Search results for "Quark"

showing 10 items of 2905 documents

Multiplicities of charged pions and charged hadrons from deep-inelastic scattering of muons off an isoscalar target

2017

Multiplicities of charged pions and charged hadrons produced in deep-inelastic scattering were measured in three-dimensional bins of the Bjorken scaling variable x , the relative virtual-photon energy y and the relative hadron energy z . Data were obtained by the COMPASS Collaboration using a 160GeV muon beam and an isoscalar target ( 6 LiD). They cover the kinematic domain in the photon virtuality Q2>1(GeV/c)2 , 0.004 1(GeV/c$)^2$, $0.004 < x < 0.4$, $0.2 < z < 0.85$ and $0.1 < y < 0.7$. In addition, a leading-order pQCD analysis was performed using the pion multiplicity results to extract quark fragmentation functions.

QuarkNuclear and High Energy PhysicsPhotonIsoscalarHadronNuclear TheoryHERMEStarget: isoscalar[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesCOMPASSscaling: BjorkenNuclear physicsPionAstronomi astrofysik och kosmologi[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Astronomy Astrophysics and CosmologyPion multiplicitiesNuclear Physics - Experiment[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]quantum chromodynamics: perturbation theory010306 general physicsNuclear ExperimentRICHDeep inelastic scattering; Fragmentation functions; Pion multiplicities; Nuclear and High Energy PhysicsPhysicsquark: fragmentation functionMuonpi: multiplicityhep-ex010308 nuclear & particles physicsScatteringmuon: beamhigher-order: 0Fragmentation functionphotonFragmentation functionsDeep inelastic scatteringhadron: energylcsh:QC1-999kinematicsPion multiplicitieHigh Energy Physics::ExperimentParticle Physics - Experimentlcsh:PhysicsDeep inelastic scattering
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Light- and strange-quark mass dependence of the ρ(770) meson revisited

2020

Recent lattice data on $\pi\pi$-scattering phase shifts in the vector-isovector channel, pseudoscalar meson masses and decay constants for strange-quark masses smaller or equal to the physical value allow us to study the strangeness dependence of these observables for the first time. We perform a global analysis on two kind of lattice trajectories depending on whether the sum of quark masses or the strange-quark mass is kept fixed to the physical point. The quark mass dependence of these observables is extracted from unitarized coupled-channel one-loop Chiral Perturbation Theory. This analysis guides new predictions on the $\rho(770)$ meson properties over trajectories where the strange-qua…

QuarkNuclear and High Energy PhysicsStrange quarkParticle physicsChiral perturbation theoryMeson530 PhysicsHigh Energy Physics::LatticeNuclear TheoryLattice QCDStrangeness01 natural sciencesPseudoscalar mesonHigh Energy Physics - Lattice0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsPhysicsTeoría de los quanta010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyObservableLattice QCDHigh Energy Physics - PhenomenologyChiral LagrangiansPartículaslcsh:QC770-798High Energy Physics::ExperimentJournal of High Energy Physics
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String breaking by light and strange quarks in QCD

2019

The energy spectrum of a system containing a static quark anti-quark pair is computed for a wide range of source separations using lattice QCD with $N_\mathrm{f}=2+1$ dynamical flavours. By employing a variational method with a basis including operators resembling both the gluon string and systems of two separated static mesons, the first three energy levels are determined up to and beyond the distance where it is energetically favourable for the vacuum to screen the static sources through light- or strange-quark pair creation, enabling both these screening phenomena to be observed. The separation dependence of the energy spectrum is reliably parameterised over this saturation region with a…

QuarkNuclear and High Energy PhysicsStrange quarkParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesLattice QCD01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHeavy quarks0103 physical sciences010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDQuarkoniumString breakinglcsh:QC1-999GluonHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics::Experimentlcsh:PhysicsPhysics Letters
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Measurement of the ttbar cross section using high-multiplicity jet events

2010

We present a measurement of the ttbar cross section using high-multiplicity jet events produced in ppbar collisions at sqrt{s}=1.96 TeV. These data were recorded at the Fermilab Tevatron collider with the D0 detector. Events with at least six jets, two of them identified as b jets, were selected from a 1 fb-1 data set. The measured cross section, assuming a top quark mass of 175 GeV/c^2, is 6.9 \pm 2.0 pb, in agreement with theoretical expectations.

QuarkNuclear and High Energy PhysicsTop quarkParticle physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronFOS: Physical sciences7. Clean energy01 natural scienceslaw.inventionHigh Energy Physics - ExperimentNuclear physicsCross section (physics)High Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderPhysicsJet (fluid)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMultiplicity (mathematics)14.65.HaHigh Energy Physics::Experiment
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Search for the t and b' quarks in hadronic decays of the Z0 boson

1990

We present a search for the third generation up type quark t and a possible fourth down type quark b' in hadronic Z0 decays observed in DELPHI at the LEP collider. For any scenario with a decay through the charged current or into a charged Higgs with a mass at least 6 GeV/c2 below the t and 3 GeVc2 below the b' mass, we set a lower limit for the t quark mass at 44.0 GeV/c2 and for the b' mass at 44.5 GeV/c2. For specific scenarios the mass limits are slightly higher, e.g. for charged current decays the limits are 44.5 and 45.0 GeV/c2 respectively, where all limits are given at a 95% confidence level. © 1990.

QuarkNuclear and High Energy PhysicsTop quarkParticle physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]Electron–positron annihilationHadron01 natural sciences7. Clean energylaw.inventionNuclear physicslaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment010306 general physicsColliderCharged currentBosonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPhysique des particules élémentairesHiggs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentPhysics Letters B
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Form factors of radiative pion decays in nonlocal chiral quark models

2012

We study the radiative pion decay π +→e +ν eγ within nonlocal chiral quark models that include wave function renormalization. In this framework we analyze the momentum dependence of the vector form factor F V(q2) and the slope of the axial-vector form factor F A(q2) at threshold. Our results are compared with available experimental information and with the predictions given by the Nambu-Jona-Lasinio model. In addition we calculate the low energy constants δ 5 and δ 6, comparing our results with the values obtained in chiral perturbation theory.

QuarkNuclear and High Energy PhysicsWave function renormalizationParticle physicsChiral perturbation theoryradiative pion decayHigh Energy Physics::LatticeCiencias FísicasFOS: Physical sciences01 natural sciencesPion form factorPartícules (Física nuclear)Momentum//purl.org/becyt/ford/1 [https]pion form factorLow energyPionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transfer010306 general physicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)Física//purl.org/becyt/ford/1.3 [https]AstronomíaHigh Energy Physics - PhenomenologyRadiative pion decayFísica nuclearCIENCIAS NATURALES Y EXACTAS
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Observation of Two NewΞb−Baryon Resonances

2015

Two structures are observed close to the kinematic threshold in the Ξb0π- mass spectrum in a sample of proton-proton collision data, corresponding to an integrated luminosity of 3.0fb-1, recorded by the LHCb experiment. In the quark model, two baryonic resonances with quark content bds are expected in this mass region: the spin-parity JP=(1/2)+ and JP=(3/2)+ states, denoted Ξb′- and Ξb∗-. Interpreting the structures as these resonances, we measure the mass differences and the width of the heavier state to be m(Ξb′-)-m(Ξb0)-m(π-)=3.653±0.018±0.006MeV/c2, m(Ξb∗-)-m(Ξb0)-m(π-)=23.96±0.12±0.06MeV/c2, Γ(Ξb∗-)=1.65±0.31±0.10MeV, where the first and second uncertainties are statistical and systema…

QuarkNuclear physicsBaryonPhysicsParticle physicsQuark modelContent (measure theory)Mass spectrumGeneral Physics and AstronomyState (functional analysis)SpectroscopyLuminosityPhysical Review Letters
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Exclusive semi-leptonic decays of bottom baryons

1990

Abstract We calculate the exclusive semi-leptonic bottom baryon decays Λ b →Λ c +l − + v l , Σ b → Σ c +l − + v l and Σ b →Σ c ∗ +l − + v l in the spectator quark model. The helicity structure of the baryonic current transitions Λb→Λc, Σ b →Σ c (Σ c ∗ ) is matched to the helicity structure of the free quark current transitions b → c at minimum momentum transfer q2 = 0. The results are continued to q2≠0 by pole dominated form factors. We obtain semi-leptonic baryonic decay rates which are close to the corresponding semi-leptonic mesonic decay rates.

QuarkNuclear physicsPhysicsBaryonNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyMomentum transferQuark modelForm factor (quantum field theory)High Energy Physics::ExperimentHelicityPhysics Letters B
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NuTeV sin2θWanomaly and nuclear parton distributions revisited

2006

By studying the Paschos-Wolfenstein (PW) ratio of deep inelastic νFe and Fe scattering cross sections, we show that it should be possible to explain the NuTeV sin2θW anomaly with quite conventional physics, by introducing mutually different nuclear modifications for the valence-u and valence-d quark distributions of the protons in iron. Keeping the EKS98 nuclear modifications for uV+dV as a baseline, we find that some 20-30 % nuclear modifications to the uV and dV distributions account for the change induced in the PW ratio by the NuTeV-suggested increase Δsin2θW = 0.005. We show that introduction of such nuclear modifications in uV and dV individually, does not lead into contradiction with…

QuarkNuclear physicsPhysicsNuclear and High Energy PhysicsDGLAPValence (chemistry)010308 nuclear & particles physicsScattering0103 physical sciencesParton010306 general physicsNucleon01 natural sciencesJournal of High Energy Physics
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Collins asymmetries in inclusive chargedKKandKπpairs produced ine+e−annihilation

2015

We present measurements of Collins asymmetries in the inclusive process e^+e^− → h_1h_2X, h_1h_2 = KK, Kπ, ππ, at the center-of-mass energy of 10.6 GeV, using a data sample of 468  fb^(−1) collected by the BABAR experiment at the PEP-II B factory at SLAC National Accelerator Center. Considering hadrons in opposite thrust hemispheres of hadronic events, we observe clear azimuthal asymmetries in the ratio of unlike sign to like sign, and unlike sign to all charged h_1h_2 pairs, which increase with hadron energies. The Kπ asymmetries are similar to those measured for the ππ pairs, whereas those measured for high-energy KK pairs are, in general, larger.

QuarkNuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationElectron–positron annihilationHadronCenter (category theory)BaBar experimentHigh Energy Physics::ExperimentSign (mathematics)B-factoryPhysical Review D
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