We revisit the radiative decays of the Higgs boson to a fermion pair
h→ffˉ​γ where f denotes a fermion in the Standard Model
(SM). We include the chirality-flipping diagrams via the Yukawa couplings at
the order O(yf2​α), the chirality-conserving contributions
via the top-quark loops of the order O(yt2​α3), and the
electroweak loops at the order O(α4). The QED correction is
about Qf2​×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−γ is about a half of
that of h→μ+μ−, and that of h→e+e−γ is more than
four orders of magnitude larger than that of h→e+e−, both of which
reach about 10−4. The branching fraction of h→τ+τ−γ is
of the order 10−3. 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→ccˉγ and evaluate the observability at
the LHC. We find it comparable to the other related studies and better than the
h→J/ψ γ channel in constraining the charm-Yukawa coupling.Comment: 23 pages, 6 figures, 6 tables; Minor corrections, references updated,
version published in JHE