$(g-2)_{e,μ}$ anomalies and decays $h, Z\to e_b e_a $ in 3-3-1 models with inverse seesaw neutrinos

The lepton flavor violating (LFV) decays $h, Z \to e_{b} e_{a}$ , and $e_{b} \to e_{a} γ$ are discussed in a class of general 3-3-1 models adding heavy neutral leptons and singly charged Higgs bosons to accommodate experimental data of neutrino oscillation and $(g - 2)_{e_{a}}$ anomalies of charged leptons through the inverse seesaw mechanism. We show that the models with the minimal number of inverse seesaw neutrinos cannot reach the $1 σ$ range of $(g - 2)_{μ}$ data due to the experimental upper bounds on decay rates of $(τ \to μ γ)$ and $(μ \to e γ)$ . Features of LFV decays are presented in detail, focusing on the regions of parameter space satisfying the $1 σ$ ranges of $(g - 2)_{e, μ}$ data.

$(g - 2)_{e, μ}$ anomalies and decays $h, Z \to e_{b} e_{a}$ in 3-3-1 models with inverse seesaw neutrinos

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$(g - 2)_{e, μ}$ anomalies and decays $h, Z \to e_{b} e_{a}$ in 3-3-1 models with inverse seesaw neutrinos

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(g−2)e,μ(g−2)e,μ​ anomalies and decays h,Z→ebeah,Z→eb​ea​ in 3-3-1 models with inverse seesaw neutrinos

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(g−2)e,μ(g−2)e,μ​ anomalies and decays h,Z→ebeah,Z→eb​ea​ in 3-3-1 models with inverse seesaw neutrinos

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$(g - 2)_{e, μ}$ anomalies and decays $h, Z \to e_{b} e_{a}$ in 3-3-1 models with inverse seesaw neutrinos

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$(g - 2)_{e, μ}$ anomalies and decays $h, Z \to e_{b} e_{a}$ in 3-3-1 models with inverse seesaw neutrinos

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