1998
DOI: 10.1142/9789812812667_0012
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Supersymmetry and FCNC Effects

Abstract: We consider Flavour Changing Neutral Current processes in the framework of the supersymmetric extension of the Standard Model. FCNC constraints on the structure of sfermion mass matrices are reviewed. Furthermore, we analyze supersymmetric contributions to FCNC transitions which remain in the limit of flavourconserving sfermion mass matrices. Implications of the FCNC constraints on the structure of sfermion mass matrices for SUSY breaking and sfermion mass generation are discussed. We conclude that the supersy… Show more

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Cited by 181 publications
(217 citation statements)
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References 33 publications
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“…We focus here on the H x → l klm channel, but due to the fact that we work with real parameters, the predictions for the CP -conjugate channel H x → l mlk will be equal. The present computation of Γ(H x → l klm ) is performed by taking into account the following assumptions and considerations: 1) The amplitude is evaluated at the one-loop level, 2) only loops containing sleptons and sneutrinos contribute since they are the only particles propagating the LFV by means of the ∆ AB mk entries with m = k, 3) the particle content assumed here is that of the MSSM, 4) the external particles h, H, A and l k ,l m are expressed in the physical mass basis, 5) the internal loop sparticles are expressed in the electroweak interaction basis, and 6) we use the Mass Insertion Approximation [49][50][51] to describe the propagation of slepton mixing changing flavor, and work in the linear approximation for each insertion ∆ AB mk , with AB = LL, RR, LR, RL, and m = k, i.e, considering one single insertion at a time.…”
Section: Analytic Results Of the Lfvhd Widths In The Miamentioning
confidence: 99%
See 1 more Smart Citation
“…We focus here on the H x → l klm channel, but due to the fact that we work with real parameters, the predictions for the CP -conjugate channel H x → l mlk will be equal. The present computation of Γ(H x → l klm ) is performed by taking into account the following assumptions and considerations: 1) The amplitude is evaluated at the one-loop level, 2) only loops containing sleptons and sneutrinos contribute since they are the only particles propagating the LFV by means of the ∆ AB mk entries with m = k, 3) the particle content assumed here is that of the MSSM, 4) the external particles h, H, A and l k ,l m are expressed in the physical mass basis, 5) the internal loop sparticles are expressed in the electroweak interaction basis, and 6) we use the Mass Insertion Approximation [49][50][51] to describe the propagation of slepton mixing changing flavor, and work in the linear approximation for each insertion ∆ AB mk , with AB = LL, RR, LR, RL, and m = k, i.e, considering one single insertion at a time.…”
Section: Analytic Results Of the Lfvhd Widths In The Miamentioning
confidence: 99%
“…These mixings are parametrized by means of a complete set of slepton flavor mixing dimensionless parameters, δ AB mk with AB = LL, RR, LR, RL, and flavor indices m, k = 1, 2, 3, with m = k. These parameters take into account, in a model-independent way and without any assumption on their particular origin, all the possible flavor mixings among the SUSY partners of the leptons with either left-handed or right-handed chirality. The novelty of this new computation is that we use a different technique, the so-called Mass Insertion Approximation (MIA) [49][50][51], that works with sleptons in the electroweak basis instead…”
Section: Jhep03(2016)055mentioning
confidence: 99%
“…Specific assumptions on the flavor structure of NP correspond to special choices of the F i functions. For example Minimal Flavor Violation (MFV) models [20]- [25] correspond to F 1 = F SM and F i =1 = 0. Following ref.…”
Section: Jhep03(2013)089mentioning
confidence: 99%
“…We give all the expressions already in the super-KM basis (see e.g. [11] for a more detailed discussion).…”
Section: Su(2)-doublets)mentioning
confidence: 99%
“…Using the notation of this Appendix, one can list (in the mass eigenstate basis) the Feynman rules necessary to calculate cross sections (3), (11) and ( 2) Interactions of charginos and neutralinos with gauge bosons:…”
Section: Su(2)-doublets)mentioning
confidence: 99%