Search results for "Quark"

showing 10 items of 2905 documents

Search for light resonances decaying to boosted quark pairs and produced in association with a photon or a jet in proton–proton collisions at s=13TeV…

2019

This Letter presents a search for new light resonances decaying to pairs of quarks and produced in association with a high- pT photon or jet. The dataset consists of proton–proton collisions with an integrated luminosity of 36.1 fb −1 at a centre-of-mass energy of s=13 TeV recorded by the ATLAS detector at the Large Hadron Collider. Resonance candidates are identified as massive large-radius jets with substructure consistent with a particle decaying into a quark pair. The mass spectrum of the candidates is examined for local excesses above background. No evidence of a new resonance is observed in the data, which are used to exclude the production of a lepto-phobic axial-vector Z′ boson.

QuarkPhysicsNuclear and High Energy PhysicsLarge Hadron ColliderPhoton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDark matterResonance01 natural sciencesNuclear physics0103 physical sciencesMass spectrumSubstructureHigh Energy Physics::Experiment010306 general physicsBosonPhysics Letters B
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Anticipating the higher generations of quarks from rephasing invariance of the mixing matrix

1986

Abstract We show that the number of invariant CP violating parameters X CP jumps from the unique universal one in three generations to nine in the four-generation case, saturating the parameter space for generation numbers higher than three. This can lead to drastically different consequences in CP -violating phenomena. We give the quark mass matrices in the three-generation case and speculate for higher generations. We also give some invariant definitions of “maximal” CP violation.

QuarkPhysicsNuclear and High Energy PhysicsMatrix (mathematics)Particle physicsFlavourCP violationFísicaParameter spaceInvariant (physics)Three generationsBottom quark
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Probabilities in nonorthogonal basis: Four--quark systems

2009

Four-quark states may exist as colorless meson-meson molecules or compact systems with two-body colored components. We derive an analytical procedure to expand an arbitrary four-quark wave function in terms of nonorthogonal color singlet-singlet vectors. Using this expansion we develop the necessary formalism to evaluate the probability of physical components with an arbitrary four-quark wave function. Its application to characterize bound and unbound four-quark states as meson-meson, molecular, or compact systems is discussed

QuarkPhysicsNuclear and High Energy PhysicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaTwo-body problemFormalism (philosophy of mathematics)Color modelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ColoredQuantum mechanicsHigh Energy Physics::ExperimentStatistical physicsWave function
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The soliton-soliton interaction in the Chiral Dilaton Model

2012

We study the interaction between two B = 1 states in the Chiral Dilaton Model where baryons are described as nontopological solitons arising from the interaction of chiral mesons and quarks. By using the hedgehog solution for B = 1 states we construct, via a product ansatz, three possible B = 2 configurations to analyse the role of the relative orientation of the hedgehog quills in the dynamics of the soliton-soliton interaction and investigate the behavior of these solutions in the range of long/intermediate distance. One of the solutions is quite binding due to the dynamics of the pi and sigma fields at intermediate distance and should be used for nuclear matter studies. Since the product…

QuarkPhysicsNuclear and High Energy PhysicsMesonNuclear TheoryHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesFísicaAstronomy and AstrophysicsInteraction energyAtomic and Molecular Physics and OpticsNuclear Theory (nucl-th)BaryonScale invarianceNonlinear Sciences::Exactly Solvable and Integrable SystemsBound stateNontopological solitonsDilatonSolitonChiral symmetriesDense matterMathematical physicsAnsatz
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Dirac operator spectrum in the linear σ model

2003

Abstract The spectrum of the Dirac operator for the linear σ Model with quarks in the large Nc approximation is presented. The spectral density can be related to the chiral condensate which is obtained using renormalization group flow equations. For small eigenvalues, the Banks-Casher relation and the vanishing linear correaction are recovered. The spectrum beyond the low energy regime is discussed.

QuarkPhysicsNuclear and High Energy PhysicsMomentum operatorHigh Energy Physics::LatticeSpectrum (functional analysis)Spectral densityDirac operatorsymbols.namesakeSpectral asymmetryQuantum mechanicssymbolsDirac seaEigenvalues and eigenvectorsProgress in Particle and Nuclear Physics
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Search for excited leptons in proton-proton collisions ats=7  TeVwith the ATLAS detector

2012

The ATLAS detector is used to search for excited leptons in the electromagnetic radiative decay channel l* -> l gamma. Results are presented based on the analysis of pp collisions at a center-of ...

QuarkPhysicsNuclear and High Energy PhysicsMuonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas (topology)Atlas detectorRadiative decayElectron01 natural sciencesNuclear physicsExcited state0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Experimental determination of in DELPHI

1998

The running mass of the b quark as defined in the MS renormalization scheme, mb, was measured at the MZ scale using 2.8 million hadronic Z0 decays collected by the DELPHI experiment at LEP. The result is mb(MZ) = 2.67 ± 0.25(stat.) ± 0.34(frag.) ± 0.27(theo.)GeV/c2 which differs from that obtained at the γ scale, by mb(Mγ2)−mb(MZ) = 1.49±0.52 GeV/c2. This measurement, performed far from the bb production threshold, provides the first experimental observation of the running of the quark masses.

QuarkPhysicsNuclear and High Energy PhysicsParticle decayParticle physicsMesonBranching fractionHadronInvariant massQuarkoniumBottom quarkAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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Perspectives in hadron and quark dynamics

1997

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physics0103 physical sciencesHadronDynamics (mechanics)010306 general physics01 natural sciencesNuclear Physics A
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Search for new particles in the two-jet decay channel with the DØ detector

2016

We present the results of a search for the production of new particles decaying into two jets in pp collisions at √s = 1.8 TeV, using the DØ 1992-1995 data set corresponding to 109 pb-1. We exclude at the 95% confidence level the production of excited quarks (q*) with masses below 775 GeV/c2, the most restrictive limit to date. We also exclude standard-model-like W′ (Z′) bosons with masses between 300 and 800 GeV/c2 (400 and 640 GeV/c2). A. W√ boson with mass <786 GeV/c2 has been excluded by previous measurements, and our lower limit is therefore the most stringent to date. © 2004 The American Physical Society.

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorJet (particle physics)01 natural sciencesLower limitlaw.inventionNuclear physicslawExcited state0103 physical sciencesHigh Energy Physics::ExperimentLimit (mathematics)Nuclear Experiment010306 general physicsColliderBosonPhysical Review D
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Subjet multiplicity of gluon and quark jets reconstructed with thek⊥algorithm inpp¯collisions

2002

The D empty set Collaboration has studied for the first time the properties of hadron-collider jets reconstructed with a successive-combination algorithm based on relative transverse momenta (k(perpendicular to)) of energy clusters. Using the standard value D = 1.0 of the jet-separation parameter in the k(perpendicular to) algorithm, we find that the p(T) of such jets is higher than the E-T of matched jets reconstructed with cones of radius R = 0.7, by about 5 (8) GeV at p(T) approximate to90 (240) GeV. To examine internal jet structure, the k(perpendicular to) algorithm is applied within D = 0.5 jets to resolve any subjets. The multiplicity of subjets in jet samples at roots = 1800 GeV and…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaMultiplicity (mathematics)RadiusJet (particle physics)Deep inelastic scattering01 natural sciencesGluonNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentResummationNuclear Experiment010306 general physicsAlgorithmEvent generatorPhysical Review D
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