Search results for " symmetry"

showing 10 items of 701 documents

Custodial vector model

2014

We analyze the Large Hadron Collider (LHC) phenomenology of heavy vector resonances with a $SU(2)_L\times SU(2)_R$ spectral global symmetry. This symmetry partially protects the electroweak S-parameter from large contributions of the vector resonances. The resulting custodial vector model spectrum and interactions with the standard model fields lead to distinct signatures at the LHC in the diboson, dilepton and associated Higgs channels.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Colliderta114electroweak sector010308 nuclear & particles physicsAtlas detectorElectroweak interactionHigh Energy Physics::PhenomenologyPP collisionsFOS: Physical scienceshep-phGlobal symmetry01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Low energy0103 physical sciencesModel spectrumHiggs bosonHigh Energy Physics::Experiment010306 general physicsPhenomenology (particle physics)
researchProduct

Hidden gauge formalism for the radiative decays of axial-vector mesons

2009

24 pages, 6 tables, 11 figures.--ISI article identifier:000262979700040 .-- ArXiv pre-print avaible at:http://arxiv.org/abs/0809.0943

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPseudoscalar mesonPseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics::ExperimentGauge theoryVector mesonPseudovectorGauge symmetry
researchProduct

Dynamically generated open and hidden charm meson systems

2006

We will study open and hidden charm scalar meson resonances within two different models. The first one is a direct application of a chiral Lagrangian already used to study flavor symmetry breaking in Skyrme models. In another approach to the problem a SU(4) symmetric Lagrangian is built and the symmetry is broken down to SU(3) by identifying currents where heavy mesons are exchanged and suppressing those. Unitarization in couple channels leads to dynamical generation of resonances in both models, in particular a new hidden charm resonance with mass 3.7 GeV is predicted. The small differences between these models and with previous works will be discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsMesonSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaStability (probability)Symmetry (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentSymmetry breakingCharm (quantum number)Quantum field theoryScalar mesonNuclear Experiment
researchProduct

A consistent study of the the low energy baryon spectrum and the nucleon-nucleon interaction within the chiral quark model

1995

By solving the Schr\"{o}dinger equation for the three-quark system in the hyperspherical harmonic approach, we have studied the low energy part of the nucleon and $\Delta$ spectra using a quark-quark interaction which reproduces the nucleon-nucleon phenomenology. The quark-quark hamiltonian considered includes, besides the usual one-gluon exchange, pion and sigma exchanges generated by the chiral symmetry breaking. The baryonic spectrum obtained is reasonable and the resulting wave function gives consistency to the ansatz used in the two baryon system.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryQuark modelFOS: Physical sciencesFísicaNuclear Theory (nucl-th)Baryonsymbols.namesakePionsymbolsHigh Energy Physics::ExperimentNuclear ExperimentHamiltonian (quantum mechanics)Chiral symmetry breakingNucleonWave functionAnsatzPhysics Letters B
researchProduct

Heavy Resonances in the Electroweak Effective Lagrangian

2015

As a first step towards the construction of a general electroweak effective Lagrangian incorporating heavy states, we present here a simplified version where only vector and axial-vector spin-1 triplets are involved. We adopt an effective field theory formalism, implementing the electroweak chiral symmetry breaking SU(2)L x SU(2)R -> SU(2)L+R, which couples the heavy states to the SM fields. At low energies, the heavy degrees of freedom are integrated out from the action and their effects are hidden in the low-energy couplings of the Electroweak Effective Theory, which can be tested experimentally. Short-distance constraints are also implemented, requiring a proper behaviour in the high-…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesOblique case01 natural sciencesFormalism (philosophy of mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective lagrangianEffective field theory010306 general physicsChiral symmetry breakingBoson
researchProduct

The self-couplings of vector bosons: does LEP-1 obviate LEP-2?

1992

Abstract Theories beyond the standard model (“meta-theories”) are severely constrained by the current body of data and must necessarily respect the standard gauge symmetry. We analyze the constraints on two generic types of meta-theory, in which fundamental scalar do or do not exist. The novel low-energy effects can be comprehensively described by grafting onto the standard lagrangian new operators that - in the sense of a Taylor expansion - form a complete set. Completeness calls for consideration of previously discarded operators, and for a thorough exploitation of the equations of motion. We illustrate the current strictures by focusing on the allowed range of departures from the most cr…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelScalar (mathematics)FísicaElementary particleWeinberg angleMinimal modelTheoretical physicsGauge theoryQuantum field theoryParticle Physics - TheoryGauge symmetry
researchProduct

Neutrino mass and invisible Higgs decays at the LHC

2015

The discovery of the Higgs boson suggests that also neutrinos get their mass from spontaneous symmetry breaking. In the simplest ungauged lepton number scheme, the Standard Model (SM) Higgs has now two other partners: a massive CP-even, as well as the massless Nambu-Goldstone boson, called majoron. For weak-scale breaking of lepton number the invisible decays of the CP- even Higgs bosons to the majoron lead to potentially copious sources of events with large missing energy. Using LHC results we study how the constraints on invisible decays of the Higgs boson restrict the relevant parameters, substantially extending those previously derived from LEP and shedding light on spontaneous lepton n…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberStandard ModelNuclear physicssymbols.namesakeHiggs fieldHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)symbolsHiggs bosonHigh Energy Physics::ExperimentHiggs mechanismMajoron
researchProduct

The strong CP problem and the solar neutrino puzzle: Are they related?

1991

We discuss the possibility that a solution of the strong CP problem via the introduction of a chiral U(1), a la Peccei-Quinn, may also provide a natural scenario for explaining the apparent depletion of the solar neutrino flux through matter enhanced neutrino oscillations. The smallness of the neutrino masses is related to the scale at which the U(1)PQ symmetry is spontaneously broken, without introducing right-handed neutrino fields and invoking the see-saw mechanism. The model is consistent with all present experimental results. In particular, the phenomenology associated to the presence of an “invisible” axion is the same as in the Dine-Fischler-Srednicki-Zhitnisky model with the excepti…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSpontaneous symmetry breakingSolar neutrinoHigh Energy Physics::PhenomenologyElementary particleStrong CP problemNeutrinoNeutrino oscillationPhenomenology (particle physics)AxionNuclear Physics B
researchProduct

Hidden charm molecules in finite volume

2013

In the present paper we address the interaction of pairs of charmed mesons with hidden charm in a finite box. We use the interaction from a recent model based on heavy-quark spin symmetry that predicts molecules of hidden charm in the infinite volume. The energy levels in the box are generated within this model, and from them some synthetic data are generated. These data are then employed to study the inverse problem of getting the energies of the bound states and phase shifts for D (D) over bar or D*(D) over bar*. Different strategies are investigated using the lowest two levels for different values of the box size, and the errors produced are studied. Starting from the upper level, fits t…

PhysicsNuclear and High Energy PhysicsParticle physicsQuantum-field theories010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Library scienceFOS: Physical sciencesFísica01 natural sciences7. Clean energyHigh Energy Physics - Lattice0103 physical sciencesEnergy spectrumHeavy quark effective theorySpin symmetryCharm (quantum number)010306 general physicsEnergy-spectrum
researchProduct

Production and decays of supersymmetric Higgs bosons in spontaneously brokenRparity

2005

We study the mass spectra, production and decay properties of the lightest supersymmetric CP-even and CP-odd Higgs bosons in models with spontaneously broken R-parity (SBRP). We compare the resulting mass spectra with expectations of the Minimal Supersymmetric Standard Model (MSSM), stressing that the model obeys the upper bound on the lightest CP-even Higgs boson mass. We discuss how the presence of the additional scalar singlet states affects the Higgs production cross sections, both for the Bjorken process and the "associated production". The main phenomenological novelty with respect to the MSSM comes from the fact that the spontaneous breaking of lepton number leads to the existence of…

PhysicsNuclear and High Energy PhysicsParticle physicsSpontaneous symmetry breakingHigh Energy Physics::PhenomenologyDoublet–triplet splitting problemFOS: Physical sciencesFísicaSupersymmetryHigh Energy Physics - Phenomenologysymbols.namesakeHiggs fieldHigh Energy Physics - Phenomenology (hep-ph)symbolsHiggs bosonHigh Energy Physics::ExperimentHiggs mechanismMinimal Supersymmetric Standard ModelMajoronPhysical Review D
researchProduct