Search results for "Quark"

showing 10 items of 2905 documents

The mesonic spectrum of bosonized QCD2 in the chiral limit

1991

Abstract By studying an equivalent non-abelian bosonic theory we resolve the mesonic spectrum of quantum chromodynamics in one space-one time dimension for massless quarks. The emphasis is placed in the non-chiral sector described be colored meson fields. Two and four point functions of these fields are explicitly calculated in the large N limit. Some of the relevant issues: chiral symmetry realization, phases, anomaly saturation, etc…, are revisited.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologySpectrum (functional analysis)Massless particleTheoretical physicsQuantum mechanicsHigh Energy Physics::ExperimentLimit (mathematics)Anomaly (physics)Realization (systems)Physics Letters B
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2019

Abstract Heavy quarkonium related observables are very useful to obtain information about the medium created in relativistic heavy ion collisions. In recent years the theoretical description of quarkonium in a medium has moved towards a more dynamical picture in which decay and recombination processes are very important. In this talk we will discuss the equations that describe the evolution of the heavy quark reduced density matrix in different approximations, highlighting the color dynamics that is absent in the Abelian case, and we will study their semi-classical limit. This will allow us to obtain stochastic equations (similar to Langevin or Boltzmann equations) that can be useful to obt…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyObservableQuarkonium7. Clean energy01 natural sciencesBoltzmann equationsymbols.namesake0103 physical sciencesBoltzmann constantQuark–gluon plasmasymbols010306 general physicsQuantumNuclear Physics A
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Developing the Framed Standard Model

2011

The framed standard model (FSM) suggested earlier, which incorporates the Higgs field and 3 fermion generations as part of the framed gauge theory structure, is here developed further to show that it gives both quarks and leptons hierarchical masses and mixing matrices akin to what is experimentally observed. Among its many distinguishing features which lead to the above results are (i) the vacuum is degenerate under a global $su(3)$ symmetry which plays the role of fermion generations, (ii) the fermion mass matrix is "universal", rank-one and rotates (changes its orientation in generation space) with changing scale $\mu$, (iii) the metric in generation space is scale-dependent too, and in …

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesAstronomy and AstrophysicsFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)Higgs fieldTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Strong CP problemHigh Energy Physics::ExperimentGauge theory
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Heavy-baryon quark model picture from lattice QCD

2015

The ground state and excited spectra of baryons containing three identical heavy quarks, $b$ or $c$, have been recently calculated in nonperturbative lattice QCD. The energy of positive and negative parity excitations has been determined with high precision. Lattice results constitute a unique opportunity to learn about the quark-confinement mechanism as well as elucidating our knowledge about the nature of the strong force. We analyze the nonperturbative lattice QCD results by means of heavy-quark static potentials derived using SU(3) lattice QCD. We make use of different numerical techniques for the three-body problem.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Lattice field theoryQCD vacuumHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLattice QCDHigh Energy Physics - ExperimentNuclear Theory (nucl-th)BaryonHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics::ExperimentLattice model (physics)
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Measurement of the forward-backward asymmetry in the distribution of leptons intt¯events in thelepton+jetschannel

2014

We present measurements of the forward-backward asymmetry in the angular distribution of leptons from decays of top quarks and antiquarks produced in proton-antiproton collisions. We consider the final state containing a lepton and at least three jets. The entire sample of data collected by the D0 experiment during Run II of the Fermilab Tevatron Collider, corresponding to 9.7 inverse fb of integrated luminosity, is used. The asymmetry measured for reconstructed leptons is $A_{FB}^l = \big(2.9 \pm 2.1(stat.) ^{+1.5}_{-1.7}(syst.) \big)$%. When corrected for efficiency and resolution effects within the lepton rapidity coverage of $|y_l|<1.5$, the asymmetry is found to be $A_{FB}^l = \big(4.2…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsGenerator (category theory)media_common.quotation_subjectHigh Energy Physics::PhenomenologyTevatronInverse7. Clean energyAsymmetryNuclear physicsHigh Energy Physics::ExperimentRapidityNuclear ExperimentLeptonmedia_commonPhysical Review D
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Monte Carlo simulation for jet fragmentation in SUSY QCD

2000

We present results from a new Monte Carlo simulation for jet fragmentation in QCD and SUSY QCD for large primary energies $\sqrt s$ up to $10^{16}$ GeV. In the case of SUSY QCD the simulation takes into account not only gluons and quarks as cascading particles, but also their supersymmetric partners. A new model-independent hadronization scheme is developed, in which the hadronization functions are found from LEP data. An interesting feature of SUSY QCD is the prediction of a sizeable flux of the lightest supersymmetric particles (LSPs), if R-parity is conserved. About 10% of the jet energy is transferred to LSPs which, owing to their harder spectra, constitute an important part of the spec…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologySupersymmetryAstrophysicsHadronizationGluonNuclear physicsHigh Energy Physics - PhenomenologyR-parityGrand Unified TheoryHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentParticle Physics - PhenomenologyPhysical Review D
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Three-jet production at LEP and the bottom quark mass

1994

We consider the possibility of extracting the bottom quark mass from LEP data. The inclusive decay rate for $\zbb +\cdots$ is obtained at order $\as$ by summing up the one-loop two-parton decay rate to the tree-level three-parton rate. We calculate the decay width of the $Z$-boson into two and three jets containing the $b$-quark including complete quark mass effects. In particular, we give analytic results for a slight modification of the JADE clustering algorithm. We also study the angular distribution with respect to the angle formed between the gluon and the quark jets, which has a strong dependence on the quark mass. The impact of higher order QCD corrections on these observables is bri…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaOrder (ring theory)FOS: Physical sciencesObservableJet (particle physics)Bottom quarkJADE (particle detector)GluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentParticle Physics - Phenomenology
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QCD moment sum rules for Coulomb systems: the charm and bottom quark masses

2002

In this work the charm and bottom quark masses are determined from QCD moment sum rules for the charmonium and upsilon systems. To illustrate the special character of these sum rules when applied to Coulomb systems we first set up and study the behaviour of the sum rules in quantum mechanics. In our analysis we include both the results from nonrelativistic QCD and perturbation theory at next-next-to-leading order. The moments are evaluated at different values of q^2 which correspond to different relative influence among the theoretical contributions. In the numerical analysis we obtain the masses by choosing central values for all input parameters. The error is estimated from a variation of…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BibliographyCoulombHigh Energy Physics::ExperimentCharm (quantum number)Perturbation theory
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Quark-mass effects for jet production in e+e- collisions at the next-to-leading order: results and applications

1999

We present a detailed description of our calculation of next-to-leading order QCD corrections to heavy quark production in e^+ e^- collisions including mass effects. In particular, we study the observables $R_3^{b\ql}$ and $D_2^{b\ql}$ in the E, EM, JADE and DURHAM jet-clustering algorithms and show how one can use these observables to obtain $m_b(m_Z)$ from data at the $Z$ peak.

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesFísicaObservableJet (particle physics)JADE (particle detector)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)High Energy Physics::Experiment
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Exclusive/inclusive ratio of semileptonicΛbdecays

2000

We present theoretical evidence that the exclusive/inclusive ratio of semileptonic ${\ensuremath{\Lambda}}_{b}$ decays exceeds that of semileptonic B decays where the experimental exclusive/inclusive ratio amounts to about 66%. We start from the observation that the spectator quark model provides a lower bound on the leading order Isgur-Wise function of the ${\ensuremath{\Lambda}}_{b}\ensuremath{\rightarrow}{\ensuremath{\Lambda}}_{c}$ transition in terms of the corresponding $\stackrel{\ensuremath{\rightarrow}}{B}{D,D}^{*}$ mesonic Isgur-Wise function. Using experimental data for the $\stackrel{\ensuremath{\rightarrow}}{B}{D,D}^{*}$ mesonic Isgur-Wise functions this bound is established. Ap…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyQuark modelForm factor (quantum field theory)Order (ring theory)LambdaBaryonHigh Energy Physics::ExperimentSum rule in quantum mechanicsPhysical Review D
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