Search results for "Gauge Symmetry"

showing 10 items of 54 documents

Measurement of trilinear gauge boson couplings fromWW+WZ→lνjjevents inpp¯collisions ats=1.96  TeV

2009

We present a direct measurement of trilinear gauge boson couplings at gamma WW and ZWW vertices inWW and WZ events produced in p (p) over bar collisions at root s = 1:96 TeV. We consider events with one electron or muon, missing transverse energy, and at least two jets. The data were collected using the D0 detector and correspond to 1:1 fb(-1) of integrated luminosity. Considering two different relations between the couplings at the gamma WW and ZWW vertices, we measure these couplings at 68% C.L. to be kappa(gamma) = 1.07(-0.29)(+0.26) lambda = 0.00(-0.06)(+0.00), and g(1)(Z) = 1.04(-0.09)(+0.09) in a scenario respecting SU(2)(L) circle times U(1)(Y) gauge symmetry and kappa = 1.04(-0.11)(…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsMuonLuminosity (scattering theory)010308 nuclear & particles physicsLambda01 natural sciencesSymmetry (physics)Nuclear physics0103 physical sciencesHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsGauge theory010306 general physicsGauge symmetryBosonPhysical Review D
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Fading of symmetry nonrestoration at finite temperature

1998

The fate of symmetries at high temperature determines the dynamics of the very early universe. It is conceivable that temperature effects favor symmetry breaking instead of restoration. Concerning global symmetries, the non-linear sigma model is analyzed in detail. For spontaneously broken gauge symmetries, we propose the gauge boson magnetic mass as a ``flag'' for symmetry (non)-restoration. We consider several cases: the standard model with one and two Higgs doublets in the perturbative regime, and the case of a strongly interacting Higgs sector. The latter is done in a model independent way with the tools provided by chiral Lagrangians. Our results clearly point towards restoration, a pa…

PhysicsNuclear and High Energy PhysicsGauge bosonSpontaneous symmetry breakingHigh Energy Physics::LatticeAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstrophysicsHiggs sectorTheoretical physicsHiggs fieldHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsHiggs bosonSymmetry breakingGauge theoryGauge symmetry
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GAUGE-HIGGS UNIFICATION MODELS WITH COSET SPACE DIMENSIONAL REDUCTION SCHEME

2009

We investigate the gauge-Higgs unification models within the scheme of the coset space dimensional reduction, beginning with two types of set up; fourteen-dimensional gauge theory with simple gauge groups and ten-dimensional gauge theory with direct product gauge groups. We found some phenomenologically acceptable models through an exhaustive search for the candidates of the coset spaces, the gauge group in higher dimension, and fermion representation.

PhysicsNuclear and High Energy PhysicsIntroduction to gauge theoryQuantum gauge theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsAtomic and Molecular Physics and OpticsBRST quantizationHigh Energy Physics::TheoryTheoretical physicsHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theoryQuantum electrodynamicsGauge anomalyGauge symmetryInternational Journal of Modern Physics 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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Hefty MSSM-like light Higgs in extended gauge models

2011

It is well known that in the MSSM the lightest neutral Higgs h^0 must be, at the tree level, lighter than the Z boson and that the loop corrections shift this stringent upper bound up to about 130 GeV. Extending the MSSM gauge group in a suitable way, the new Higgs sector dynamics can push the tree-level mass of h^0 well above the tree-level MSSM limit if it couples to the new gauge sector. This effect is further pronounced at the loop level and h^0 masses in the 140 GeV ballpark can be reached easily. We exemplify this for a sample setting with a low-scale U(1)_R x U(1)_B-L gauge symmetry in which neutrino masses can be implemented via the inverse seesaw mechanism.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGauge (firearms)01 natural sciencesUpper and lower boundsHiggs sectorHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Gauge group0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsGauge symmetry
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Phenomenology of fermion dark matter as neutrino mass mediator with gauged B-L

2021

We analyze a model with unbroken B-L gauge symmetry where neutrino masses are generated at one loop, after spontaneous breaking of a global U(1) symmetry. These symmetries ensure dark matter stability and the Diracness of neutrinos. Within this context, we examine fermionic dark matter. Consistency between the required neutrino mass and the observed relic abundance indicates dark matter masses and couplings within the reach of direct detection experiments.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)FermionAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesSymmetry (physics)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceNeutrino010306 general physicsPhenomenology (particle physics)Gauge symmetryPhysics Letters
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Scotogenic dark matter stability from gauged matter parity

2019

We explore the idea that dark matter stability results from the presence of a matter-parity symmetry, arising naturally as a consequence of the spontaneous breaking of an extended $\mathrm{SU(3) \otimes SU(3)_L \otimes U(1)_X \otimes U(1)_{N}}$ electroweak gauge symmetry with fully gauged B-L. Using this framework we construct a theory for scotogenic dark matter and analyze its main features.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSpontaneous symmetry breakingDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesParity (physics)Stability result01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicslcsh:PhysicsGauge symmetryPhysics Letters
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Observable Majoron emission in neutrinoless double beta decay

1992

We consider a class of simplest Majoron models where neutrino- majoron couplings can be in the range $g \sim 10^{-5}-10^{-3}$ leading to the observability of neutrinoless double beta decay with majoron emission. The majoron is a singlet of the electroweak gauge symmetry, thus avoiding conflict with the LEP data on Z decay, which rules out the triplet and doublet majoron models.

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHigh Energy Physics::ExperimentSinglet stateNeutrinoNuclear ExperimentMajoronGauge symmetry
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Sparticle Mass Spectra from SO(10) Grand Unified Models with Yukawa Coupling Unification

1999

We examine the spectrum of superparticles obtained from the minimal SO(10) grand unified model, where it is assumed the gauge symmetry breaking yields the Minimal Supersymmetric Standard Model (MSSM) as the effective theory at $M_{GUT}\sim 2\times 10^{16}$ GeV. In this model, unification of Yukawa couplings implies a value of $\tan\beta\sim 45-55$. At such high values of $\tan\beta$, assuming universality of scalar masses, the usual mechanism of radiative electroweak symmetry breaking breaks down. We show that a set of weak scale sparticle masses consistent with radiative electroweak symmetry breaking can be generated by imposing non-universal GUT scale scalar masses consistent with univers…

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesSupersymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Effective field theoryHigh Energy Physics::ExperimentSymmetry breakingSO(10)Minimal Supersymmetric Standard ModelGauge symmetry
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Lepton flavour violation in a left-right symmetric model

1997

We consider in this paper a Left-Right symmetric gauge model in which a global lepton-number-like symmetry is introduced and broken spontaneously at a scale that could be as low as 10^4 GeV or so. The corresponding physical Nambu-Goldstone boson, which we call majoron and denote J, can have tree-level flavour-violating couplings to the charged fermions, leading to sizeable majoron-emitting lepton-flavour-violating weak decays. We consider explicitly a leptonic variant of the model and show that the branching ratios for \mu -> e+J, \tau -> e + J and \tau -> \mu + J decays can be large enough to fall within the sensitivities of future \mu and \tau factories. On the other hand the left-right g…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologySymmetric modelFOS: Physical sciencesFísicaFermionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentMajoronGauge symmetryLeptonBoson
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