Phenomenology in the Zee model with the A{sub 4} symmetry
Journal Article
·
· Physical Review. D, Particles Fields
- Department of Physics and R-GIRO, Ritsumeikan University, Kusatsu, Shiga 525-8577 (Japan)
- The Abdus Salam ICTP of UNESCO and IAEA, Strada Costiera 11, 34151 Trieste (Italy)
The Zee model generates neutrino masses at the one-loop level by adding charged SU(2){sub L}-singlet and extra SU(2){sub L}-doublet scalars to the standard model of particle physics. We introduce the softly broken A{sub 4} symmetry to the Zee model as the origin of the nontrivial structure of the lepton flavor mixing. This model is compatible with the tribimaximal mixing which agrees well with neutrino oscillation measurements. Then, a sum rule m{sub 1}e{sup i{alpha}{sub 12}}+2m{sub 2}+3m{sub 3}e{sup i{alpha}{sub 32}}=0 is obtained and it results in {Delta}m{sub 31}{sup 2}<0 and m{sub 3}{>=}1.8x10{sup -2} eV. The effective mass |(M{sub {nu}}){sub ee}| for the neutrinoless double beta decay is predicted as |(M{sub {nu}}){sub ee}|{>=}1.7x10{sup -2} eV. The characteristic particles in this model are SU(2){sub L}-singlet charged Higgs bosons s{sub {alpha}}{sup +}({alpha}={xi},{eta},{zeta}) which are made from a 3 representation of A{sub 4}. Contributions of s{sub {alpha}}{sup {+-}} to the lepton flavor violating decays of charged leptons are almost forbidden by an approximately remaining Z{sub 3} symmetry; only BR({tau}{yields}{bar e}{mu}{mu}) can be sizable by the flavor changing neutral current interaction with SU(2){sub L}-doublet scalars. Therefore, s{sub {alpha}}{sup {+-}} can easily be light enough to be discovered at the LHC with satisfying current constraints. The flavor structures of BR(s{sub {alpha}}{sup -}{yields}l{nu}) are also discussed.
- OSTI ID:
- 21537474
- Journal Information:
- Physical Review. D, Particles Fields, Journal Name: Physical Review. D, Particles Fields Journal Issue: 5 Vol. 83; ISSN PRVDAQ; ISSN 0556-2821
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
ACCELERATORS
BETA DECAY
BETA-MINUS DECAY
BOSONS
CERN LHC
COMPOSITE MODELS
CYCLIC ACCELERATORS
DECAY
DOUBLE BETA DECAY
EFFECTIVE MASS
ELEMENTARY PARTICLES
EQUATIONS
FERMIONS
FIELD THEORIES
FLAVOR MODEL
GRAND UNIFIED THEORY
HIGGS BOSONS
INTERACTIONS
LEPTONS
LIE GROUPS
MASS
MASSLESS PARTICLES
MATHEMATICAL MODELS
NEUTRAL-CURRENT INTERACTIONS
NEUTRINO OSCILLATION
NEUTRINOS
NUCLEAR DECAY
PARTICLE DECAY
PARTICLE INTERACTIONS
PARTICLE MODELS
POSTULATED PARTICLES
QUANTUM FIELD THEORY
QUARK MODEL
STANDARD MODEL
STORAGE RINGS
SU GROUPS
SU-2 GROUPS
SUM RULES
SYMMETRY BREAKING
SYMMETRY GROUPS
SYNCHROTRONS
UNIFIED GAUGE MODELS
ACCELERATORS
BETA DECAY
BETA-MINUS DECAY
BOSONS
CERN LHC
COMPOSITE MODELS
CYCLIC ACCELERATORS
DECAY
DOUBLE BETA DECAY
EFFECTIVE MASS
ELEMENTARY PARTICLES
EQUATIONS
FERMIONS
FIELD THEORIES
FLAVOR MODEL
GRAND UNIFIED THEORY
HIGGS BOSONS
INTERACTIONS
LEPTONS
LIE GROUPS
MASS
MASSLESS PARTICLES
MATHEMATICAL MODELS
NEUTRAL-CURRENT INTERACTIONS
NEUTRINO OSCILLATION
NEUTRINOS
NUCLEAR DECAY
PARTICLE DECAY
PARTICLE INTERACTIONS
PARTICLE MODELS
POSTULATED PARTICLES
QUANTUM FIELD THEORY
QUARK MODEL
STANDARD MODEL
STORAGE RINGS
SU GROUPS
SU-2 GROUPS
SUM RULES
SYMMETRY BREAKING
SYMMETRY GROUPS
SYNCHROTRONS
UNIFIED GAUGE MODELS