Search results for "Boson"

showing 10 items of 1360 documents

Probing long-range leptonic forces with solar and reactor neutrinos

2006

In this work we study the phenomenological consequences of the existence of long-range forces coupled to lepton flavour numbers in solar neutrino oscillations. We study electronic forces mediated by scalar, vector or tensor neutral bosons and analyze their effect on the propagation of solar neutrinos as a function of the force strength and range. Under the assumption of one mass scale dominance, we perform a global analysis of solar and KamLAND neutrino data which depends on the two standard oscillation parameters, \Delta m^2_{21} and \tan^2\theta_{12}, the force coupling constant, its range and, for the case of scalar-mediated interactions, on the neutrino mass scale as well. We find that,…

Coupling constantPhysicsParticle physics010308 nuclear & particles physicsOscillationSolar neutrinoHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesAstronomy and Astrophysics7. Clean energy01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentTensorNeutrino010306 general physicsLeptonBosonJournal of Cosmology and Astroparticle Physics
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Radiatively Induced Neutrino Masses and Large Higgs-Neutrino Couplings in the Standard Model with Majorana Fields

1999

The Higgs sector of the Standard Model with one right-handed neutrino per family is systematically analyzed. In a model with intergenerational independent mixings between families, we can account for very light neutrinos acquiring Majorana masses radiatively at the first electroweak loop level. We also find that in such a scenario the Higgs coupling to the light-heavy neutrinos and to the heavy-heavy ones may be remarkably enhanced with significant implications for the production of these heavy neutrinos at high energy colliders.

CouplingPhysicsHigh energyParticle physicsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesHiggs sectorStandard ModelMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentNeutrinoEngineering (miscellaneous)Particle Physics - Phenomenology
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Small neutrino masses and gauge coupling unification

2014

The physics responsible for gauge coupling unification may also induce small neutrino masses. We propose a novel gauge mediated radiative seesaw mechanism for calculable neutrino masses. These arise from quantum corrections mediated by new $SU(3)_c \times SU(2)_L \times U(1)_X$ (3-3-1) gauge bosons and the physics driving gauge coupling unification. Gauge couplings unify for a 3-3-1 scale in the TeV range, making the model directly testable at the LHC.

CouplingPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaYang–Mills theoryGauge (firearms)High Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSupersymmetric gauge theoryNeutrinoGauge anomaly
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Gamma(Z --> bb): A signature of hard mass terms for a heavy top

1988

Abstract We calculate analytically the weak radiative corrections to the weak neutral current gauge boson-bottom fermion vertex, keeping the mass mt of the internal fermion line for the relevant diagrams. We find, to order α, a hard mass-term dependence m t 2 M W 2 of the amplitude, for large mt values. Its origin comes from the unphysical charged Higgs coupling to fermions in the renormalizable gauge or, equivalently, from the longitudinal charged gauge boson couplings. The diagonal Z0 decay width to b-quarks decreases, due to these weak radiative corrections, by 0.6%–2.5% when the top mass mt varies from 45 to 200 GeV.

CouplingPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsNeutral currentHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFermionlcsh:QC1-999Vertex (geometry)AmplitudeQuantum electrodynamicsRadiative transferHiggs bosonlcsh:Physics
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Limits on anomalous trilinear gauge boson couplings from WW, WZ and Wγ production in pp¯ collisions at s=1.96 TeV

2012

We present searches for the anomalous γWW and ZWW trilinear gauge boson couplings from WW and WZ production using lepton plus dijet final states and a combination with results from Wγ, WW, and WZ production with leptonic final states. The analyzed data correspond to up to 8.6fb -1 of integrated luminosity collected by the D0 detector in pp- collisions at s=1.96TeV. We set the most stringent limits at a hadron collider to date assuming two different relations between the anomalous coupling parameters δκ γ, λ, and δg1Z for a cutoff energy scale Λ=2TeV. The combined 68% C.L. limits are -0.057lδκ γl0.154, -0.015lλl0.028, and -0.008lδg1Zl0.054 for the LEP parameterization, and -0.007lδκl0.081 an…

CouplingPhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonLuminosity (scattering theory)Large Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciences7. Clean energyNuclear physics0103 physical sciencesQuadrupoleCutoffHigh Energy Physics::Experiment010306 general physicsMagnetic dipoleLeptonPhysics Letters B
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Top quark anomalous tensor couplings in the two-Higgs-doublet models

2013

We compute the one loop right and left anomalous tensor couplings (g(R) and g(L), respectively) for the top quark, in the aligned two-Higgs-doublet model. They are the magnetic-like couplings in the most general parameterization of the tbW vertex. We find that the aligned two-Higgs doublet model, that includes as particular cases some of the most studied extensions of the Higgs sector, introduces new electroweak contribution's and provides theoretical predictions that are very sensitive to both new scalar masses and the neutral scalar mixing angle. For a largo area in the parameters space we obtain significant deviations in both the real and the imaginary parts of the couplings gR and gL, c…

CouplingPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkStandard ModelLarge Hadron ColliderPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyElectroweak interactionFísicaFOS: Physical sciencesHiggs sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Beyond Standard ModelHiggs bosonCP violationJournal of High Energy Physics
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Eta-eta' Photoproduction and the axial isoscalar neutral current coupling

1995

We show that coherentη andη′ photoproduction by means of the Primakoff Effect on the proton depends on the strange component of the neutral axial current coupling. We construct polarization asymmetries that are sensitive to this coupling through theγ−Z interference. Theη′ is not a Goldstone boson of a spontaneously broken chiral symmetry, but a phenomenological analysis of theη andη′ production through chiral perturbation theory allows to calculate the observables of interest. The polarized proton or polarized photon asymmetries are predicted to be close to 10−4 for −q 2∼0.1−0.5 GeV2.

CouplingPhysicsParticle physicsChiral perturbation theoryPhysics and Astronomy (miscellaneous)Neutral currentIsoscalarElementary particlePrime (order theory)Partícules (Física nuclear)Nuclear physicsGoldstone bosonHigh Energy Physics::ExperimentNucleonNuclear ExperimentPrimakoff effectBoson
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Experimental constraints on the coupling of the Higgs boson to electrons

2015

In the standard model (SM), the coupling of the Higgs boson to electrons is real and very small, proportional to the electron mass. New physics could significantly modify both real and imaginary parts of this coupling. We discuss experiments which are sensitive to the Higgs-electron coupling and derive the current bounds on new physics contributing to this coupling. The strongest constraint follows from the ACME bound on the electron electric dipole moment (EDM). We calculate the full analytic two-loop result for the electron EDM and show that it bounds the imaginary part of the Higgs-electron coupling to be less than 1.7 x 10^-2 times the SM electron Yukawa coupling. Deviations of the real…

CouplingPhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron ColliderAnomalous magnetic dipole momentPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesElectron electric dipole momentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentJournal of High Energy Physics
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gg→HH : Combined uncertainties

2021

In this paper we discuss the combination of the usual renormalization and factorization scale uncertainties of Higgs-pair production via gluon fusion with the novel uncertainties originating from the scheme and scale choice of the virtual top mass. Moreover, we address the uncertainties related to the top-mass definition for different values of the trilinear Higgs coupling and their combination with the other uncertainties.

CouplingPhysicsParticle physicsScale (ratio)010308 nuclear & particles physicsPhysicsHigh Energy Physics::LatticeHigh Energy Physics::Phenomenology01 natural sciencesGluonRenormalizationNonlinear Sciences::Exactly Solvable and Integrable SystemsFactorization0103 physical sciencesHiggs bosonddc:530High Energy Physics::Experiment010306 general physicsPhysical Review D
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Quantum simulation of the spin-boson model with a microwave circuit

2017

We consider superconducting circuits for the purpose of simulating the spin-boson model. The spin-boson model consists of a single two-level system coupled to bosonic modes. In most cases, the model is considered in a limit where the bosonic modes are sufficiently dense to form a continuous spectral bath. A very well known case is the ohmic bath, where the density of states grows linearly with the frequency. In the limit of weak coupling or large temperature, this problem can be solved numerically. If the coupling is strong, the bosonic modes can become sufficiently excited to make a classical simulation impossible. Here, we discuss how a quantum simulation of this problem can be performed …

CouplingPhysicsQuantum PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter - SuperconductivityFOS: Physical sciencesQuantum simulator01 natural sciences010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)ResonatorCircuit quantum electrodynamicsQuantum mechanicsQubitQuantum electrodynamicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesDensity of statesQuantum Physics (quant-ph)010306 general physicsBosonSpin-½
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