Search results for "wave function"

showing 10 items of 395 documents

Massive quarks in NLO dipole factorization for DIS : Longitudinal photon

2021

In this work, we will present the first complete calculation of the one-loop longitudinal photon-to-quark-antiquark light cone wave function, with massive quarks. The quark masses are renormalized in the pole mass scheme. The result is used to calculate the next-to-leading order correction to the high energy Deep Inelastic Scattering longitudinal structure function on a dense target in the dipole factorization framework. For massless quarks the next-to-leading order correction was already known to be sizeable, and our result makes it possible to evaluate it also for massive quarks.

QuarkParticle physicsPhotonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryQUANTUM ELECTRODYNAMICSFOS: Physical scienceshiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)FactorizationLight coneINFINITE-MOMENTUM0103 physical sciencesSCATTERINGPICTURE010306 general physicsWave functionPhysics010308 nuclear & particles physicskvarkitLIGHT-FRONT QCDHigh Energy Physics::PhenomenologyDeep inelastic scatteringINVARIANCEMassless particleDipoleHigh Energy Physics - PhenomenologykvanttiväridynamiikkaHigh Energy Physics::ExperimentBK EVOLUTION
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Dipole picture and the nonrelativistic expansion

2022

We study exclusive quarkonium production in the dipole picture at next-to-leading order (NLO) accuracy, using the non-relativistic expansion for the quarkonium wavefunction. This process offers one of the best ways to obtain information about gluon distributions at small $x$, in ultraperipheral heavy ion collisions and in deep inelastic scattering. The quarkonium light cone wave functions needed in the dipole picture have typically been available only at tree level, either in phenomenological models or in the nonrelativistic limit. In this paper, we discuss the compatibility of the dipole approach and the non-relativistic expansion and compute NLO relativistic corrections to the quarkonium …

QuarkParticle physicselectron-ion collisionsPhotonNuclear TheoryQC1-999High Energy Physics::LatticeFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Light cone0103 physical sciences010306 general physicsWave functionNuclear ExperimentPhysics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyQuarkoniumDeep inelastic scatteringrelativistic heavy-ion collionsGluonHigh Energy Physics - PhenomenologyDipoleHeavy ionHigh Energy Physics::Experimentydinfysiikka
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Few-body quark dynamics for doubly heavy baryons and tetraquarks

2018

We discuss the adequate treatment of the 3- and 4-body dynamics for the quark model picture of double-charm baryons and tetraquarks. We stress that the variational and Born-Oppenheimer approximations give energies very close to the exact ones, while the diquark approximation might be rather misleading. The Hall-Post inequalities also provide very useful lower bounds that exclude the possibility of stable tetraquarks for some mass ratios and some color wave functions.

QuarkParticle physicswave functionNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Born–Oppenheimer approximationFOS: Physical sciencestetraquark: energy01 natural sciencesNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsWave functionBorn-Oppenheimer approximation[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]Physicsquark model010308 nuclear & particles physicsQuark modelDynamics (mechanics)High Energy Physics::Phenomenologybaryon: energyMass ratiotetraquark: stabilityBaryonDiquarkHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]symbolsapproximation: diquark[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]mass ratio
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Very Heavy Flavored Dibaryons

2020

We explore the possibility of very heavy dibaryons with three charm quarks and three beauty quarks, $bbbccc$, using a constituent model which should drive to the correct solution in the limit of hadrons made of heavy quarks. The six-body problem is treated rigorously, in particular taking into account the orbital, color and spin mixed-symmetry components of the wave function. Unlike a recent claim based on lattice QCD, no bound state is found below the lowest dissociation threshold.

QuarkParticle physicswave function[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryHigh Energy Physics::LatticeHadronLattice field theoryNuclear TheoryGeneral Physics and AstronomyFOS: Physical sciencesdissociationspin01 natural sciencesCharm quarkquarkNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciencesBound stateheavy quark010306 general physicsWave functionconstituentNuclear ExperimentNuclear theoryPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologylattice field theoryLattice QCDcolordibaryon: heavybound stateHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Elementary Particles and FieldsHigh Energy Physics::ExperimenthadroncharmPhysical Review Letters
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One-Loop Self Energy and Renormalization of the Speed of Light for some Anisotropic Improved Quark Actions

2000

One-loop corrections to the fermion rest mass M_1, wave function renormalization Z_2 and speed of light renormalization C_0 are presented for lattice actions that combine improved glue with clover or D234 quark actions and keep the temporal and spatial lattice spacings, a_t and a_s, distinct. We explore a range of values for the anisotropy parameter \chi = a_s/a_t and treat both massive and massless fermions.

QuarkPhysicsCondensed Matter::Quantum GasesNuclear and High Energy PhysicsWave function renormalizationParticle physicsHigh Energy Physics::LatticeLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFermionRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeSelf-energyLattice gauge theoryInvariant mass
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Production of exotic tetraquarks QQq¯q¯ in heavy-ion collisions at the LHC

2019

We investigate the production of exotic tetraquarks, $QQ\overline{q}\overline{q}\ensuremath{\equiv}{T}_{QQ}$ ($Q=c$ or $b$ and $q=u$ or $d$), in relativistic heavy-ion collisions using the quark coalescence model. The ${T}_{QQ}$ yield is given by the overlap of the density matrix of the constituents in the emission source with the Wigner function of the produced tetraquark. The tetraquark wave function is obtained from exact solutions of the four-body problem using realistic constituent models. The production yields are typically one order of magnitude smaller than previous estimations based on simplified wave functions for the tetraquarks. We also evaluate the consequences of the partial r…

QuarkPhysicsDensity matrixParticle physicsLarge Hadron Collider010308 nuclear & particles physicsQuark model01 natural sciencesHadronization0103 physical sciencesWigner distribution functionTetraquark010306 general physicsWave functionPhysical Review D
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Nucleon Form Factors at high q2 within constituent quark models

2000

The nucleon form factors are calculated using a non-relativistic description in terms of constituent quarks. The emphasis is put on the reliability of present numerical methods used to solve the three-body problem in order to correctly reproduce the expected asymptotic behavior of form factors. Nucleon wave functions obtained in the hyperspherical formalism or employing Faddeev equations have been considered. While a q**(-8) behavior is expected at high q for a quark-quark force behaving like 1/r at short distances, it is found that the hypercentral approximation in the hyperspherical formalism (K=0) leads to a q**(-7) behavior. An infinite set of waves is required to get the correct behavi…

QuarkPhysicsFaddeev equationsInfinite set010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Numerical analysisNuclear Theory01 natural sciencesAtomic and Molecular Physics and OpticsMomentumAmplitude0103 physical sciencesFísica nuclear010306 general physicsNucleonWave functionMathematical physics
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Hyperspherical harmonic study of identical-flavor four-quark systems

2006

4 pages.-- ISI Article Identifier: 000248297600103.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0610287

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaWave-functionsQuantum numberHigh Energy Physics - PhenomenologyFormalism (philosophy of mathematics)High Energy Physics - Phenomenology (hep-ph)Quantum mechanicsHigh Energy Physics::ExperimentWave functionFlavor
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Extended van Royen-Weisskopf formalism for lepton-antilepton meson decay widths within non-relativistic quark models

2001

The classical van Royen-Weisskopf formula for the decay width of a meson into a lepton-antilepton pair is modified in order to include non-zero quark momentum contributions within the meson as well as relativistic effects. Besides, a phenomenological electromagnetic density for quarks is introduced. The meson wave functions are obtained from two different models: a chiral constituent quark model and a quark potential model including instanton effects. The modified van Royen-Weisskopf formula is found to improve systematically the results for the widths, giving an overall good description of all known decays.

QuarkPhysicsNuclear and High Energy PhysicsInstantonParticle physicsMesonNuclear Theory010308 nuclear & particles physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyConstituent quarkFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Formalism (philosophy of mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsRelativistic quantum chemistryWave functionLepton
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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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