1982
DOI: 10.1103/physrevd.25.1895
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Permutation symmetries and the fermion mass matrix

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Cited by 150 publications
(60 citation statements)
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“…In some setups where the fermion transformations under S 3 are not appropriately adjusted, the off-diagonal Yukawa couplings may become order one which induce sizable neutral scalar mediated rare processes, like K L → µe or K L → 2π, at tree level. This requires those neutral scalars to lie beyond several TeV [6,11]. But in our case, once we adjust the f i /g u,d…”
Section: Scalar Couplings To Gauge and Matter Fieldsmentioning
confidence: 99%
“…In some setups where the fermion transformations under S 3 are not appropriately adjusted, the off-diagonal Yukawa couplings may become order one which induce sizable neutral scalar mediated rare processes, like K L → µe or K L → 2π, at tree level. This requires those neutral scalars to lie beyond several TeV [6,11]. But in our case, once we adjust the f i /g u,d…”
Section: Scalar Couplings To Gauge and Matter Fieldsmentioning
confidence: 99%
“…Obviously, the matrices in Eq. (66) correspond to the triplet representation. Thus, we can obtain their characters.…”
Section: Amentioning
confidence: 99%
“…The solution is obtained as (m 1 , m 2 , m 3 ) = (3, 0, 1). That is, the A 4 group has three singlets, 1, 1 ′ , and 1 ′′ , and a single triplet 3, where the triplet corresponds to (66).…”
Section: Amentioning
confidence: 99%
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“…On the other hand, much attention has been devoted to the question whether these models can be extended to describe the observed pattern of quark masses and mixing angles, and whether these can be made compatible with the SU(5) or SO(10) grand unified theory (GUT). The attractive candidate is the S 4 symmetry, which has been already used for the neutrino masses and the neutrino flavor mixing [74,75,76,77]. The exact tri-bimaximal neutrino mixing is realized in S 4 flavor models [78,79,80,81,82,83,84].…”
Section: Introductionmentioning
confidence: 99%