2014
DOI: 10.1007/jhep08(2014)019
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Fermion EDMs with minimal flavor violation

Abstract: Abstract:We study the electric dipole moments (EDMs) of fermions in the standard model supplemented with right-handed neutrinos and its extension including the neutrino seesaw mechanism under the framework of minimal flavor violation (MFV). In the quark sector, we find that the current experimental bound on the neutron EDM does not yield a significant restriction on the scale of MFV. In addition, we consider how MFV may affect the contribution of the strong theta-term to the neutron EDM. For the leptons, the e… Show more

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Cited by 19 publications
(15 citation statements)
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“…(2.9) complex due to imaginary parts among the traces of the matrix products A i B j A k · · · . Such imaginary contributions turn out to be small [29][30][31][32], and so hereafter we ignore Im ξ r .…”
Section: Jhep04(2015)174mentioning
confidence: 99%
See 1 more Smart Citation
“…(2.9) complex due to imaginary parts among the traces of the matrix products A i B j A k · · · . Such imaginary contributions turn out to be small [29][30][31][32], and so hereafter we ignore Im ξ r .…”
Section: Jhep04(2015)174mentioning
confidence: 99%
“…(2.8), and so A can have much greater elements if the right-handed neutrinos' mass M in M ν is sufficiently large. Since as an infinite series ∆ has to converge, M cannot be arbitrarily large [29][30][31][32]. Accordingly, we require the largest eigenvalue of A to be unity, which implies that the elements of B = Y e Y † e are small compared to those of A and that, consequently, we can drop most of the terms in eq.…”
Section: Jhep04(2015)174mentioning
confidence: 99%
“…To maximize the new-physics effects, we assume that the righthanded neutrinos' mass M is large enough to render the biggest eigenvalue of A equal to unity, which conforms to the perturbativity requirement [59,60,74,75]. Given that the eigenvalues of B are at most y 2 τ ∼ 1 × 10 −4 , we may consequently drop from ∆ all the terms with B, which would otherwise be needed in a study concerning CP violation [59][60][61]. Accordingly, the relevant building block is [61] …”
Section: Jhep09(2015)093mentioning
confidence: 99%
“…As Imξ 1,2,4 are tiny [59,60,74,75], we can further approximate ∆ † = ∆. One could then construct the desired G ℓ -invariant effective Lagrangians that are SM gauge singlet.…”
Section: Jhep09(2015)093mentioning
confidence: 99%
“…It should also be noted that several authors have recently considered the NEDM within frameworks beyond the SM;-see for instance refs. [23][24][25].…”
Section: Introductionmentioning
confidence: 99%