Search results for "Standard Model"

showing 10 items of 1206 documents

Flavor changing neutral currents in the dualized standard model

1998

The Dualized Standard Model which gives explanations for both fermion generations and Higgs fields has already been used to calculate fermion mass and mixing parameters with success. In this paper, we extend its application to low energy FCNC effects deriving bounds for various processes in terms of one single mass scale. Using then experimental information from K_L - K_S mass difference and air showers beyond the GZK cut-off, these bounds are converted into rough, order-of-magnitude predictions. In particular, the estimates for the decay K_L \to e^\pm \mu^\mp and for the mass difference between the neutral D-mesons seem accessible to experiment in the near future.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesDuality (optimization)FísicaScale (descriptive set theory)FermionStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentFlavorMixing (physics)
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Revealing the Majorana nature of heavy neutrinos via a heavy Higgs boson

1992

Abstract Analyzing several recently proposed models, based on simple extensions of the standard model (SM), with heavy Majorana neutrinos, it is shown that the change of detecting lepton number violation through their production and subsequent decays may be significantly enhanced, if a heavy Higgs boson with mass within a reasonably broad range is present.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyElementary particleMass matrixLepton numberStandard ModelNuclear physicsParticle scatteringMAJORANAHiggs bosonHigh Energy Physics::ExperimentNeutrinoPhysics Letters B
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Search for neutral Higgs bosons from supersymmetry in Z decays

1990

The light scalar Higgs boson h and the pseudoscalar Higgs boson A of the minimal supersymmetric standard model have been searched for in the processes e+e−→hff and e+e−→hA using data collected by ALEPH at the LEP e+e− collider, with center of mass energies at and near the Z peak. Using a variety of signatures adapted to various mass ranges for h and A, we have excluded a large domain in the parameter space. For large values of ν2ν1, the ratio of the vacuum expectation values of the two Higgs fields, the whole range from 0 to 38.8 GeV is excluded for Mh and MA at 95% CL.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyElementary particleSupersymmetrylcsh:QC1-999Standard ModelPseudoscalarsymbols.namesakeHiggs bosonsymbolsHigh Energy Physics::ExperimentHiggs mechanismParticle Physics - Experimentlcsh:PhysicsMinimal Supersymmetric Standard ModelBosonPhysics Letters B
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Lepton Flavour Violation in charged leptons within SUSY-seesaw

2009

6 pages, 6 figures.-- Pre-print archive.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)SupersymmetryAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentNeutrinoLeptonMinimal Supersymmetric Standard Model
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Photo-transmutation of leptons

2001

By photo-transmutation of leptons we mean photon-lepton reactions of the following type: $\gamma l_\alpha \longrightarrow \gamma l_\beta$ with $l_\alpha \neq l_\beta$, occurring as a consequence of the lepton mass matrix changing its orientation (rotating) under changing scales. In this paper, we first discuss these reactions in general terms, then proceed to the calculation of their cross sections in two specific schemes, one within the framework of the conventional Standard Model, the other being the so-called Dualized Standard Model we ourselves advocate. Although the cross section obtained is generally small the calculation reveals certain special circumstances where these reactions may…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Mass matrixStandard ModelOrientation (vector space)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentLepton
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Charge Breaking Minima in the Broken R-parity Minimal Supersymmetric Standard Model

2005

We reconsider the possible presence of charge and colour breaking minima in the scalar potential of the minimal supersymmetric standard model (MSSM) and its minimal generalization with R-parity explicitly broken by bilinear terms (RMSSM). First we generalize some results previously derived for the MSSM case. Next we investigate how robust is the MSSM against its RMSSM extension. We examine the constraints on the RMSSM parameter space that follow from the required absence of charge breaking minima in the scalar potential. We point out the possibility of generating non--zero vacuum expectation values for the charged Higgs field which is not present in the MSSM. However, given the smallness of…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesScalar potentialParameter spaceMaxima and minimaHiggs fieldHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parityHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMinimal Supersymmetric Standard Model
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5D perspective on Higgs production at the boundary of a warped extra dimension

2014

A comprehensive, five-dimensional calculation of Higgs-boson production in gluon fusion is performed for both the minimal and the custodially protected Randall-Sundrum (RS) model, with Standard Model fields propagating in the bulk and the scalar sector confined on or near the IR brane. For the first time, an exact expression for the gg->h amplitude in terms of the five-dimensional fermion propagator is derived, which includes the full dependence on the Higgs-boson mass. Various results in the literature are reconciled and shown to correspond to different incarnations of the RS model, in which the Higgs field is either localized on the IR brane or is described in terms of a narrow bulk st…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesPropagatorParameter spaceStandard ModelHigh Energy Physics - PhenomenologyHiggs fieldHigh Energy Physics - Phenomenology (hep-ph)AmplitudeHiggs bosonBraneJournal of High Energy Physics
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Bounds on a light scalar in two-Higgs-doublet models

1992

22 páginas, 4 figuras.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyScalar (mathematics)FísicaElementary particleStandard ModelHiggs fieldPionHiggs bosonGrand Unified TheoryHigh Energy Physics::ExperimentNuclear ExperimentBosonParticle Physics - Phenomenology
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Is charged lepton flavor violation a high energy phenomenon?

2013

Searches for rare processes such as mu --> e gamma put stringent limits on lepton flavour violation expected in many Beyond the Standard Model physics scenarios. This usually precludes the observation of flavour violation at high energy colliders such as the LHC. We here discuss a scenario where right-handed neutrinos are produced via a Z' portal but which can only decay via small flavour violating couplings. Consequently, the process rate is unsuppressed by the small couplings and can be visible despite unobservably small mu --> e gamma rates.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh energyLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciences01 natural sciencesProcess rateHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsEnergy (signal processing)FlavorLeptonPhysical Review D
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Weakly interacting dark matter particle of a minimal technicolor theory

2007

We consider the possibility that a massive fourth family neutrino, predicted by a recently proposed minimal technicolor theory, could be the source of the dark matter in the Universe. The model has two techniflavors in the adjoint representation of a SU(2) techicolor gauge group and its consistency requires the existence of a fourth family of leptons. By a suitable hypercharge assignment the techniquarks together with the new leptons look like a conventional fourth standard model family. We show that the new (Majorana) neutrino N can be the dark matter particle if m{sub N}{approx}100-500 GeV and the expansion rate of the Universe at early times is dominated by an energy component scaling as…

PhysicsNuclear and High Energy PhysicsParticle physicsHypercharge010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyDark matterAdjoint representation01 natural sciencesUniverseStandard ModelGauge group0103 physical sciencesNeutrino010306 general physicsLeptonmedia_commonPhysical Review D
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