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S3 as a flavour symmetry for quarks and leptons after the Daya Bay result on \theta 13
High Energy Physics - Phenomenology · Submitted 14 Mar 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We present a model based on the flavour group S3 X Z3 X Z6 to explain the main features of fermion masses and mixing.
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The abstract, sentence by sentence
We present a model based on the flavour group S3 X Z3 X Z6 to explain the main features of fermion masses and mixing. In particular, in the neutrino sector the breaking of the S3 symmetry is responsible for a naturally small r=\Delta m^2_sol/\Delta m^2_atm and suitable next-to-leading order corrections bring \theta 13 at the level of ~ 0.13, fully compatible with the recent Daya Bay result. In the quark sector, the model accommodates the different mass hierarchies in the up and down quark sectors as well as the Cabibbo angle and Vcb (or Vub, depending on the charge assignment of the right-handed b-quark) in the correct range.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present a model based on the flavour group S3 X Z3 X Z6 to explain the main features of fermion masses and mixing. | contribution 0.90 | 0.91 | 0.21 | asserted 1.00 |
| s1 | In particular, in the neutrino sector the breaking of the S3 symmetry is responsible for a naturally small r=\Delta m^2_sol/\Delta m^2_atm and suitable next-to-leading order corrections bring \theta 13 at the level of ~ 0.13, fully compatible with the recent Daya Bay result. | result 0.95 | 0.85 | 0.44 | asserted 0.96 |
| s2 | In the quark sector, the model accommodates the different mass hierarchies in the up and down quark sectors as well as the Cabibbo angle and Vcb (or Vub, depending on the charge assignment of the right-handed b-quark) in the correct range. | result 0.93 | 0.79 | 0.12 | asserted 0.90 |
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The paper
Original abstract
We present a model based on the flavour group S3 X Z3 X Z6 to explain the main features of fermion masses and mixing. In particular, in the neutrino sector the breaking of the S3 symmetry is responsible for a naturally small r=\Delta m^2_sol/\Delta m^2_atm and suitable next-to-leading order corrections bring \theta 13 at the level of ~ 0.13, fully compatible with the recent Daya Bay result. In the quark sector, the model accommodates the different mass hierarchies in the up and down quark sectors as well as the Cabibbo angle and Vcb (or Vub, depending on the charge assignment of the right-handed b-quark) in the correct range.
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References
How the literature uses it
22 arXiv papers cite this in 24 sentences
Papers citing it · 9 sentences without a confident label
Cites it as background 15 papers
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As a result of the rapidly changing landscape of neutrino mixing parameters, many models based on discrete family symmetry (see [ref] and references therein) which were proposed initially to account for TB mixing are now either excluded, or have been subjected to modification [ref] .
A Grand Delta(96) x SU(5) Flavour Model · Introduction · 0.87
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singlet under $S_3$ [ref] .
Quark sector of S3 models: classification and comparison with experimental data · Introduction · 0.81
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As it is well known, in several extended models with three Higgs doblets (3HD) and the $𝐒_3$ flavor symmetry [ The $S_3$ flavor symmetry has been studied exhaustively in different frameworks [ref] .
A comparative study between the modified Fritzsch and nearest neighbor interaction textures · Quark Mass Matrix · 0.97
What it cites · 10 sentences without a confident label
Contests 2 papers
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In [ref] it has been suggested to introduce a further symmetry under which $x_1 = -x_2$ and $v_ϕ= v_χ$; however, as pointed out in [ref] , this additional symmetry does not commute with $S_3$ and the whole symmetry group is larger than the latter.
Fermion Mass Hierarchies and Flavour Mixing from a Minimal Discrete Symmetry · Charged leptons · contest 0.74
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In [ref] it has been suggested to introduce a further symmetry under which $x_1 = -x_2$ and $v_ϕ= v_χ$; however, as pointed out in [ref] , this additional symmetry does not commute with $S_3$ and the whole symmetry group is larger than the latter.
A discrete symmetry group for maximal atmospheric neutrino mixing · Charged leptons · contest 0.74
Uses data or values from 1 paper
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In these plots, the horizontal gray bands are the regions excluded by the experimental data at 3$σ$, as obtained from the second reference in [ref] .
Evidence of theta(13)>0 from global neutrino data analysis · Numerical analysis of the lepton sector · 0.82
Cites as background 3 papers
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Discrete symmetries [ref] have been invoked as a powerful tool to solve/mitigate some of these problems and, among several choices, the non-abelian discrete group $S_3$ [ref] has also been investigated.
Discrete Flavor Symmetries and Models of Neutrino Mixing · Introduction · 0.92
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Interesting attempts in this direction have been done in the context of GUT theories [ref] and in a non-unified approach [ref] - [ref] .
Fermion Mass Hierarchies and Flavour Mixing from a Minimal Discrete Symmetry · Introduction · 0.80
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Interesting attempts in this direction have been done in the context of GUT theories [ref] and in a non-unified approach [ref] - [ref] .
Broken S_3 Flavor Symmetry of Leptons and Quarks: Mass Spectra and Flavor Mixing Patterns · Introduction · 0.80
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