2007
DOI: 10.1142/s0217751x07036865
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LIMITS ON THE ELECTROMAGNETIC AND WEAK DIPOLE MOMENTS OF THE TAU-LEPTON IN E6 SUPERSTRING MODELS

Abstract: We obtain limits on the electromagnetic and weak dipole moments of the tau-lepton in the framework of a Left-Right symmetric model (LRSM) and a class of E 6 inspired models with an additional neutral vector boson Z θ . Using as an input the data obtained by the L3 and OPAL Collaborations for the reaction e + e − → τ + τ − γ, we get a stringent limit on the LRSM mixing angle φ, −1.66 × 10 −3 < φ < 1.22 × 10 −3 , which in turn induces bounds on the tau weak dipole moments which are consistent with the bounds obt… Show more

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Cited by 35 publications
(31 citation statements)
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“…An important feature of E 6 inspired SUSY models is that the mass of the lightest Higgs particle can be substantially larger in these scenarios than in the MSSM and NMSSM [24]. Previously, the implications of E 6 inspired SUSY models with an additional Uð1Þ 0 gauge symmetry have been studied for EWSB [21][22][23][24], neutrino physics [25,26], leptogenesis [27,28], EW baryogenesis [29], muon anomalous magnetic moment [30], electric dipole moment of electron [31] and tau lepton [32], lepton flavor violating processes like ! e [33] and CP violation in the Higgs sector [34].…”
Section: Introductionmentioning
confidence: 99%
“…An important feature of E 6 inspired SUSY models is that the mass of the lightest Higgs particle can be substantially larger in these scenarios than in the MSSM and NMSSM [24]. Previously, the implications of E 6 inspired SUSY models with an additional Uð1Þ 0 gauge symmetry have been studied for EWSB [21][22][23][24], neutrino physics [25,26], leptogenesis [27,28], EW baryogenesis [29], muon anomalous magnetic moment [30], electric dipole moment of electron [31] and tau lepton [32], lepton flavor violating processes like ! e [33] and CP violation in the Higgs sector [34].…”
Section: Introductionmentioning
confidence: 99%
“…Recently, the latest Tevatron and early LHC Z ′ mass limits in these models have been discussed in [9] while different aspects of phenomenology of exotic quarks and squarks have been considered in [10]. Also the implications of the E 6 inspired SUSY models have been studied for EW symmetry breaking (EWSB) [11]- [14], neutrino physics [15]- [16], leptogenesis [17]- [18], EW baryogenesis [19], muon anomalous magnetic moment [20], electric dipole moment of electron [21] and tau lepton [22], lepton flavour violating processes like µ → eγ [23] and CP-violation in the Higgs sector [24]. The neutralino sector in E 6 inspired SUSY models was analysed previously in [13], [21]- [23], [25]- [29].…”
mentioning
confidence: 99%
“…Previously, the implications of E 6 inspired SUSY models with an additional U(1) gauge symmetry have been studied for electroweak symmetry breaking (EWSB) [31][32][33][34][35][36][37], neutrino physics [38,39], leptogenesis [40,41], electroweak (EW) baryogenesis [42,43], the muon anomalous magnetic moment [44,45], the electric dipole moment of the electron [46] and of the tau lepton [47], for lepton flavor violating processes like µ → eγ [48] and for CP-violation in the Higgs sector [49]. The neutralino sector in E 6 inspired SUSY models was analysed in [36,[46][47][48][50][51][52][53][54][55][56][57]. Such models have also been proposed as the solution to the tachyon problems of anomaly-mediated SUSY breaking, via U(1) D-term contributions [58], and have been used in combination with a generation symmetry to construct a model explaining the fermion mass hierarchy and mixing [59].…”
Section: Jhep01(2015)153mentioning
confidence: 99%