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Constraining Lepton Flavor Violating Higgs Couplings at the HL-LHC in the Vector Boson Fusion Channel

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arxiv 2210.16287 v2 pith:DPY4ATXP submitted 2022-10-28 hep-ph

classification hep-ph
keywords higgshl-lhcbosonmodelbranchingchannelcouplingsflavor
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We explore the parameter space of lepton flavor violating (LFV) neutral Higgs Yukawa couplings with the muon and tau leptons that can be probed at the high-luminosity Large Hadron Collider (HL-LHC) via the vector boson fusion~(VBF) Higgs production process. Our projected sensitivities for the Standard Model Higgs ($h$) LFV branching ratio ${\rm Br}(h \to \mu\tau)$ in the $pp \to h j j \to (h \to \mu \tau) jj$ channel at the HL-LHC are contrasted with the current and future low-energy constraints from the anomalous magnetic moment and electric dipole moment of the muon, as well as with other LFV observables, such as $\tau\to 3\mu$ and $\tau\to \mu\gamma$. We also study the LFV prospects of a generic beyond the Standard Model neutral Higgs boson ($H$) with a mass in the range of $m_{H}\in [20,800]~$GeV and give the projected model-independent upper limits on the VBF production cross-section of $Hjj$ times the branching ratio of $H\to \mu\tau$ at the HL-LHC. We interpret these results in the context of a two-Higgs doublet model as a case study.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. LFV decays in a 3-3-1 model with singlet leptoquarks

    hep-ph 2026-07 conditional novelty 5.0 of 10

    In the 3-3-1 model with a singlet leptoquark, Higgs and Z lepton-flavor-violating decays are nearly proportional to radiative charged-lepton decays, and the model cannot produce large electron and muon magnetic anomal...

  2. The Higgs boson decay $h \rightarrow bs$ in the NB-LSSM

    hep-ph 2026-07 conditional novelty 4.0 of 10

    Under B̄ o Xsγ constraints, NB-LSSM parameters can raise Br(h o bs) to ~10^{-5}, orders of magnitude above the SM, while remaining consistent with Higgs mass and signal strengths.

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