and a Photon in Proton-Proton Collisions at *%𝑠 = 13 TeV / A.Hayrapetyan, S.Afanasiev, V.Alexakhin, D.Budkouski, I.Golutvin, I.Gorbunov, V.Karjavine, V.Korenkov, A.Lanev, A.Malakhov, V.Matveev, V.Palichik, V.Perelygin, M.Savina, V.Shalaev, S.Shmatov, S.Shulha, V.Smirnov, O.Teryaev, N.Voytishin, B.S.Yuldashev, A.Zarubin, I.Zhizhin, N.Krasnikov, O.Kodolova, A.Nikitenko, S.Polikarpov, Z.Tsamalaidze, [CMS Collab.]. – Text : electronic // Physics Letters B. – 2025. – Vol. 865. – P. 139462. – URL: https://doi.org/10.1016/j.physletb.2025.139462. – Bibliogr.: 64.
A search is presented for rare decays of the Z and Higgs bosons to a photon and a J∕*q or a *q(2S) meson, with the charmonium state subsequentially decaying to a pair of muons. The data set corresponds to an integrated luminosity of 123 fb&sup(−1) of proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. No evidence for branching fractions of these rare decay channels larger than predicted in the standard model is observed. Upper limits at 95% confidence level are set: B(H *> J∕*q*g ) < 2.6 × 10&sup(−4), B(H *> *q(2S)*g ) < 9.9 × 10&sup(−4), B(Z *> J∕*q*g ) < 0.6 × 10&sup(−6), and B(Z *> *q(2S)g ) < 1.3 × 10&sup(−6). The ratio of the Higgs boson coupling modifiers *k&sub(c)∕*k&sub(*g) is constrained to be in the interval (−157, +199) at 95% confidence level. Assuming *k&sub(*g) = 1, this interval becomes (−166, +208).
Спец.(статьи,препринты) = С 346.6д1 - Чармоний, боттомоний, топ-кварк. Очарованные частицы и др. резонансы из тяжелых кварков
Спец.(статьи,препринты) = С 346.2в - Взаимодействие протонов с протонами
ОИЯИ = ОИЯИ (JINR)2025
Hayrapetyan, A.
Search for Rare Decays of the Z and Higgs Bosons to a J∕*q or *q(2S) Meson and a Photon in Proton-Proton Collisions at *%𝑠 = 13 TeV / A.Hayrapetyan, S.Afanasiev, V.Alexakhin, D.Budkouski, I.Golutvin, I.Gorbunov, V.Karjavine, V.Korenkov, A.Lanev, A.Malakhov, V.Matveev, V.Palichik, V.Perelygin, M.Savina, V.Shalaev, S.Shmatov, S.Shulha, V.Smirnov, O.Teryaev, N.Voytishin, B.S.Yuldashev, A.Zarubin, I.Zhizhin, N.Krasnikov, O.Kodolova, A.Nikitenko, S.Polikarpov, Z.Tsamalaidze, [CMS Collab.]. – Text : electronic // Physics Letters B. – 2025. – Vol. 865. – P. 139462. – URL: https://doi.org/10.1016/j.physletb.2025.139462. – Bibliogr.: 64.
A search is presented for rare decays of the Z and Higgs bosons to a photon and a J∕*q or a *q(2S) meson, with the charmonium state subsequentially decaying to a pair of muons. The data set corresponds to an integrated luminosity of 123 fb&sup(−1) of proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. No evidence for branching fractions of these rare decay channels larger than predicted in the standard model is observed. Upper limits at 95% confidence level are set: B(H *> J∕*q*g ) < 2.6 × 10&sup(−4), B(H *> *q(2S)*g ) < 9.9 × 10&sup(−4), B(Z *> J∕*q*g ) < 0.6 × 10&sup(−6), and B(Z *> *q(2S)g ) < 1.3 × 10&sup(−6). The ratio of the Higgs boson coupling modifiers *k&sub(c)∕*k&sub(*g) is constrained to be in the interval (−157, +199) at 95% confidence level. Assuming *k&sub(*g) = 1, this interval becomes (−166, +208).
Спец.(статьи,препринты) = С 346.6д1 - Чармоний, боттомоний, топ-кварк. Очарованные частицы и др. резонансы из тяжелых кварков
Спец.(статьи,препринты) = С 346.2в - Взаимодействие протонов с протонами
ОИЯИ = ОИЯИ (JINR)2025