2013
DOI: 10.1103/physrevd.87.013010
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Supersymmetric type-III seesaw mechanism: Lepton flavor violation and LHC phenomenology

Abstract: We study a supersymmetric version of the type-III seesaw mechanism considering two variants of the model: a minimal version for explaining neutrino data with only two copies of 24 superfields and a model with three generations of 24-plets. The latter predicts, in general, rates for ! e inconsistent with experimental data. However, this bound can be evaded if certain special conditions within the neutrino sector are fulfilled. In the case of two 24-plets, lepton flavor violation constraints can be satisfied muc… Show more

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Cited by 8 publications
(9 citation statements)
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References 134 publications
(201 reference statements)
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“…LFV violating observables have been intensively discussed in supersymmetric high-scale seesaw models [13][14][15][16][17][18][19][20][21][22][24][25][26]. In view of the above-mentioned controversy, we focus on the Z-penguin and, in particular, on the chargino-sneutrino contributions.…”
Section: Revising the 1-loopmentioning
confidence: 99%
“…LFV violating observables have been intensively discussed in supersymmetric high-scale seesaw models [13][14][15][16][17][18][19][20][21][22][24][25][26]. In view of the above-mentioned controversy, we focus on the Z-penguin and, in particular, on the chargino-sneutrino contributions.…”
Section: Revising the 1-loopmentioning
confidence: 99%
“…The other two seesaw variants have received much less attention. The LFV phenomenology of the SUSY type-II seesaw has been considered in [60,[76][77][78][79][80][81], whereas the SUSY type-III seesaw has been studied in [82][83][84]. More recently, the interplay between the Higgs mass constraint and LFV was studied in [62] for the three seesaw variants.…”
Section: Standard High-scale Seesaw Scenariosmentioning
confidence: 99%
“…In this case, the large mixing of neutrino families required by the data also implies that charged LFV may occur at enhanced rates for sufficiently small JHEP09(2020)197 soft supersymmetry-breaking masses. This can occur in rare decays and conversions (e.g., µ → eγ and τ → µγ, µ → 3e, τ → eγ and µ − e conversion [22,23]), 1 but also in other processes such as sparticle production at the LHC [26][27][28][29][30][31][32][33][34][35][36] and slepton pair production at a Linear Collider (LC) [37][38][39][40][41][42][43][44][45], particularly in the decays of the second-lightest neutralino.…”
Section: Introductionmentioning
confidence: 99%