Search results for "quantum chromodynamics"

showing 10 items of 1027 documents

Elliptic Flow of Electrons from Beauty-Hadron Decays in Pb-Pb Collisions at sNN=5.02  TeV

2021

The elliptic flow of electrons from beauty hadron decays at midrapidity ($|y|$ $<$ 0.8) is measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV with the ALICE detector at the LHC. The azimuthal distribution of the particles produced in the collisions can be parameterized with a Fourier expansion, in which the second harmonic coefficient represents the elliptic flow, $v_{\rm 2}$. The $v_{\rm 2}$ coefficient is measured for the first time in transverse momentum ($p_{\rm{T}}$) range 1.3-6 GeV/$c$ in the centrality class 30-50%. The measurement of electrons from beauty-hadron decays exploits their larger mean proper decay length $c\tau \approx$ 500 $\mu$m compared to that of charm had…

Quantum chromodynamicsPhysicsQuarkParticle physicsDegree (graph theory)MesonElliptic flowHadronGeneral Physics and Astronomy01 natural sciences7. Clean energy0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentCharm (quantum number)Nuclear Experiment010306 general physicsPhysical Review Letters
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Quarks in nuclei

1992

We review some properties of Quantum Chromodynamics, the theory of the hadronic interactions, which serve as guidelines to introduce low energy models of hadron structure. Among these we shall center our attention in the non relativistic quark model and the topological bag model. We present some of their applications to actual problems in experimental and theoretical nuclear physics. In particular we discuss exotic nuclei, quark matter, deep inelastic scattering, proton spin,... and their relation to such phenomena as quark Pauli blocking, strangeness enhancement, nuclear structure functions, bosonization,...

Quantum chromodynamicsPhysicsQuarkParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHadronQuark modelStrangenessDeep inelastic scatteringStrange matterProton spin crisisHigh Energy Physics::ExperimentNuclear Experiment
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Quarks in Few Hadron Systems

1994

We make use of QCD-based quark models to analyze the observability of quark effects in few hadron systems. A hadron is described by a two phase picture. The dynamics of the interior (perturbative) phase consists of a mechanism to confine the elementary degrees of freedom and an asymptotic QGD type interaction. The dynamics of the exterior (non perturbative) phase is approximated by an effective mesonic lagrangian.

Quantum chromodynamicsPhysicsQuarkParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadronPhase (waves)Degrees of freedom (physics and chemistry)High Energy Physics::ExperimentObservabilityNon-perturbativeWave function
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Search for dark matter produced in association with a Higgs boson decaying to two bottom quarks inppcollisions ats=8  TeVwith the ATLAS detector

2016

This article reports on a search for dark matter pair production in association with a Higgs boson decaying to a pair of bottom quarks, using data from 20.3 fb(-1) of pp collisions at a center-of-m ...

Quantum chromodynamicsPhysicsQuarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyDark matter01 natural sciencesNuclear physicsPair productionmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesHiggs bosonmedicineEffective field theoryHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Prediction of positive parity Bs mesons and search for the X(5568)

2016

We use a combination of quark-antiquark and $B^{(*)}K$ interpolating fields to predict the mass of two QCD bound states below the $B^*K$ threshold in the quantum channels $J^P=0^+$ and $1^+$. The mesons correspond to the b-quark cousins of the $D_{s0}^*(2317)$ and $D_{s1}(2460)$ and have not yet been observed in experiment, even though they are expected to be found by LHCb. In addition to these predictions, we obtain excellent agreement of the remaining p-wave energy levels with the known $B_{s1}(5830)$ and $B_{s2}^*(5840)$ mesons. The results from our first principles calculation are compared to previous model-based estimates. More recently the D0 collaboration claimed the existence of an …

Quantum chromodynamicsPhysicsQuarkParticle physicsMesonHigh Energy Physics::LatticeLattice (order)Hadron spectroscopyHigh Energy Physics::PhenomenologyBound stateHigh Energy Physics::ExperimentTetraquarkParity (physics)Proceedings of 34th annual International Symposium on Lattice Field Theory — PoS(LATTICE2016)
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Bottomonium precision tests from full lattice QCD: Hyperfine splitting, ϒ leptonic width, and b quark contribution to e+e−→hadrons

2021

We calculate the mass difference between the $\mathrm{\ensuremath{\Upsilon}}$ and ${\ensuremath{\eta}}_{b}$ and the $\mathrm{\ensuremath{\Upsilon}}$ leptonic width from lattice QCD using the highly improved staggered quark formalism for the $b$ quark and including $u$, $d$, $s$ and $c$ quarks in the sea. We have results for lattices with lattice spacing as low as 0.03 fm and multiple heavy quark masses, enabling us to map out the heavy quark mass dependence and determine values at the $b$ quark mass. Our results are ${M}_{\mathrm{\ensuremath{\Upsilon}}}\ensuremath{-}{M}_{{\ensuremath{\eta}}_{b}}=57.5(2.3)(1.0)\text{ }\text{ }\mathrm{MeV}$ (where the second uncertainty comes from neglect of …

Quantum chromodynamicsPhysicsQuarkParticle physicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHadronLattice QCDCorrelation function (quantum field theory)01 natural sciencesBottom quark0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Natural constraints on the gluon-quark vertex

2016

In principle, the strong-interaction sector of the Standard Model is characterised by a unique renormalisation-group-invariant (RGI) running interaction and a unique form for the dressed--gluon-quark vertex, $\Gamma_\mu$; but, whilst much has been learnt about the former, the latter is still obscure. In order to improve this situation, we use a RGI running-interaction that reconciles both top-down and bottom-up analyses of the gauge sector in quantum chromodynamics (QCD) to compute dressed-quark gap equation solutions with 1,660,000 distinct Ansaetze for $\Gamma_\mu$. Each one of the solutions is then tested for compatibility with three physical criteria and, remarkably, we find that merely…

Quantum chromodynamicsPhysicsQuarkParticle physicsNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyHadronStrong interactionFOS: Physical sciencesObservable01 natural sciencesGluonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear theoryPhysical Review D
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QCD effects and $b$-tagging at LEP I

1995

We analyze the impact of using $b$-tagged samples in studying non-Abelian effects due to QCD in $e^+e^-\ar 4$jet events at $\sqrt s=M_{Z^0}$, using angular variable analyses and comparisons with $e^+e^-\ar 3 \mbox{jet}\gamma$ events. We find that QCD effects are largely enhanced in $b$-quark samples with respect to `unflavoured' ones, where energy-ordering is used to distinguish between gluon and quark jets. We show that the $b$-quark mass influences the angular distributions significantly and should not be neglected

Quantum chromodynamicsPhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesJet (particle physics)b-taggingGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::Experiment
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Generalized on-shell renormalization of heavy quarks

1992

A generalized on-shell (GOS) renormalization scheme of QCD is developed to evaluate the renormalization of heavy quark wave functions and currents. All large logarithms arising from the physical range of quark masses and momentum transferq 2 can be absorbed into wave function and vertex renormalization. Our results are more general than those of the heavy quark effective theory and agree with the latter only at zero recoil. The proposed GOS scheme is very suitable for the μ/m Q expansion. As an application we discuss the renormalization of the flavour changing currentsb-c, t-b andt-c.

Quantum chromodynamicsPhysicsQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFlavourElementary particleRenormalizationRecoilHigh Energy Physics::ExperimentQuantum field theoryWave functionEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Correlation of pp data with predictions of improved six-quark structure models.

1987

Recent experimental data indicate a structure in \ensuremath{\Delta}${\ensuremath{\sigma}}_{L}$ corresponding to a pp mass of 2.7 GeV/${c}^{2}$, as earlier predicted for a six-quark $^{1}\mathrm{S}_{0}$ state by an R-matrix treatment of the cloudy-bag-model quark degrees of freedom interior to a coupled-isobar-channel system. The $^{1}\mathrm{S}_{0}$ model is improved to agree with 2\ensuremath{\pi} production data at 800 MeV laboratory energy. The resulting $^{1}\mathrm{S}_{0}$ partial wave and recently improved models of the background partial waves as well as older versions of the phase parameters predict experimental observables in the resonance region. The predicted width and inelastic…

Quantum chromodynamicsPhysicsQuarkParticle physicsQuark modelFísicaProduction (computer science)Inelastic scatteringWave functionEnergy (signal processing)R-matrixPhysical review. D, Particles and fields
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