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Lepton flavor violating Higgs boson decays from massive seesaw neutrinos
High Energy Physics - Phenomenology · Submitted 27 Jul 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim In contrast, in the MSSM-seesaw case, sizeable branching ratios are found for some of the leptonic flavor violating decays of the MSSM neutral Higgs bosons and for some choices of the seesaw matrices and MSSM parameters.
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Lepton flavor violating Higgs boson decays are studied within the context of seesaw models with Majorana massive neutrinos. Two models are considered: The SM-seesaw, with the Standard Model Particle content plus three right handed neutrinos, and the MSSM-seesaw, with the Minimal Supersymmetric Standard Model particle content plus three right handed neutrinos and their supersymmetric partners. The widths for these decays are derived from a full one-loop diagrammatic computation in both models, and they are analyzed numerically in terms of the seesaw parameters, namely, the Dirac and Majorana mass matrices. Several possible scenarios for these mass matrices that are compatible with neutrino data are considered. In the SM-seesaw case, very small branching ratios are found for all studied scenarios. These ratios are explained as a consequence of the decoupling behaviour of the heavy right handed neutrinos. In contrast, in the MSSM-seesaw case, sizeable branching ratios are found for some of the leptonic flavor violating decays of the MSSM neutral Higgs bosons and for some choices of the seesaw matrices and MSSM parameters. The relevance of the two competing sources of lepton flavor changing interactions in the MSSM-seesaw case is also discussed. The non-decoupling behaviour of the supersymmetric particles contributing in the loop-diagrams is finally shown.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Lepton flavor violating Higgs boson decays are studied within the context of seesaw models with Majorana massive neutrinos. | contribution 0.74 | 0.63 | 0.04 | asserted 0.93 |
| s1 | Two models are considered: The SM-seesaw, with the Standard Model Particle content plus three right handed neutrinos, and the MSSM-seesaw, with the Minimal Supersymmetric Standard Model particle content plus three right handed neutrinos and their supersymmetric partners. | method 0.80 | 0.45 | 0.02 | asserted 0.97 |
| s2 | The widths for these decays are derived from a full one-loop diagrammatic computation in both models, and they are analyzed numerically in terms of the seesaw parameters, namely, the Dirac and Majorana mass matrices. | method 0.96 | 0.95 | 0.05 | asserted 1.00 |
| s3 | Several possible scenarios for these mass matrices that are compatible with neutrino data are considered. | method 0.85 | 0.80 | 0.02 | asserted 0.75 |
| s4 | In the SM-seesaw case, very small branching ratios are found for all studied scenarios. | result 1.00 | 0.94 | 0.17 | asserted 1.00 |
| s5 | These ratios are explained as a consequence of the decoupling behaviour of the heavy right handed neutrinos. | interpretation 1.00 | 0.74 | 0.09 | asserted 1.00 |
| s6 | In contrast, in the MSSM-seesaw case, sizeable branching ratios are found for some of the leptonic flavor violating decays of the MSSM neutral Higgs bosons and for some choices of the seesaw matrices and MSSM parameters. | result 1.00 | 0.94 | 0.63 | asserted 1.00 |
| s7 | The relevance of the two competing sources of lepton flavor changing interactions in the MSSM-seesaw case is also discussed. | contribution 0.85 | 0.76 | 0.05 | asserted 0.50 |
| s8 | The non-decoupling behaviour of the supersymmetric particles contributing in the loop-diagrams is finally shown. | result 0.73 | 0.90 | 0.20 | asserted 1.00 |
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Original abstract
Lepton flavor violating Higgs boson decays are studied within the context of seesaw models with Majorana massive neutrinos. Two models are considered: The SM-seesaw, with the Standard Model Particle content plus three right handed neutrinos, and the MSSM-seesaw, with the Minimal Supersymmetric Standard Model particle content plus three right handed neutrinos and their supersymmetric partners. The widths for these decays are derived from a full one-loop diagrammatic computation in both models, and they are analyzed numerically in terms of the seesaw parameters, namely, the Dirac and Majorana mass matrices. Several possible scenarios for these mass matrices that are compatible with neutrino data are considered. In the SM-seesaw case, very small branching ratios are found for all studied scenarios. These ratios are explained as a consequence of the decoupling behaviour of the heavy right handed neutrinos. In contrast, in the MSSM-seesaw case, sizeable branching ratios are found for some of the leptonic flavor violating decays of the MSSM neutral Higgs bosons and for some choices of the seesaw matrices and MSSM parameters. The relevance of the two competing sources of lepton flavor changing interactions in the MSSM-seesaw case is also discussed. The non-decoupling behaviour of the supersymmetric particles contributing in the loop-diagrams is finally shown.
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References
How later papers used it
61 later papers cite it
1 later paper by other authors is listed below: 1 built on it. 1 more paper by the same authors is listed: 1 compared its own results with it.
Builds on it 1 of 2 papers with this label
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Presented results for the full one-loop computation in the physical neutrino mass basis based on this paper's results for the type-I seesaw model.
Lepton flavor violation from low scale seesaw neutrinos with masses reachable at the LHC (2017) · 0.86 · paraphrased: the licence does not allow quoting
Compares with it 1 of 4 papers with this label · 1 by the same authors
By the same authors
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Compared its own numerical predictions for partial widths and branching ratios of the H to lepton-pair decays with those from the full one-loop computation in the mass basis taken from this paper and another work.
Effective lepton flavor violating $\boldsymbol{H\ell_i\ell_j}$ vertex from right-handed neutrinos within the mass insertion approximation (2016) (same authors) · 0.99 · paraphrased: the licence does not allow quoting
How the literature uses it
56 arXiv papers cite this in 97 sentences
Papers citing it · 56 sentences without a confident label
Contests it 1 paper
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Notice that we have corrected the global signs of $F_L^(1)$, $F_L,R^(4)$ and $F_L,R^(5)$, which were typos in the original expressions given in [ref] .
Lepton flavor violation from low scale seesaw neutrinos with masses reachable at the LHC · Oblique parameters: $S, T, U$ · contest 0.93
Builds on it 2 papers
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First we present, based on the results for the type-I seesaw model in Ref. [ref] , the results for the full one-loop computation done in the physical neutrino mass basis.
Lepton flavor violation from low scale seesaw neutrinos with masses reachable at the LHC · Introduction · 0.86
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[ref] substituting $U$ by $N$.
Higgs lepton flavour violation: UV completions and connection to neutrino masses · Dirac neutrinos, see-saw type I and III, inverse see-saw · 0.86
Uses its method or tool 2 papers
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In Fig. [ref] we have used the complete computation presented in [ref] .
Global constraints on heavy neutrino mixing · LFV $h$ decays · 0.90
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The mass matrices of the other SUSY particles, namely the charginos, neutralinos, and charged sleptons, are the same as in the SUSY type-I seesaw studied in Ref. [ref] , so we will use their definitions of the corresponding rotation matrices, which in turn were based on the conventions of Ref. [ref] for the charginos and neutralinos.
Lepton flavor violation from low scale seesaw neutrinos with masses reachable at the LHC · The SUSY Inverse Seesaw model · 0.83
Uses its data or values 2 papers
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The results of the LFV vertex functions are taken from [ref] , and are not written here explicitely for shortness.
Sensitivity to the Higgs Sector of SUSY-Seesaw Models in the Lepton Flavour Violating tau-->mu f0(980) decay · Results for BR$(τ→μf_0(980))$ · 1.00
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The respective partial decay width in the limit $m_h≫m_a,b$ is [ref] [equation] The corresponding branching ratio is Br$(h→e_ae_b)= Γ(h→e_ae_b)/Γ^total_h$ where $Γ^total_h≃4.1×10^-3$ GeV [ref] with $q^2 ≡( p_1+p_2)^2=m^2_h$.
$(g-2)_{e,\mu}$ and Lepton flavor violating decays in a left-right model · The LFV decays $Z→e_b^±e_a^∓$ and $h→e_b^±e_a^∓$ · 0.81
Compares with it 2 papers
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We found that, having these neutrinos TeV scale masses and large Yukawa couplings at the same time, the LFVHD rates are manifestly enhanced with respect to the standard type-I seesaw, where rates of $𝒪(10^-30)$ were obtained [ref] .
Lepton flavor violation from low scale seesaw neutrinos with masses reachable at the LHC · Maximum allowed BR($H→ℓ_kℓ̅_m$) · 0.92
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In particular, we derive the full effective cLFV $Z$ and Higgs vertices in the presence of heavy neutral leptons without any simplifying assumptions, finding good agreement with previous calculations [ref] .
LFV Higgs and $Z$-boson decays: leptonic CPV phases and CP asymmetries · Introduction · 0.97
Cites it as support 1 paper
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The MSSM, being a Two-Higgs-Doublet models of type-II, cannot [In fact, several studies have shown that one cannot accommodate $BR(h →τμ) ∼1 %$ when the low-energy theory is the MSSM [ref] .
Lepton flavor violation beyond the MSSM · Higgs LFV decays · 0.99
Cites it as background 24 papers
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In particular, previous studies of $h→τμ$ within the supersymmetric framework have been carried out in Refs. [ref] .
Large BR(h->tau mu) in the MSSM? · Introduction · 1.00
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[ref] for details.
Higgs lepton flavour violation: UV completions and connection to neutrino masses · Dirac neutrinos, see-saw type I and III, inverse see-saw · 0.93
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Also, the LFVHD of neutral Higgses were studied widely [ref] where one-loop contributions were computed in many specific frameworks such as suppersymmetric (SUSY) [ref] , lepton-flavored dark matter [ref] , leptoquark [ref] , seesaw [ref] , extended mirror fermion [ref] , 3-3-1 and radiative neutrino mass models [ref] , and others [ref] .
One loop contributions to neutral Higgs decay h-->mu tau · Introduction · 0.92
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