Search results for "kvarkit"

showing 10 items of 27 documents

Direct observation of the dead-cone effect in quantum chromodynamics.

2022

In particle collider experiments, elementary particle interactions with large momentum transfer produce quarks and gluons (known as partons) whose evolution is governed by the strong force, as described by the theory of quantum chromodynamics (QCD)1. These partons subsequently emit further partons in a process that can be described as a parton shower2, which culminates in the formation of detectable hadrons. Studying the pattern of the parton shower is one of the key experimental tools for testing QCD. This pattern is expected to depend on the mass of the initiating parton, through a phenomenon known as the dead-cone effect, which predicts a suppression of the gluon spectrum emitted by a he…

ALICE CollaborationkvarkitGeneral Science & TechnologykvanttiväridynamiikkahiukkasfysiikkaGeneral
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Massive quarks in NLO dipole factorization for DIS : Transverse photon

2022

We calculate the light cone wave functions for the QCD Fock components in a transverse virtual photon necessary for applications at next-to-leading order in the QCD coupling, including quark masses. We present a detailed calculation of both the one loop wave function for the quark-antiquark Fock component and the tree level wave function for the quark-antiquark-gluon Fock component. The quark masses are renormalized in the pole mass scheme, satisfying constraints from the requirement of Lorentz invariance. In particular the quark Pauli form factor at NLO is recovered from the on-shell limit of the quark-antiquark Fock component. We use our result to calculate the next-to-leading order corre…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)fotonitkvarkitHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::Experimentsirontakvanttiväridynamiikkahiukkasfysiikka114 Physical sciences
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Massive Quarks at One Loop in the Dipole Picture of Deep Inelastic Scattering

2022

We calculate the light cone wave functions for a virtual photon to split into quark-antiquark states, including for the first time quark masses at one loop accuracy. These wave functions can be used to calculate cross sections for several precision probes of perturbative gluon saturation at the Electron-Ion Collider. Using these wave functions we derive, for the first time, the dipole picture DIS cross sections at one loop for longitudinal and transverse virtual photons including quark masses. The quark masses are renormalized in the pole mass scheme, satisfying constraints from the requirement of Lorentz invariance of the quark Dirac and Pauli form factors.

High Energy Physics - TheorykvarkitHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical scienceshiukkasfysiikka114 Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)sirontaHigh Energy Physics::ExperimentPhysical Review Letters
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Diquark correlations in hadron physics: Origin, impact and evidence

2020

The last decade has seen a marked shift in how the internal structure of hadrons is understood. Modern experimental facilities, new theoretical techniques for the continuum bound-state problem and progress with lattice-regularised QCD have provided strong indications that soft quark+quark (diquark) correlations play a crucial role in hadron physics. For example, theory indicates that the appearance of such correlations is a necessary consequence of dynamical chiral symmetry breaking, viz. a corollary of emergent hadronic mass that is responsible for almost all visible mass in the universe; experiment has uncovered signals for such correlations in the flavour-separation of the proton's elect…

Nuclear TheoryHigh Energy Physics::LatticeHadronNuclear Theoryhiukkasfysiikka01 natural sciencesHigh Energy Physics - ExperimentBroad spectrumHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentQuantum chromodynamicsPhysicsDiquark correlationsBaryon spectra and structureHigh Energy Physics - Lattice (hep-lat)symmetry breaking: chiralDyson-Schwinger equationsDiquarkbound statediquark: correlationHigh Energy Physics - PhenomenologyQuark modelsChiral symmetry breakingPhenomenology (particle physics)QuarkNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]diquark correlationsNuclear Theory (nucl-th)High Energy Physics - Latticehadron physics0103 physical sciencesquantum chromodynamics010306 general physicsBaryon spectra and structure; Diquark correlations; Dyson-Schwinger equations; Lattice quantum chromodynamics; Quantum chromodynamics; Quark modelskvarkit010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]hadron spectroscopyHigh Energy Physics::PhenomenologyLattice quantum chromodynamicsform factor: electromagnetic[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Linearly polarized gluons and axial charge fluctuations in the glasma

2018

We calculate of the one- and two-point correlation functions of the energy density and the divergence of the Chern-Simons current in the nonequilibrium Glasma state formed in a high-energy nuclear collision. We show that the latter depends on the difference of the total and linearly polarized gluon transverse momentum distributions. Since the divergence of the Chern-Simons current provides the source of axial charge, we infer information about the statistical properties of axial charge production at early times. We further develop a simple phenomenological model to characterize axial charge distributions in terms of distributions of the energy density.

Nuclear Theoryquark-gluon plasmaField (physics)FLOWFOS: Physical sciencesparticle productionNon-equilibrium thermodynamicsHEAVY-ION COLLISIONS114 Physical sciences01 natural sciencesHYDRODYNAMICSNuclear Theory (nucl-th)hiukkasetHigh Energy Physics - Phenomenology (hep-ph)nuclear physicsCONDENSATE0103 physical sciencesPhenomenological modelFIELD010306 general physicsDivergence (statistics)plasmaPhysicsta114ionitkvarkit010308 nuclear & particles physicsLinear polarizationkvarkki-gluoniplasmaCharge densityCharge (physics)EVOLUTIONGluonHigh Energy Physics - PhenomenologyDENSITYQuantum electrodynamicsENERGY NUCLEAR COLLISIONSAtomic physicsydinfysiikkarelativistic heavy-ion collisionsPhysical Review
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Measurement of beauty production via non-prompt D0 mesons in Pb-Pb collisions at √sNN = 5.02 TeV

2022

The production of non-prompt D0 mesons from beauty-hadron decays was measured at midrapidity (|y| 5 GeV/c in the 0–10% central Pb-Pb collisions. The data are described by models that include both collisional and radiative processes in the calculation of beauty-quark energy loss in the quark-gluon plasma, and quark recombination in addition to fragmentation as a hadronisation mechanism. The ratio of the non-prompt to prompt D0-meson RAA is larger than unity for pT> 4 GeV/c in the 0–10% central Pb-Pb collisions, as predicted by models in which beauty quarks lose less energy than charm quarks in the quark-gluon plasma because of their larger mass. [Figure not available: see fulltext.]

Nuclear and High Energy PhysicsHeavy Ion ExperimentskvarkitHeavy Quark ProductionhiukkasfysiikkaQuark Gluon Plasmaydinfysiikka
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Forward quark jet-nucleus scattering in a light-front Hamiltonian approach

2020

We investigate the scattering of a quark jet on a high-energy heavy nucleus using the time-dependent light-front Hamiltonian approach. We simulate a real-time evolution of the quark in a strong classical color field of the relativistic nucleus, described as the Color Glass Condensate. We study the sub-eikonal effect by letting the quark jet carry realistic finite longitudinal momenta, and we find sizeable changes on the transverse coordinate distribution of the quark. We also observe the energy loss of the quark through gluon emissions in the $\ket{q}+\ket{qg}$ Fock space. This approach provides us with an opportunity to study scattering processes from non-perturbative aspects.

PhysicsQuarkParticle physicsField (physics)Nuclear TheoryScatteringkvarkitHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesJet (particle physics)hiukkasfysiikka114 Physical sciencesFock spaceGluonColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentydinfysiikkaNuclear ExperimentHamiltonian (control theory)
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Applicability of pion-nucleus Drell-Yan data in global analysis of nuclear parton distribution functions

2017

Despite the success of modern nuclear parton distribution functions (nPDFs) in describing nuclear hard-process data, they still suffer from large uncertainties. One of the poorly constrained features is the possible asymmetry in nuclear modifications of valence $u$ and $d$ quarks. We study the possibility of using pion-nucleus Drell-Yan dilepton data as a new constraint in the global analysis of nPDFs. We find that the nuclear cross-section ratios from the NA3, NA10 and E615 experiments can be used without imposing significant new theoretical uncertainties and, in particular, that these datasets may have some constraining power on the $u$/$d$ -asymmetry in nuclei.

QuarkDrell-Yan processParticle physicsNuclear and High Energy PhysicsNuclear Theorymedia_common.quotation_subjectNuclear TheoryDrell–Yan processFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciencesAsymmetry114 Physical sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)PionRATIO0103 physical sciencesmedicinePion–nucleus scatteringNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear theoryNuclear Experimentmedia_commonPhysicsta114010308 nuclear & particles physicskvarkitHigh Energy Physics::PhenomenologyDrell–Yan processNuclear parton distribution functionsPion-nucleus scatteringlcsh:QC1-999pion–nucleus scatteringnuclear parton distribution functionsHigh Energy Physics - PhenomenologyDistribution functionmedicine.anatomical_structureDIMUON PRODUCTIONHigh Energy Physics::ExperimentNucleusPDFSlcsh:Physics
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Exclusive heavy vector meson production at next-to-leading order in the dipole picture

2021

We calculate exclusive production of a longitudinally polarized heavy vector meson at next-to-leading order in the dipole picture. The large quark mass allows us to separately include both the first QCD correction proportional to the coupling constant $\alpha_s$, and the first relativistic correction suppressed by the quark velocity $v^2$. Both of these corrections are found to be numerically important in $\mathrm{J}/\psi$ production. The results obtained are directly suitable for phenomenological calculations. We also demonstrate how vector meson production provides complementary information to structure function analyses when one extracts the initial condition for the energy evolution of …

QuarkNuclear and High Energy PhysicsParticle physicsCOLLISIONSProtonJ/PSI MESONSQC1-999High Energy Physics::LatticeNuclear TheoryStructure (category theory)FOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesInitial value problemVector meson010306 general physicsNUCLEUSPhysicsCoupling constantQuantum chromodynamicskvarkit010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyELECTROPRODUCTIONEVOLUTIONDipoleHigh Energy Physics - PhenomenologyPHOTOPRODUCTIONHigh Energy Physics::Experiment
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Quark Structure of the X (4500), X (4700) and χc(4P,5P) States

2021

We study some of the main properties (masses and open-flavor strong decay widths) of 4P and 5P charmonia. While there are two candidates for the χc0(4P,5P) states, the X(4500) and X(4700), the properties of the other members of the χc(4P,5P) multiplets are still completely unknown. With this in mind, we start to explore the charmonium interpretation for these mesons. Our second goal is to investigate if the apparent mismatch between the Quark Model (QM) predictions for χc0(4P,5P) states and the properties of the X(4500) and X(4700) mesons can be overcome by introducing threshold corrections in the QM formalism. According to our coupled-channel model results for the threshold mass shifts, th…

QuarkParticle physicsMesonFormalism (philosophy)QC1-999Materials Science (miscellaneous)BiophysicsStructure (category theory)General Physics and Astronomystrong decayshiukkasfysiikka01 natural sciencesInterpretation (model theory)charmonia phenomenology0103 physical sciencesPhysical and Theoretical Chemistry010306 general physics3P0 modelMathematical PhysicsPhysicsquark modelkvarkit010308 nuclear & particles physicsPhysicsexotic statesQuark modelunquenched quark modelHigh Energy Physics - PhenomenologycharmoniaydinfysiikkaFrontiers in Physics
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