Search results for "Yukawa [coupling]"

showing 10 items of 110 documents

Collective mass parameters and linear response techniques in three-dimensional grids

1984

We discuss four prescriptions for evaluating a collective mass parameter suitable for translations, rotations and large amplitude collective motions. These are the adiabatic time dependent Hartree-Fock theory (ATDHF) and the generator coordinate method (GCM), both with and without curvature corrections. As practical example we consider the16O+16O collision using a recently developed density dependent interaction with direct Yukawa and Coulomb terms. We present a fast iteration scheme for solving the linear response equation in a three-dimensional coordinate or momentum space grid. As test cases we consider the rotational and translational inertia parameters for various distances between the…

PhysicsNuclear and High Energy PhysicsClassical mechanicsAmplitudemedia_common.quotation_subjectYukawa potentialCoulombPosition and momentum spaceAdiabatic processInertiaCurvatureRotation (mathematics)media_commonZeitschrift f�r Physik A Atoms and Nuclei
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NEUTRINO SPECTRUM IN NONSUPERSYMMETRIC SO(10)

1996

We present a predictive scheme for fermion masses and mixings inspired by nonsupersymmetric SO(10) in which the hierarchy problem is resolved without fine tuning the Yukawa couplings. This calls for a nonminimal Higgs sector which we exploit in deriving the expressions for the mass matrices. To keep the predictivity of the model under control we limit the structure of the mass matrices by imposing U(1) symmetries. A very predictive neutrino spectrum is then obtained.

PhysicsNuclear and High Energy PhysicsFine-tuningParticle physicsHigh Energy Physics::PhenomenologyYukawa potentialGeneral Physics and AstronomyAstronomy and AstrophysicsHierarchy problemFermionHiggs sectorLimit (mathematics)NeutrinoSO(10)Modern Physics Letters A
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A theory for scotogenic dark matter stabilised by residual gauge symmetry

2020

Dark matter stability can result from a residual matter-parity symmetry, following naturally from the spontaneous breaking of the gauge symmetry. Here we explore this idea in the context of the $\mathrm{SU(3)_c \otimes SU(3)_L \otimes U(1)_X \otimes U(1)_{N}}$ electroweak extension of the standard model. The key feature of our new scotogenic dark matter theory is the use of a triplet scalar boson with anti-symmetric Yukawa couplings. This naturally implies that one of the light neutrinos is massless and, as a result, there is a lower bound for the $\rm 0\nu\beta\beta$ decay rate.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesScalar boson01 natural sciencesSymmetry (physics)lcsh:QC1-999Massless particleStandard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicslcsh:PhysicsGauge symmetry
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An A4 model for lepton masses and mixings

2009

We study an extension of the standard model based on the flavor symmetry A(4) only. Neutrino Majorana mass terms arise from a dimension five operator and charged lepton masses from renormalizable Yukawa couplings. We introduce three Higgs doublets that belong to one triplet irreducible representation of A(4). We study the most general A(4)-invariant scalar potential and the phenomenological consequences of the model. We find that the reactor angle could be as large as sin(2)theta(13max)similar to 0.03, while the atmospheric mixing angle theta(23) is close to maximal, sin(2)theta(23)=1/2.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDimension (graph theory)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesWeinberg angle7. Clean energy01 natural sciencesStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Irreducible representation0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsNeutrino oscillationParticle Physics - PhenomenologyLepton
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extended MSSM

2012

We investigate the perturbative regime of the Minimal Supersymmetric Con- formal Technicolor and show that it allows for a stable vacuum correctly breaking the electroweak symmetry. We nd that the particle spectrum is richer than the MSSM one since it features several new particles stemming out from the new N = 4 sector of the theory. The parameter space of the new theory is reduced imposing naturalness of the cou- plings and soft supersymmetry breaking masses, perturbativity of the model at the EW scale as well as phenomenological constraints. By studying the RGEs at two loops we nd that the Yukawa couplings of the heavy fermionic states

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionYukawa potentialConformal mapTechnicolorParameter space01 natural sciencesSupersymmetry breakingSymmetry (physics)Naturalness0103 physical sciences010306 general physicsNuclear Physics B
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Constraints on doubly charged Higgs interactions at linear collider

1996

Production of a single doubly charged Higgs boson $Delta^{--}$ in polarized $e^+e^-$ and $e^+\gamma$ collision modes of the linear collider have been investigated. The mass range of $Delta^{--}$ to be probed extends up to the collision energy. The diagonal lepton number violating Yukawa coupling $h_{ee}$ will be tested at least three orders of magnitude more strictly than in present experiments.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaCoupling (probability)01 natural sciencesLepton number3. Good healthlaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)law0103 physical sciencesHiggs bosonProduction (computer science)High Energy Physics::Experiment010306 general physicsColliderEnergy (signal processing)
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Minimal 3-loop neutrino mass models and charged lepton flavor violation

2020

We study charged lepton flavor violation for the three most popular 3-loop Majorana neutrino mass models. We call these models "minimal" since their particle content correspond to the minimal sets for which genuine 3-loop models can be constructed. In all the three minimal models the neutrino mass matrix is proportional to some powers of Standard Model lepton masses, providing additional suppression factors on top of the expected loop suppression. To correctly explain neutrino masses, therefore large Yukawa couplings are needed in these models. We calculate charged lepton flavor violating observables and find that the three minimal models survive the current constraints only in very narrow …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesObservableMinimal modelsMass matrix01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Beyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentNeutrino010306 general physicsLepton
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Flavor violation in supersymmetric SU(5) GUT at large tan beta

2001

We study flavor violation in the general SUSY SU(5) GUT assuming all the third generation Yukawa couplings to be due to the renormalizable physics above GUT scale. At large tan beta, as suggested by Yukawa unification in SU(5), sizable flavor violation in the left (right) slepton (down squark) sector can be induced in nonminimal models due to renormalization effects of down type Yukawa couplings between GUT and Planck scales, in addition to the flavor violation in the right slepton sector. The new flavor physics contribution to K-(K) over bar, B-(B) over bar mixing is small but might be of phenomenological interest in the case of b --> s gamma. The sign of the latter contribution is the sam…

PhysicsNuclear and High Energy PhysicsParticle physicsBranching fractionHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFísicaElementary particleSupersymmetryRenormalizationCharginoHigh Energy Physics::ExperimentLepton
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CKM matrix and fermion masses in the dualized standard model

1997

A Dualized Standard Model recently proposed affords a natural explanation for the existence of Higgs fields and of exactly 3 generations of fermions, while giving at the same time the observed fermion mass hierarchy together with a tree-level CKM matrix equal to the identity matrix. It further suggests a method for generating from loop corrections the lower generation masses and nondiagonal CKM matrix elements. In this paper, the proposed calculation is carried out to 1-loop. It is found first that with the method suggested one can account readily for the masses of the second generation fermions as a `leakage' from the highest generation. Then, with the Yukawa couplings fixed by fitting the…

PhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixElectroweak interactionHigh Energy Physics::PhenomenologyIdentity matrixYukawa potentialFOS: Physical sciencesFísicaFermionHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Higgs bosonFree parameter
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Neutral heavy leptons and electroweak baryogenesis

1996

We investigate the possibility that baryogenesis occurs during the weak phase transition in a minimal extension of the Standard Model which contains extra neutral leptons and conserves total lepton number. The necessary CP-violating phases appear in the leptonic Yukawa couplings. We compute the CP-asymmetries in both the neutral and the charged lepton fluxes reflected on the bubble wall. Using present experimental bounds on the mixing angles and Standard Model estimates for the parameters related to the scalar potential, we conclude that it seems unlikely to produce the observed baryon to entropy ratio within this type of models. We comment on the possibility that the constraints on the mix…

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaScalar potentialLepton numberStandard ModelBaryonBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentParticle Physics - PhenomenologyLepton
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