Search results for "Gauge"

showing 10 items of 710 documents

Hadron correlators and the structure of the quark propagator

1994

The structure of the quark propagator of $QCD$ in a confining background is not known. We make an Ansatz for it, as hinted by a particular mechanism for confinement, and analyze its implications in the meson and baryon correlators. We connect the various terms in the K\"allen-Lehmann representation of the quark propagator with appropriate combinations of hadron correlators, which may ultimately be calculated in lattice $QCD$. Furthermore, using the positivity of the path integral measure for vector like theories, we reanalyze some mass inequalities in our formalism. A curiosity of the analysis is that, the exotic components of the propagator (axial and tensor), produce terms in the hadron c…

QuarkPhysicsHigh Energy Physics - TheoryPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesFísicaBaryonTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Path integral formulationHigh Energy Physics::ExperimentGauge theoryEngineering (miscellaneous)Ansatz
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Review of Particle Properties

2002

This biennial Review summarizes much of Particle Physics. Using data from previous editions, plus 2205 new measurements from 667 papers, we list, evaluate, and average measured properties of gauge bosons, leptons, quarks, mesons, and baryons. We also summarize searches for hypothetical particles such as Higgs bosons, heavy neutrinos, and supersymmetric particles. All the particle properties and search limits are listed in Summary Tables. We also give numerous tables, figures, formulae, and reviews of topics such as the Standard Model, particle detectors, probability, and statistics. This edition features expanded coverage of CP violation in B mesons and of neutrino oscillations. For the fir…

QuarkPhysicsNuclear and High Energy PhysicsGauge bosonParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronElementary particleParticle Data GroupFermion01 natural sciencesStandard Model0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Search for W′ boson production in the W′→tb¯ decay channel

2006

We present a search for the production of a new heavy gauge boson W' that decays to a top quark and a bottom quark. We have analyzed 230 pb(-1) of data collected with the DO detector at the Fermilab Tevatron collider at a center-of-mass energy of 1.96 TeV. No significant excess of events above the standard model expectation is found in any region of the final state invariant mass distribution. We set upper limits on the production cross section of W' bosons times branching ratio to top quarks at the 95% confidence level for several different W, boson masses. We exclude masses between 200 and 610 GeV for a W' boson with standard-model-like couplings, between 200 and 630 GeV for a W, boson wi…

QuarkPhysicsNuclear and High Energy PhysicsGauge bosonTop quarkParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyScalar boson7. Clean energy01 natural sciencesBottom quarkStandard ModelNuclear physicsW and Z bosons0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsBosonPhysics Letters B
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Two-loop gluino corrections to the inclusive decayB→Xsγin theCPviolating MSSM with largetanβ

2004

We investigate two-loop gluino corrections to the effective Lagrangian for b{yields}s+{gamma}(g) in the minimal supersymmetric extension of the standard model (MSSM) at large tan{beta}, including the contributions in which quark flavor change is mediated by charginos. Using the translation invariance of loop momenta and the Ward-Takahashi identities that are required by the SU(3){sub c}xU(1){sub em} gauge invariance, we simplify our expressions to concise forms. As an example, we discuss two-loop gluino corrections to the CP asymmetry of inclusive B{yields}X{sub s}{gamma} decay in CP violating MSSM.

QuarkPhysicsNuclear and High Energy PhysicsGluinoParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySuperpartnerSupersymmetry01 natural sciencesStandard Model (mathematical formulation)0103 physical sciencesCP violationHigh Energy Physics::ExperimentB mesonGauge theory010306 general physicsPhysical Review D
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Nonperturbative renormalization in coordinate space

2003

We present an exploratory study of a gauge-invariant non-perturbative renormalization technique. The renormalization conditions are imposed on correlation functions of composite operators in coordinate space on the lattice. Numerical results for bilinears obtained with overlap and O(a)-improved Wilson fermions are presented. The measurement of the quark condensate is also discussed.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)field theory gauge theory lattice renormalizationFOS: Physical sciencesFísicaParticle Physics - LatticeFermionAtomic and Molecular Physics and OpticsComposite operatorRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeLattice (order)Non-perturbativeCoordinate spaceMathematical physics
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On the Pauli-Villars regularisation scheme in the NJL model

1993

Abstract We consider the Nambu-Jona-Lasinio model with a Pauli-Villars cutoff. We point out that previous attempts to use this regularisation have not been consistent and it is shown that if used correctly this approach yields very reasonable values for the cutoff parameter and quark condensate when we demand that ƒπ is fixed to its experimental value. Finally it is argued that because of its covariance and smooth nature this regularisation scheme has significant advantages over other regulators on the market.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryStrong interactionElementary particleCovariancesymbols.namesakePauli exclusion principleRegularization (physics)Quantum electrodynamicssymbolsApplied mathematicsCutoffGauge theoryPhysics Letters B
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Hidden beauty molecules within the local hidden gauge approach and heavy quark spin symmetry

2013

Using a coupled channel unitary approach, combining the heavy quark spin symmetry and the dynamics of the local hidden gauge, we investigate the meson-meson interaction with hidden beauty and obtain several new states. Both I = 0 and I = 1 states are analyzed, and it is shown that in the I = 1 sector, the interactions are too weak to create any bound states within our framework. In total, we predict with confidence the existence of six bound states and six more possible weakly bound states. The existence of these weakly bound states depends on the influence of the coupled channel effects.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBound statesMeson resonancesHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGauge (firearms)01 natural sciencesUnitary stateHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesBound stateMoleculeSpin symmetryNuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
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S3 symmetry and the quark mixing matrix

2016

We impose an $S_3$ symmetry on the quark fields under which two of three quarks transform like a doublet and the remaining one as singlet, and use a scalar sector with the same structure of $SU(2)$ doublets. After gauge symmetry breaking, a $\mathbb{Z}_2$ subgroup of the $S_3$ remains unbroken. We show that this unbroken subgroup can explain the approximate block structure of the CKM matrix. By allowing soft breaking of the $S_3$ symmetry in the scalar sector, we show that one can generate the small elements, of quadratic or higher order in the Wolfenstein parametrization of the CKM matrix. We also predict the existence of exotic new scalars, with unconventional decay properties, which can …

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixSpontaneous symmetry breakingScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciences01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologyExplicit symmetry breakingHigh Energy Physics - Phenomenology (hep-ph)Quadratic equation0103 physical sciencesHigh Energy Physics::ExperimentSinglet state010306 general physicslcsh:PhysicsGauge symmetryPhysics Letters B
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Non-cancellation of electroweak logarithms in high-energy scattering

2014

We study electroweak Sudakov corrections in high energy scattering, and the cancellation between real and virtual Sudakov corrections. Numerical results are given for the case of heavy quark production by gluon collisions involving the rates $gg \to t \bar t, b \bar b, t \bar b W, t \bar t Z, b \bar b Z, t \bar t H, b \bar b H$. Gauge boson virtual corrections are related to real transverse gauge boson emission, and Higgs virtual corrections to Higgs and longitudinal gauge boson emission. At the LHC, electroweak corrections become important in the TeV regime. At the proposed 100 TeV collider, electroweak interactions enter a new regime, where the corrections are very large and need to be re…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonLarge Hadron ColliderScatteringHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical scienceslcsh:QC1-999law.inventionGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lawHiggs bosonHigh Energy Physics::ExperimentColliderlcsh:PhysicsPhysics Letters B
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Non-perturbative renormalisation of left left four-fermion operators with Neuberger fermions

2006

We outline a general strategy for the non-perturbative renormalisation of composite operators in discretisations based on Neuberger fermions, via a matching to results obtained with Wilson-type fermions. As an application, we consider the renormalisation of the four-quark operators entering the Delta S=1 and Delta S=2 effective Hamiltonians. Our results are an essential ingredient for the determination of the low-energy constants governing non-leptonic kaon decays.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)field theory gauge theory lattice renormalizationHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParticle Physics - LatticeFermionComposite operatorRenormalizationFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - LatticeOperator (computer programming)High Energy Physics::ExperimentNon-perturbativeMathematical physics
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