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Search for the Higgs boson decay to $Z\gamma$ in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$
Results are presented from a search for the Higgs boson decay $\mathrm{H}\to\mathrm{Z}\gamma$, where $\mathrm{Z}\to\ell^+\ell^-$ with $\ell=\mathrm{e}$ or $\mu$. This search is performed using a sample of proton-proton collision data at a center-of-mass energy of $13~\mathrm{TeV}$, recorded by the C...
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Publicado: |
2021
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Acceso en línea: | http://cds.cern.ch/record/2784454 |
Sumario: | Results are presented from a search for the Higgs boson decay $\mathrm{H}\to\mathrm{Z}\gamma$, where $\mathrm{Z}\to\ell^+\ell^-$ with $\ell=\mathrm{e}$ or $\mu$. This search is performed using a sample of proton-proton collision data at a center-of-mass energy of $13~\mathrm{TeV}$, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of $137~\mathrm{fb}^{-1}$. Events are assigned to mutually exclusive categories, which exploit differences in event topology and kinematics of distinct Higgs production modes to enhance signal sensitivity. To detect a potential signal, fits are performed to the distributions of $m_{\ell^+\ell^-\gamma}$ in each of these categories simultaneously. The observed (expected) upper limit at $95\%$ confidence level on the signal strength $\mu$, defined as the product of the cross section and the branching fraction [$\sigma(\mathrm{pp}\to\mathrm{H})\times\,\mathcal{B}(\mathrm{H}\to\mathrm{Z}\gamma)$], relative to the standard model expectation, is $4.1\,$($1.8$). The best fit value of the signal strength is found to be $\mu=2.4\,\pm0.9$, corresponding to $\sigma(\mathrm{pp}\to\mathrm{H})\times\,\mathcal{B}(\mathrm{H}\to\mathrm{Z}\gamma)=0.21\pm0.08~\mathrm{pb}$. The statistical significance of the observed excess of events under the background-only hypothesis is 2.7 standard deviations at $m_\mathrm{H}=125.38~\mathrm{GeV}$. $$\textit{This document has been revised with respect to the version dated October 18, 2021}$$ |
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