Search results for "Coupling"

showing 10 items of 1862 documents

Extended HQEFT Lagrangian and currents

2000

From the tree-level heavy quark effective Lagrangian keeping particle-antiparticle mixed sectors we derive the vector current coupling to a hard gluonic field allowing for heavy quark-antiquark pair annihilation and creation.

QuarkPhysicsCouplingNuclear and High Energy PhysicsParticle physicsCurrent (mathematics)AnnihilationField (physics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Effective lagrangiansymbolsHigh Energy Physics::ExperimentLagrangian
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Nonperturbative renormalization constants and light quark masses

2002

We present the results of an extensive non-perturbative calculation of the renormalization constants of bilinear quark operators for the non-perturbatively O(a)-improved Wilson action. The results are obtained at four values of the lattice coupling, by using the RI/MOM and the Ward identities methods. A new non-perturbative renormalization technique, which is based on the study of the lattice correlation functions at short distance in x-space, is also numerically investigated. We then use our non-perturbative determination of the quark mass renormalization constants to compute the values of the strange and the average up/down quark masses. After performing an extrapolation to the continuum …

QuarkPhysicsCouplingNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeContinuum (design consultancy)High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyExtrapolationDown quarkFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsRenormalizationHigh Energy Physics - LatticeLattice (music)High Energy Physics::ExperimentNon-perturbative
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The phi NN coupling from chiral loops

2002

Starting from effective Lagrangians which combine a gauge formulation of Vector Meson Dominance with Chiral Lagrangians, the coupling of the phi to the nucleon, which is zero at tree level due to the OZI rule, is calculated perturbatively considering loop contributions to the electric and magnetic form factors. We obtain reasonably smaller values for both form factors than those for rho NN and consistent with the expected order of magnitude of the OZI rule violation.

QuarkPhysicsCouplingNuclear and High Energy PhysicsParticle physicsNuclear TheoryNuclear TheoryHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesVector meson dominanceGauge (firearms)Nuclear Theory (nucl-th)OZI ruleHigh Energy Physics::ExperimentNucleonOrder of magnitudeMixing (physics)
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Test of the flavour independence of αs

1995

Abstract Using about 950000 hadronic events collected during 1991 and 1992 with the ALEPH detector, the ratios r b = α s b α s udsc and r uds = α s uds α s cb have been measured in order to test the flavour independence of the strong coupling constant α s . The analysis is based on event-shape variables using the full hadronic sample, two b -quark samples enriched by lepton tagging and lifetime tagging, and a light-quark sample enriched by lifetime antitagging. The combined results are r b = 1.002±0.023 and r uds = 0.971 ± 0.023.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectron–positron annihilationPhysicsHadronFlavour01 natural sciencesALEPH ExperimentNuclear physics0103 physical sciencesStrong coupling010306 general physicsALEPH experimentIndependence (probability theory)Lepton
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The Weak-Magnetic Moment of Heavy Quarks

1997

With initial and final particles on-shell, the anomalous weak-magnetic dipole moments of b and c quarks are electroweak gauge invariant quantities of the effective couplings Zb\bar{b} and Zc\bar{c}, respectively, and good candidates to test the Standard Model and/or new physics. Here we present a complete computation of these quantities within the Standard Model. We show that decoupling properties with respect to heavy particles do take place in the weak magnetic moment. The obtained values, a_b(M_Z^2)=(2.98-1.56i)x10^(-4) and a_c(M_Z^2)=(-2.80+1.09i)x10^(-5) are dominated by one-gluon exchange diagrams. The electroweak corrections are less than 1% of the total magnitude.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsMagnetic momentPhysics beyond the Standard ModelComputationElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesDecoupling (cosmology)Invariant (physics)Partícules (Física nuclear)DipoleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::Experiment
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Zb(10610) and Zb′(10650) decays in a covariant quark model

2017

We present a calculation of the strong decays of the exotic states ${Z}_{b}(10610)$ and ${Z}_{b}^{\ensuremath{'}}(10650)$ using a covariant quark model. We use a molecular-type four-quark current for the coupling of the ${Z}_{b}(10610)$ and ${Z}_{b}^{\ensuremath{'}}(10650)$ to the constituent heavy and light quarks.

QuarkPhysicsParticle physicsCurrent (mathematics)010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyQuark modelCoupling (probability)01 natural sciences0103 physical sciencesHigh Energy Physics::ExperimentCovariant transformation010306 general physicsPhysical Review D
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Search for New Phenomena in Final States with Two Leptons and One or No b -Tagged Jets at s=13  TeV Using the ATLAS Detector

2021

A search for new phenomena is presented in final states with two leptons and one or no $b$-tagged jets. The event selection requires the two leptons to have opposite charge, the same flavor (electrons or muons), and a large invariant mass. The analysis is based on the full Run-2 proton-proton collision dataset recorded at a center-of-mass energy of $\sqrt{s} = 13$ TeV by the ATLAS experiment at the LHC, corresponding to an integrated luminosity of 139 fb$^{-1}$. No significant deviation from the expected background is observed in the data. A four-fermion contact interaction between two quarks ($b,s$) and two leptons ($ee$ or $\mu\mu$), inspired by the $B$-meson decay anomalies, is used as a…

QuarkPhysicsParticle physicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyATLAS experimentGeneral Physics and AstronomyLambdaCoupling (probability)7. Clean energy01 natural sciences0103 physical sciencesHigh Energy Physics::ExperimentInvariant mass010306 general physicsLeptonPhysical Review Letters
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Measurement of jet charge in dijet events froms=8  TeVppcollisions with the ATLAS detector

2016

The momentum-weighted sum of the charges of tracks associated to a jet is sensitive to the charge of the initiating quark or gluon. This paper presents a measurement of the distribution of momentum ...

QuarkQuantum chromodynamicsCoupling constantPhysicsParticle physics010308 nuclear & particles physicsScatteringAtlas detectorHigh Energy Physics::Latticemedia_common.quotation_subjectNuclear TheoryHigh Energy Physics::PhenomenologyPerturbative QCD01 natural sciencesAsymmetryGluonNuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsmedia_commonPhysical Review D
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QCD exotics versus a standard model Higgs boson

2012

The present collider data put severe constraints on any type of new strongly interacting particle coupling to the Higgs boson. We analyze the phenomenological limits on exotic quarks belonging to nontriplet $SU(3{)}_{C}$ representations and their implications on Higgs searches. The discovery of the standard model Higgs, in the experimentally allowed mass range, would exclude the presence of exotic quarks coupling to it. Thus, such QCD particles could only exist provided that their masses do not originate in the SM Higgs mechanism.

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaElementary particleCoupling (probability)Standard ModelHiggs fieldsymbols.namesakeHiggs bosonsymbolsHigh Energy Physics::ExperimentHiggs mechanism
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QCD corrections to static heavy-quark form factors

2005

Interactions of heavy quarks, in particular of top quarks, with electroweak gauge bosons are expected to be very sensitive to new physics effects related to electroweak symmetry breaking. These interactions are described by the so-called static form factors, which include anomalous magnetic moments and the effective weak charges. We compute the second-order QCD corrections to these static form factors, which turn out to be sizeable and need to be taken into account in searches for new anomalous coupling effects.

QuarkQuantum chromodynamicsPhysicsParticle physicsGauge boson010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesTechnicolor01 natural sciencesCoupling (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentSymmetry breaking010306 general physics
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