REVIEW
$(g-2)_{\ell}$ and LFV decays in a $U(1)_{L_{\mu} -L_{\tau}}$ left-right model with inverse seesaw neutrinos
High Energy Physics - Phenomenology · Submitted 30 Aug 2026 · 92 references
Pith's verdict: Solid and technically careful: the LFV suppression is genuinely symmetry-driven, but the (g-2) fit is a proof-of-existence with a few table typos.
T0 · AI review
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Referee report
The paper
The paper claims
A left-right model with muon-tau symmetry can explain the muon and electron g-2 anomalies via a charged Higgs boson while universally suppressing all lepton-flavor-violating decays.
The reading
Extended reading notes
Core claim
The LR one-loop contributions from singly charged Higgs bosons can give sizable contributions to Δa_{e,μ}, reaching values close to the current experimental sensitivities, namely Δa_μ ≃ 10^{-9} and Δa_e ∼ O(10^{-13}), while all one-loop contributions to lepton-flavor-violating decay amplitudes vanish for the chirally-enhanced part, leading to LFV rates far below current bounds.
Load-bearing premise
The assumption that the Yukawa matrices Y_ℓ and Ỹ_ℓ are diagonal, which follows from the U(1)_{Lμ-Lτ} charge assignments of the left-handed and right-handed leptons. This diagonality is responsible for the vanishing of the dominant chirally-enhanced LR contributions to LFV decays. If the symmetry were broken or the charge assignments were different, off-diagonal couplings would appear and could generate observable LFV rates, invalidating the central claim.
Original abstract
In the framework of a $U(1)_{L_{\mu} -L_{\tau}}$ left-right model with inverse seesaw neutrinos recently proposed, we show that one-loop contributions from heavy singly charged Higgs bosons to the anomalous magnetic moments of charged leptons $(g-2)_{e,\mu}$ can accommodate the observed discrepancies, of $10^{-9}$ and $\mathcal{O}(10^{-13})$ for the muon and electron, respectively. Meanwhile, all lepton-flavor violating decay rates for $h\to e_b^\pm e_a^\mp $, $Z\to e_b^\pm e_a^\mp$, and $e_b\to e_a \gamma$ are found to be highly suppressed as a consequence of the gauged $U(1)_{L_{\mu}-L_\tau}$ symmetry.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
In the framework of a $U(1)_{L_{\mu} -L_{\tau}}$ left-right model with inverse seesaw neutrinos recently proposed, we show that one-loop contributions from heavy singly charged Higgs bosons to the anomalous magnetic moments of charged leptons $(g-2)_{e,\mu}$ can accommodate the observed discrepancies, of $10^{-9}$ and $\mathcal{O}(10^{-13})$ for the muon and electron, respectively. Meanwhile, all lepton-flavor violating decay rates for $h\to e_b^\pm e_a^\mp $, $Z\to e_b^\pm e_a^\mp$, and $e_b\to e_a \gamma$ are found to be highly suppressed as a consequence of the gauged $U(1)_{L_{\mu}-L_\tau}$ symmetry.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In the framework of a $U(1)_{L_{\mu} -L_{\tau}}$ left-right model with inverse seesaw neutrinos recently proposed, we show that one-loop contributions from heavy singly charged Higgs bosons to the anomalous magnetic moments of charged leptons $(g-2)_{e,\mu}$ can accommodate the observed discrepancies, of $10^{-9}$ and $\mathcal{O}(10^{-13})$ for the muon and electron, respectively. | result 0.94 | 0.92 | 0.73 | asserted 0.97 |
| s1 | Meanwhile, all lepton-flavor violating decay rates for $h\to e_b^\pm e_a^\mp $, $Z\to e_b^\pm e_a^\mp$, and $e_b\to e_a \gamma$ are found to be highly suppressed as a consequence of the gauged $U(1)_{L_{\mu}-L_\tau}$ symmetry. | result 1.00 | 0.93 | 0.17 | asserted 1.00 |
What was examined, and what was not
- arXiv listing abstract v1
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- references and citing sentences
- relations to other papers
- P abstract
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Figures
Showing 4 of the paper's 8 figures. See all figures in the PDF ↗ Figures reproduced from arXiv:2608.29697 by the authors.
References
How the literature uses it
What this paper does with the arXiv papers it cites
What it cites · 49 sentences without a confident label
Uses the method or tool of 11 papers
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The analytic formulas for the one-loop contributions considered here are expressed in terms of Passarino–Veltman (PV) functions, using the results of Ref. [ref] , which are consistent with previous works [ref] and with the LoopTools package [ref] .
Two-body lepton-flavour-violating decays in a 2HDM with soft family-lepton-number breaking · Analytic formulas for decay rates LFV$Z$ and LFV$h$ in the LRiss · 0.89
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The analytic formulas for the one-loop contributions considered here are expressed in terms of Passarino–Veltman (PV) functions, using the results of Ref. [ref] , which are consistent with previous works [ref] and with the LoopTools package [ref] .
$(g-2)_{e,\mu}$ anomalies and decays $h\to e_a e_b$, $Z\to e_ae_b$, and $e_b\to e_a \gamma$ in a two Higgs doublet model with inverse seesaw neutrinos · Analytic formulas for decay rates LFV$Z$ and LFV$h$ in the LRiss · 0.89
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The analytic formulas for the one-loop contributions considered here are expressed in terms of Passarino–Veltman (PV) functions, using the results of Ref. [ref] , which are consistent with previous works [ref] and with the LoopTools package [ref] .
$(g-2)_{e,\mu}$ and Lepton flavor violating decays in a left-right model · Analytic formulas for decay rates LFV$Z$ and LFV$h$ in the LRiss · 0.89
Uses data or values from 31 papers
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The current experimental data on $(g-2)_μ$ [ref] are consistent with the SM prediction [ref] , with $Δa_μ≡Δa^exp_μ= a^exp_μ -a^SM_μ =(3.8±6.3 ) ×10^-10$, which still allows for sizable values of $Δa_μ ≃10^-9$.
The anomalous magnetic moment of the muon in the Standard Model: an update · Introduction · 0.99
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The current experimental data on $(g-2)_μ$ [ref] are consistent with the SM prediction [ref] , with $Δa_μ≡Δa^exp_μ= a^exp_μ -a^SM_μ =(3.8±6.3 ) ×10^-10$, which still allows for sizable values of $Δa_μ ≃10^-9$.
2506.03069 · Introduction · 0.99
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The current experimental data on $(g-2)_μ$ [ref] are consistent with the SM prediction [ref] , with $Δa_μ≡Δa^exp_μ= a^exp_μ -a^SM_μ =(3.8±6.3 ) ×10^-10$, which still allows for sizable values of $Δa_μ ≃10^-9$.
2308.06230 · Introduction · 0.99
Compares with 5 papers
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Except for the contributions from the singly charged Higgs bosons, our calculations of the remaining one-loop contributions involving the two singly charged gauge bosons, neutral Higgs bosons, and neutral gauge bosons are generally consistent with those presented in Refs. [ref] .
Neutrino mass and charged lepton flavor violation in an extended left-right symmetric model · Feynman rules for one-loop contributions to LFV decays · 1.00
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Except for the contributions from the singly charged Higgs bosons, our calculations of the remaining one-loop contributions involving the two singly charged gauge bosons, neutral Higgs bosons, and neutral gauge bosons are generally consistent with those presented in Refs. [ref] .
Neutrino mass, mixing and muon $g-2$ explanation in $U(1)_{L_\mu-L_\tau}$ extension of left-right theory · Feynman rules for one-loop contributions to LFV decays · 1.00
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The results given in Eq. [ref] agree with those of Ref. [ref] with $t_R=1$.
$(g-2)_{e,\mu}$ and Lepton flavor violating decays in a left-right model · The $U(1)_L_μ -L_τ$ left-right model with ISS neutrinos · 1.00
Cites as background 18 papers
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In Sec. [ref], we review the LRiss model, including the particle content, Higgs potential, and Yukawa Lagrangian introduced in Ref. [ref] .
Neutrino mass, mixing and muon $g-2$ explanation in $U(1)_{L_\mu-L_\tau}$ extension of left-right theory · Introduction · 0.83
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The quark sector and $H_L$ were discussed in Refs. [ref] ; however, they are not relevant to the present work and are therefore omitted here.
Neutrino mass and charged lepton flavor violation in an extended left-right symmetric model · The $U(1)_L_μ -L_τ$ left-right model with ISS neutrinos · 0.95
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The LRiss model is a left-right (LR) extension of the original LR models [ref] and retains the characteristic neutral gauge boson $Z'_μτ$ associated with the $U(1)_L_μ-L_τ$ symmetry [ref] .
Simple Left-Right Theory: Lepton Number Violation at the LHC · Introduction · 0.88
Discussion
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