Search results for "Chromodynamics"

showing 10 items of 1030 documents

QCD Jets at HERA II.O(? s 2 ) four-jet cross-sections

1989

We present exact expressions for theO(α s 2 ) tree graph four-jet cross-sections in neutral current and charged current deep inelasticep scattering initiated by quarks, antiquarks and gluons including lepton polarization effects. Using helicity amplitudes the partonic cross-sections are given in concise form including all colour, flavour and statistical factors. We explicate the electroweak coupling dependence and state how the partonic cross-sections are folded with the respective parton densities to obtain theep jet cross-sections toO(α s 2 ). We present some numerical results for the neutral current one-photon exchange case. We elaborate on the cut dependence of the jet rates and present…

QuarkQuantum chromodynamicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)Neutral currentHigh Energy Physics::PhenomenologyElectroweak interactionPartonHERAHelicityGluonNuclear physicsHigh Energy Physics::ExperimentEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
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Double Parton Distributions in Light-Front Constituent Quark Models

2014

Double parton distribution functions (dPDF), accessible in high energy proton-proton and proton nucleus collisions, encode information on how partons inside a proton are correlated among each other and could represent a tool to explore the 3D proton structure. In recent papers, double parton correlations have been studied in the valence quark region, by means of constituent quark models. This framework allows to understand clearly the dynamical origin of the correlations and to establish which, among the features of the results, are model independent. Recent relevant results, obtained in a relativistic light-front scheme, able to overcome some drawbacks of previous calculations, such as the…

QuarkQuantum chromodynamicsPhysicsParticle physicsValence (chemistry)Nuclear TheoryFísicaFOS: Physical sciencesConstituent quarkPartonAtomic and Molecular Physics and OpticsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution functionAtomic and Molecular PhysicsHomogeneous spaceCovariant transformationand OpticsNuclear ExperimentFew-Body Systems
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Double parton correlations in Light-Front constituent quark models

2014

Double parton distribution functions (dPDF) represent a tool to explore the 3D proton structure. They can be measured in high energy proton-proton and proton nucleus collisions and encode information on how partons inside a proton are correlated among each other. dPFDs are studied here in the valence quark region, by means of a constituent quark model, where two particle correlations are present without any additional prescription. This framework allows to understand the dynamical origin of the correlations and to clarify which, among the features of the results, are model independent. Use will be made of a relativistic light-front scheme, able to overcome some drawbacks of the previous cal…

QuarkQuantum chromodynamicsPhysicsParticle physicsValence (chemistry)Nuclear TheoryPhysicsQC1-999Nuclear TheoryFOS: Physical sciencesConstituent quarkPartonCovarianceNuclear Theory (nucl-th)Physics and Astronomy (all)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution functionHomogeneous spaceNuclear ExperimentEPJ Web of Conferences
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3-Loop Heavy Flavor Corrections in Deep-Inelastic Scattering with Two Heavy Quark Lines

2014

We consider gluonic contributions to the heavy flavor Wilson coefficients at 3-loop order in QCD with two heavy quark lines in the asymptotic region $Q^2 \gg m_{1(2)}^2$. Here we report on the complete result in the case of two equal masses $m_1 = m_2$ for the massive operator matrix element $A_{gg,Q}^{(3)}$, which contributes to the corresponding heavy flavor transition matrix element in the variable flavor number scheme. Nested finite binomial sums and iterated integrals over square-root valued alphabets emerge in the result for this quantity in $N$ and $x$-space, respectively. We also present results for the case of two unequal masses for the flavor non-singlet OMEs and on the scalar int…

QuarkQuantum chromodynamicsPhysicsParticle physicsWilson loopHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesDeep inelastic scatteringLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Field theory (psychology)High Energy Physics::ExperimentFlavor
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QCD thermodynamics with two flavours of Wilson fermions on large lattices

2012

We explore the phase diagram of two flavour QCD at vanishing chemical potential using dynamical O(a)-improved Wilson quarks. In the approach to the chiral limit we use lattices with a temporal extent of N_t=16 and spatial extent L=32,48 and 64 to enable the extrapolation to the thermodynamic limit with small discretisation effects. In addition to an update on the scans at constant \kappa, reported earlier, we present first results from scans along lines of constant physics at a pion mass of 290 MeV. We probe the transition using the Polyakov loop and the chiral condensate, as well as spectroscopic observables such as screening masses.

QuarkQuantum chromodynamicsPhysicsTheoretical physicsHigh Energy Physics - LatticeQuantum electrodynamicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesddc:530FermionLimit (mathematics)Phase diagram
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Longitudinal contribution to the alignment polarization of quarks produced in e + e - -annihilation: an O (α s ) effect

1996

We calculate the longitudinal contribution to the alignment polarization Pl of quarks produced in e+e− annihilation. In the Standard Model, the longitudinal alignment polarization vanishes at the Born term level and thus receives its first non-zero contribution from the O(αs) tree graph process. We provide analytical and numerical results for the longitudinal alignment polarization of massless and massive quarks, in particular for the recently discovered top quark.

QuarkQuantum chromodynamicsPhysicsTop quarkParticle physicsAnnihilationPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeElectron–positron annihilationHigh Energy Physics::PhenomenologyPolarization (waves)Massless particleNuclear physicsBorn approximationZeitschrift f�r Physik C Particles and Fields
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Polar angle dependence of the longitudinal polarization of quarks produced in e + e - -annihilation

1997

We calculate one-loop radiative QCD corrections to the three polarized and unpolarized structure functions that determine the beam-quark polar angle dependence of the longitudinal polarization of light and heavy quarks produced in e+e−-annihilations. We present analytical and numerical results for the longitudinal polarization and its polar angle dependence. We discuss in some detail the zero-mass limit of our results and the role of the anomalous spin-flip contributions to the polarization observables in the zero-mass limit. Our discussion includes transverse and longitudinal beam polarization effects.

QuarkQuantum chromodynamicsPhysicsTransverse planeAnnihilationPhysics and Astronomy (miscellaneous)Quantum electrodynamicsHigh Energy Physics::PhenomenologyStructure functionRadiative transferPhysics::Accelerator PhysicsPolar coordinate systemPolarization (waves)Zeitschrift f�r Physik C Particles and Fields
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s-channel single top quark production and decay at next-to-next-to-leading-order in QCD

2018

We report on a fully differential next-to-next-to-leading order (NNLO) calculation of s-channel single top (anti)quark production with a semileptonic decay at the LHC, neglecting the color correlation between the light and heavy quark lines and in the narrow width approximation. The NNLO corrections can increase the cross section by about 10% in the low transverse momentum region of the top quark and reduce scale variation uncertainty. In order to compare with experimental results without unfolding procedures, we also present theoretical predictions with fiducial cuts, including total cross sections and distributions of observables used in the experimental multivariate analysis. The NNLO co…

QuarkSemileptonic decayQuantum chromodynamicsPhysicsTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNuclear TheoryOrder (ring theory)Observable01 natural sciencesCross section (physics)0103 physical sciences010306 general physicsPhysical Review
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Perturbative generation of a strange-quark asymmetry in the nucleon

2004

We point out that perturbative evolution in QCD at three loops generates a strange-antistrange asymmetry s(x)-sbar(x) in the nucleon's sea just from the fact that the nucleon has non-vanishing up and down quark valence densities. The recently computed three-loop splitting functions allow for an estimate of this effect. We find that a fairly sizable asymmetry may be generated. Results for analogous asymmetries in the heavy-quark sector are also presented.

QuarkStrange quarkParticle physicsSTRANGECiencias Físicasmedia_common.quotation_subjectHigh Energy Physics::LatticeNuclear TheoryGeneral Physics and AstronomyDown quarkFOS: Physical sciencesStrangenessAsymmetry//purl.org/becyt/ford/1 [https]High Energy Physics - Phenomenology (hep-ph)PERTURBATIVENuclear Experimentmedia_commonPhysicsQuantum chromodynamicsValence (chemistry)High Energy Physics::PhenomenologyFísica//purl.org/becyt/ford/1.3 [https]AstronomíaHigh Energy Physics - PhenomenologyQuantum electrodynamicsASYMMETRYHigh Energy Physics::ExperimentNucleonCIENCIAS NATURALES Y EXACTAS
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Effective Field Theories for heavy probes in a hot QCD plasma and in the early universe

2016

International audience; There are many interesting problems in heavy-ion collisions and in cosmology that involve the interaction of a heavy particle with a medium. An example is the dissociation of heavy quarkonium seen in heavy-ion collisions. This was believed to be due to the screening of chromoelectric fields that prevents the heavy quarks from binding, however in the last years several perturbative and lattice computations have pointed out to the possibility that dissociation is due to the finite lifetime of a quarkonium state inside the medium. Regarding cosmology, the study of the behavior of heavy Majorana neutrinos in a hot medium is important to understand if this model can expla…

Quarkcosmological modelParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]QC1-999Populationdissociationquantum chromodynamics: plasma01 natural sciences7. Clean energydark matterCosmologythermalquarkonium: heavyBaryon asymmetryparticle: heavy0103 physical sciencesquantum chromodynamicseffective field theoriesheavy quarkNuclear Experiment010306 general physicseducationMajorana neutrinoslatticeeffective field theory: nonrelativisticQuantum chromodynamicsPhysicseducation.field_of_studyquantum chromodynamics: nonrelativisticquarkonium suppressionta114010308 nuclear & particles physicsPhysicsscreeningquarkonium: suppressionHigh Energy Physics::PhenomenologychromoelectricQuarkoniumheavy ionMAJORANAresummation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]baryon: asymmetryneutrino: Majoranaquarkonium: lifetimeNeutrinoQuark Confinement and the Hadron Spectrum
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