Search results for "gauge boson"

showing 10 items of 171 documents

Abelian charges in a nonabelian Yang-Mills theory from the stratification of the space of gauge potentials

1992

Abstract The Abelian charges in a non-Abelian Yang-Mills-Dirac theory arising from the reduction of the structure group are studied. They are defined by the concept of the stabilizer gauge transformations. Their properties are investigated. The relationship between the whole class of stabilizers and the stratification of the space of gauge potentials is given. The effect of the spontaneous symmetry breaking mechanism on these charges is discussed.

PhysicsHigh Energy Physics::TheoryGauge bosonIntroduction to gauge theoryQuantum gauge theoryHamiltonian lattice gauge theoryHigh Energy Physics::LatticeSpontaneous symmetry breakingGeneral Physics and AstronomyYang–Mills theoryGauge theoryAbelian groupMathematical physicsAnnals of Physics
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The Higgs Mechanism and Spontaneous Symmetry Breaking

2002

As is well known all gauge bosons of a pure Yang-Mills theory are necessarily massless. This is so because any ad-hoc mass term such as $$ m_i^2 A_\mu ^{(i)} A^{(i)\mu } or \sum\limits_{ik} {M_{ik} } A_\mu ^{(i)} A^{(k)\mu } $$ is incompatible with local gauge invariance. It is saidthat W. Pauli hadd evelopednonab elian gauge theory for himself (or knew about it from the work of H. Weyl and O. Klein) before the work of C.N. Yang and R. Mills (1954) but dismissedit because he hadrealizedthat the gauge particles wouldall be massless. As there was only one massless spin-1 particle known at the time (the photon) nonabelian gauge theory was to be rejectedon physical grounds. The few facts that w…

PhysicsHigh Energy Physics::TheoryParticle physicsIntroduction to gauge theoryHiggs fieldGauge bosonQuantum gauge theoryHamiltonian lattice gauge theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyYang–Mills theoryGauge anomalyGauge symmetry
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Beyond the Standard Model at HERA

2007

The prospects of physics beyond the standard model in deep inelastic scattering are reviewed, emphasizing the search for contact interactions, for leptoquarks and for supersymmetry with R-parity violation, R-parity violating supersymmetry is explored as a speculative source of events with high energy muons and missing transverse momentum, but no convincing explanation for events of this type observed at HI is found.

PhysicsHigh energyGauge bosonParticle physicsMuonPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyTransverse momentumHigh Energy Physics::ExperimentSupersymmetryHERADeep inelastic scattering
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Associated production of weak bosons at the LHC with the ATLAS detector

2009

The study of the associated production of weak vector bosons at the LHC allows to search for New Physics through the measurement of possible deviations of the weak boson self-couplings from the expectation within the Standard Model. The sensitivity of the ATLAS experiment to Standard Model diboson (W+ W-, Wplusmn; Z0, Z0 Z0, W± γ, and Z0 γ) production in pp collisions at = 14 TeV, using final states containing electrons, muons and photons, is presented. These studies use Monte Carlo data sets with full detector simulation from the ATLAS Computer System Commissioning, which furthermore include detailed trigger information as well as effects of detector calibration and alignment corrections. …

PhysicsHistoryParticle physicsGauge bosonPhotonMuonLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysics beyond the Standard ModelATLAS experimentTevatron01 natural sciencesComputer Science ApplicationsEducationNuclear physics0103 physical sciences010306 general physicsBosonJournal of Physics: Conference Series
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Collider signals of the Mirror Twin Higgs boson through the hypercharge portal

2019

We consider the collider signals arising from kinetic mixing between the hypercharge gauge boson of the Standard Model and its twin counterpart in the Mirror Twin Higgs model, in the framework in which the twin photon is massive. Through the mixing, the Standard Model fermions acquire charges under the mirror photon and the mirror Z boson. We determine the current experimental bounds on this scenario, and show that the mixing can be large enough to discover both the twin photon and the twin Z at the LHC, or at a future 100 TeV hadron collider, with dilepton resonances being a particularly conspicuous signal. We show that, in simple models, measuring the masses of both the mirror photon and …

PhysicsHyperchargeGauge bosonParticle physicsPhotonLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical scienceshep-phlaw.inventionStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawHiggs bosonHigh Energy Physics::ExperimentColliderBoson
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Gauge-invariant proper self-energies and vertices in gauge-theories with broken symmetry

1990

Using the pinch technique, we show how to recover, from the {ital S} matrix of a spontaneously broken non-Abelian gauge theory, proper self-energies and vertices which are fully gauge invariant when one or more momenta are off shell. Explicit calculations are carried out at the one-loop level for gauge-boson self-energies and fermion--gauge-boson vertices in a simple SU(2) gauge theory with a Higgs boson. The same technique allows us to calculate, at one-loop order, a neutrino electromagnetic form factor which is gauge invariant at all photon momenta, thus resolving a long-standing problem. We show how massless Goldstone bosons, not present in the {ital S} matrix, must be introduced into Gr…

PhysicsIntroduction to gauge theoryGauge bosonParticle physicsQuantum gauge theoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaBRST quantizationTheoretical physicsHigh Energy Physics::TheoryHamiltonian lattice gauge theorySupersymmetric gauge theoryLattice gauge theoryGauge anomaly
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Measurement of the W-pair cross section in $e^+ e^-$ collisions at 172 GeV

1997

The e(+)e(-) --> W+W- cross section is measured in a data sample collected by ALEPH at a mean centre-of-mass energy of 172.09 GeV, corresponding to an integrated luminosity of 10.65 pb(-1). Cross sections are given for the three topologies, fully leptonic, semi-leptonic and hadronic of a W-pair decay. Under the assumption that no other decay modes are present, the W-pair cross section is measured to be 11.7 +/- 1.2(stat.) +/- 0.3(syst.) pb. The existence of the triple gauge boson vertex of the Standard Model is clearly preferred by the data. The decay branching ratio of the W boson into hadrons is measured to be B(W --> hadrons) = 67.7 +/- 3.1(stat.) +/- 0.7(syst.) %, allowing a determinati…

PhysicsNuclear and High Energy PhysicsAlephGauge bosonParticle physics010308 nuclear & particles physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationHadronHigh Energy Physics::Phenomenology01 natural sciencesVertex (geometry)ALEPH ExperimentNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsNuclear ExperimentALEPH experimentParticle Physics - Experiment
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Study of muon-pair production at centre-of-mass energies from 20 to 136 GeV with the ALEPH detector

1997

The total cross section and the forward-backward asymmetry for the process e(+)e --> mu(+)mu(-)(n gamma) are measured in the energy range 20-136 GeV by reconstructing the effective centre-of-mass energy after initial state radiation. The analysis is based on the data recorded with the ALEPH detector at LEP between 1990 and 1995, corresponding to a total integrated luminosity of 143.5 pb(-1). Two different approaches are used: in the first one an exclusive selection of events with hard initial state radiation in the energy range 20-88 GeV is directly compared with the Standard Model predictions showing good agreement. In the second one, all events are used to obtain a precise measurement of …

PhysicsNuclear and High Energy PhysicsAlephParticle physicsRange (particle radiation)Gauge bosonMuonLuminosity (scattering theory)010308 nuclear & particles physicsPhysicsmuon cross sectionLEP01 natural sciencesStandard ModelNuclear physicsPair production0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experiment010306 general physicsAleph; LEP; muon cross sectionAlephParticle Physics - ExperimentBoson
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Constraints on anomalous QGC's in $e^{+}e^{-}$ interactions from 183 to 209 GeV

2004

The acoplanar photon pairs produced in the reaction e+ e- --> nu nubar gamma gamma are analysed in the 700 inverse nanobarns of data collected by the ALEPH detector at centre-of-mass energies between 183 and 209 GeV. No deviation from the Standard Model predictions is seen in any of the distributions examined. The resulting 95% C.L. limits set on the anomalous QGC's, az_0, az_c, aw_0 and aw_c, are -0.012 GeV**-2 < az_0/Lambda**2 < +0.019 GeV**-2, -0.041 GeV**-2 < az_c/Lambda**2 < +0.044 GeV**-2, -0.060 GeV**-2 < aw_0/Lambda**2 < +0.055 GeV**-2, -0.099 GeV**-2 < aw_c/Lambda**2 < +0.093 GeV**-2, where Lambda is the energy scale of the new Physics responsible for the anomalous couplings.

PhysicsNuclear and High Energy PhysicsGAUGE BOSON COUPLINGS010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaElectron–positron annihilationLEPLambdaFINAL-STATES01 natural sciencesHIGGSStandard ModelENERGYNuclear physicsCOLLIDERSLIMITS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentNuclear Experiment010306 general physicsParticle Physics - ExperimentQUARTIC COUPLINGS
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Nonperturbative gluon and ghost propagators for d=3 Yang-Mills theory

2010

We study a manifestly gauge-invariant set of Schwinger-Dyson equations to determine the non-perturbative dynamics of the gluon and ghost propagators in d = 3 Yang-Mills theory. The use of the well-known Schwinger mechanism, in the Landau gauge leads to the dynamical generation of a mass for the gauge boson (gluon in d = 3), which, in turn, gives rise to an infrared finite gluon propagator and ghost dressing function. The propagators obtained from the numerical solution of these nonperturbative equations are in very good agreement with the results of SU(2) lattice simulations. We would like to thank A. Cucchieri and T. Mendes for kindly making their lattice results available to us, and for t…

PhysicsNuclear and High Energy PhysicsGauge bosonHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics::PhenomenologyPropagatorLie groupYang–Mills theoryGluonHigh Energy Physics::TheoryQuantum electrodynamicsGauge theoryQuantum field theory
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