Search results for "HIGGS"

showing 10 items of 1127 documents

Radiative Corrections to Scalar Masses and Mixing in a Scale Invariant Two Higgs Doublet Model

2012

We study the Higgs-boson mass spectrum of a classical scale-invariant realization of the two-Higgs-doublet model (SI-2HDM). The classical scale symmetry of the theory is explicitly broken by quantum loop effects due to gauge interactions, Higgs self-couplings and top-quark Yukawa couplings. We determine the allowed parameter space compatible with perturbative unitarity and electroweak precision data. Taking into account the LEP and the recent LHC exclusion limits on a Standard-Model-like Higgs boson H_SM, we obtain rather strict constraints on the mass spectrum of the heavy Higgs sector of the SI-2HDM. In particular, if M_{H_SM} \sim 125 GeV, the SI-2HDM strongly favours scenarios, in which…

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorHiggs sectorStandard ModelHiggs fieldTwo-Higgs-doublet modelsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonsymbolsHigh Energy Physics::ExperimentHiggs mechanism
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Doubly charged Higgs at LHC

1996

We have investigated production of doubly charged Higgs particles $\Delta_{L,R}^{++}$ via WW fusion process in proton-proton collisions at LHC energies in the framework of the left-right symmetric model. The production cross section of the right-triplet Higgs is for representative values of model parameters at femtobarn level. The discovery reach depends on the mass of the right-handed gauge boson W_R. At best $\Delta_R^{++}$ mass up to 2.4 TeV are achievable within one year run. For $\Delta^{++}_L$ the corresponding limit is 1.75 TeV which depends on the value of the left-triplet vev v_L. Comparison with Drell-Yan pair production processes shows that studies of the WW fusion processes exte…

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonLarge Hadron ColliderMissing energy010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciences7. Clean energy01 natural sciencesLepton numberStandard ModelHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLepton
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Dynamical left-right symmetry breaking.

1995

We study a left--right symmetric model which contains only elementary gauge boson and fermion fields and no scalars. The phenomenologically required symmetry breaking emerges dynamically leading to a composite Higgs sector with a renormalizable effective Lagrangian. We discuss the pattern of symmetry breaking and phenomenological consequences of this scenario. It is shown that a viable top quark mass can be achieved for the ratio of the VEVs of the bi--doublet $\tan\beta\equiv\kappa/\kappa'$ =~ 1.3--4. For a theoretically plausible choice of the parameters the right--handed scale can be as low as $\sim 20 TeV$; in this case one expects several intermediate and low--scale scalars in addition…

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonSpontaneous symmetry breakingHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesHiggs sectorStandard ModelHiggs fieldExplicit symmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentSymmetry breakingPhysical review. D, Particles and fields
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Gauge- and renormalization-group-invariant formulation of the Higgs-boson resonance

1997

A gauge- and renormalization-group- invariant approach implemented by the pinch technique is formulated for resonant transitions involving the Higgs boson. The lineshape of the Higgs boson is shown to consist of two distinct and physically meaningful contributions: a process-independent resonant part and a process-dependent non-resonant background, which are separately gauge independent, invariant under the renormalization group, satisfy naive, tree-level Ward identities, and respect the optical and equivalence theorem individually. The former process-independent quantity serves as the natural extension of the concept of the effective charge to the case of the Higgs scalar, and constitutes …

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonUnitarityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaInvariant (physics)Renormalization groupRenormalizationHiggs fieldTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonBibliographyParticle Physics - Phenomenology
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Elimination of unitarily nonequivalent vacua in supersymmetric grand unified theories by gravity

1983

Abstract In globally supersymmetric grand unified theories, there may be unitarily nonequivalent vacua which are not present in ordinary theories, reflecting the invariance of the Higgs potential under the complex extension of the gauge group. We show that such vacua are eliminated in the presence of N = 1 supergravity coupling, if local supersymmetry is broken and the costomological constant vanishes.

PhysicsNuclear and High Energy PhysicsParticle physicsGravity (chemistry)SupergravityHigh Energy Physics::PhenomenologyDoublet–triplet splitting problemSupersymmetryCoupling (probability)General Relativity and Quantum CosmologyHigh Energy Physics::TheoryTheoretical physicsGauge groupHiggs bosonConstant (mathematics)Physics Letters B
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Electric Dipole Moments in Two-Higgs-Doublet Models

2014

Electric dipole moments are extremely sensitive probes for additional sources of CP violation in new physics models. Specifically, they have been argued in the past to exclude new CP-violating phases in two-Higgs-doublet models. Since recently models including such phases have been discussed widely, we revisit the available constraints in the presence of mechanisms which are typically invoked to evade flavour-changing neutral currents. To that aim, we start by assessing the necessary calculations on the hadronic, nuclear and atomic/molecular level, deriving expressions with conservative error estimates. Their phenomenological analysis in the context of two-Higgs-doublet models yields strong…

PhysicsNuclear and High Energy PhysicsParticle physicsHiggs PhysicsAtomic Physics (physics.atom-ph)Physics beyond the Standard ModelHadronHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesContext (language use)ObservableBeyond Standard Model; CP violation; Higgs Physics; High Energy Physics - Phenomenology; High Energy Physics - Phenomenology; High Energy Physics - Experiment; Physics - Atomic Physics; Nuclear and High Energy PhysicsHigh Energy Physics - ExperimentPhysics - Atomic PhysicsHigh Energy Physics - PhenomenologyDipoleHigh Energy Physics - Experiment (hep-ex)CP violationHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonCP violationSensitivity (control systems)
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A realistic model of neutrino masses with a large neutrinoless double beta decay rate

2011

The minimal Standard Model extension with the Weinberg operator does accommodate the observed neutrino masses and mixing, but predicts a neutrinoless double beta ($0\nu\beta\beta$) decay rate proportional to the effective electron neutrino mass, which can be then arbitrarily small within present experimental limits. However, in general $0\nu\beta\beta$ decay can have an independent origin and be near its present experimental bound; whereas neutrino masses are generated radiatively, contributing negligibly to $0\nu\beta\beta$ decay. We provide a realization of this scenario in a simple, well defined and testable model, with potential LHC effects and calculable neutrino masses, whose two-loop…

PhysicsNuclear and High Energy PhysicsParticle physicsHiggs PhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesType (model theory)Quantum numberPartícules (Física nuclear)Neutrino physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Standard-Model ExtensionDouble beta decayBeyond Standard ModelHigh Energy Physics::ExperimentConnection (algebraic framework)NeutrinoElectron neutrinoLepton
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Status and implications of neutrino masses: a brief panorama

2015

15 pages.- 10 figures

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeElectroweak interactionDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsFlavor symmetryAstrophysics::Cosmology and Extragalactic AstrophysicsAtomic and Molecular Physics and OpticsCosmologyNeutrino mixing and oscillationsHigh Energy Physics - PhenomenologyQuark-lepton unificationHigh Energy Physics - Phenomenology (hep-ph)Double beta decayHiggs bosonCP violationSeesaw mechanismHigh Energy Physics::ExperimentNeutrinoLepton
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Limits on associated production of visibly and invisibly decaying Higgs bosons from Z decays

1994

Many extensions of the standard electroweak model Higgs sector suggest that the main Higgs decay channel is "invisible", for example, $h \to J J$ where $J$ denotes the majoron, a weakly interacting pseudoscalar Goldstone boson associated to the spontaneous violation of lepton number. In many of these models the Higgs boson may also be produced in association to a massive pseudoscalar boson (HA), in addition to the standard Bjorken mechanism (HZ). We describe a general strategy to determine limits from LEP data on the masses and couplings of such Higgs bosons, using the existing data on acoplanar dijet events as well as data on four and six $b$ jet event topologies. For the sake of illustrat…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberHiggs sectorPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonHiggs bosonHigh Energy Physics::ExperimentMajoronBoson
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The Case of a WW Dynamical Scalar Resonance within a Chiral Effective Description of the Strongly Interacting Higgs Sector

1999

We have studied the strongly interacting $W_L W_L \to W_L W_L$ I=L=0 partial wave amplitude making use of effective chiral Lagrangians. The Higgs boson is explicitly included and the N/D method is used to unitarize the amplitude. We recover the chiral perturbative expansion at next to leading order for low energies. The cases $m_H<< 4��v$ and $m_H>> 4 ��v$ are considered in detail. It is shown that in the latter situation a state appears with a mass $\lesssim 1$ TeV. This state is dynamically generated through the strong interactions between the $W_L$ and is not responsible for the spontaneous electroweak symmetry breaking. However, its shape can be very similar to that of the $…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeScalar (mathematics)Electroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Resonance (particle physics)Higgs sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeHiggs bosonHigh Energy Physics::ExperimentSymmetry breaking
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