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    Radiative Decays of the Higgs Boson to a Pair of Fermions

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    We revisit the radiative decays of the Higgs boson to a fermion pair h→ffˉγh\rightarrow f\bar{f}\gamma where ff denotes a fermion in the Standard Model (SM). We include the chirality-flipping diagrams via the Yukawa couplings at the order O(yf2α)\mathcal{O}(y_f^2 \alpha), the chirality-conserving contributions via the top-quark loops of the order O(yt2α3)\mathcal{O}(y_t^2 \alpha^3), and the electroweak loops at the order O(α4)\mathcal{O}(\alpha^4). The QED correction is about Qf2×O(1%)Q_f^2\times {\cal O}(1\%) and contributes to the running of fermion masses at a similar level, which should be taken into account for future precision Higgs physics. The chirality-conserving electroweak-loop processes are interesting from the observational point of view. First, the branching fraction of the radiative decay h→μ+μ−γh \to \mu^+\mu^- \gamma is about a half of that of h→μ+μ−h \to \mu^+\mu^-, and that of h→e+e−γh \to e^+ e^- \gamma is more than four orders of magnitude larger than that of h→e+e−h \to e^+ e^-, both of which reach about 10−410^{-4}. The branching fraction of h→τ+τ−γh \to \tau^+\tau^- \gamma is of the order 10−310^{-3}. All the leptonic radiative decays are potentially observable at the LHC Run 2 or the HL-LHC. The kinematic distributions for the photon energy or the fermion pair invariant mass provide non-ambiguous discrimination for the underlying mechanisms of the Higgs radiative decay. We also study the process h→ccˉγh \to c\bar c \gamma and evaluate the observability at the LHC. We find it comparable to the other related studies and better than the h→J/ψ γh \to J/\psi\ \gamma channel in constraining the charm-Yukawa coupling.Comment: 23 pages, 6 figures, 6 tables; Minor corrections, references updated, version published in JHE
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