Search results for " QCD"

showing 10 items of 463 documents

Measurement of Event Shape and Inclusive Distributions at $\sqrt{s} =$ 130 and 136 GeV

1997

Inclusive charged particle and event shape distributions are measured using 321 hadronic events collected with the DELPHI experiment at LEP at effective centre of mass energies of 130 to 136 GeV. These distributions are presented and compared to data at lower energies, in particular to the precise Z data. Fragmentation models describe the observed changes of the distributions well. The energy dependence of the means of the event shape variables can also be described using second order QCD plus power terms. A method independent of fragmentation model corrections is used to determine $\alpha_s$ from the energy dependence of the mean thrust and heavy jet mass. It is measured to be: % %\alpha_s…

High energyParticle physicsZ(0) RESONANCEPhysics and Astronomy (miscellaneous)Electron–positron annihilationHADRONIC Z-DECAYS; E+E-ANNIHILATION; ALPHA-S; POWER CORRECTIONS; Z(0) RESONANCE; MONTE-CARLO; QCD MODELS; ENERGY; FRAGMENTATION; PREDICTIONSHadronPREDICTIONSThrust01 natural sciences7. Clean energyPartícules (Física nuclear)Nuclear physicsENERGYFragmentation (mass spectrometry)POWER CORRECTIONSMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ALPHA-S010306 general physicsDetectors de radiacióDELPHIPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyE+E-ANNIHILATIONLARGE ELECTRON POSITRON COLLIDERCharged particleHADRONIC Z-DECAYSLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIQCD MODELSPARTICLE PHYSICSHigh Energy Physics::ExperimentFRAGMENTATIONParticle Physics - Experiment
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A new lattice action for studying topological charge

1996

We propose a new lattice action for non-abelian gauge theories, which will reduce short-range lattice artifacts in the computation of the topological susceptibility. The standard Wilson action is replaced by the Wilson action of a gauge covariant interpolation of the original fields to a finer lattice. If the latter is fine enough, the action of all configurations with non-zero topological charge will satisfy the continuum bound. As a simpler example we consider the $O(3)$ $\sigma$-model in two dimensions, where a numerical analysis of discretized continuum instantons indicates that a finer lattice with half the lattice spacing of the original is enough to satisfy the continuum bound.

InstantonNuclear and High Energy PhysicsHigh Energy Physics::LatticeLattice field theoryFOS: Physical sciencesTheoretical physicsLattice constantHigh Energy Physics - LatticeHamiltonian lattice gauge theoryLattice (order)Lattice gauge theoryCovariant transformationGauge theoryScalingTopological quantum numberMathematicsPhysicsQuantum gauge theoryNumerical analysisHigh Energy Physics - Lattice (hep-lat)FísicaLattice QCDMap of latticesAtomic and Molecular Physics and OpticsReciprocal latticeQuantum electrodynamicsLattice model (physics)Nuclear Physics B - Proceedings Supplements
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B-K-parameter from N-f=2 twisted mass lattice QCD

2011

We present an unquenched N-f = 2 lattice computation of the B-K parameter which controls K-0 - (K) over bar (0) oscillations. A partially quenched setup is employed with two maximally twisted dynamical (sea) light Wilson quarks, and valence quarks of both the maximally twisted and the Osterwalder-Seiler variety. Suitable combinations of these two kinds of valence quarks lead to a lattice definition of the B-K parameter which is both multiplicatively renormalizable and O(a) improved. Employing the nonperturbative RI-MOM scheme, in the continuum limit and at the physical value of the pion mass we get B-K(RGI) = 0.729 +/- 0.030, a number well in line with the existing quenched and unquenched d…

K-antiK mixing; indirect CP violation; Lattice QCDHigh Energy Physics::LatticeHigh Energy Physics::Phenomenologyindirect CP violationFísicaK-antiK mixingLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi Matematici
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Search for the H-Dibaryon in two flavor Lattice QCD

2016

Parikshit Junnarkar∗, Anthony Francis, Jeremy Green, Chuan Miao, Thomas Rae, Hartmut Wittig Helmholtz-Institut Mainz, Institut fur Kernphysik, and PRISMA Cluster of Excellence, Johannes Gutenberg-Universitat Mainz, Germany Department of Physics and Astronomy, York University, Toronto Canada Bergische Universitat Wuppertal, Germany E-mail: junnarka@kph.uni-mainz.de, afranc@yorku.ca, green@kph.uni-mainz.de, chuan@kph.uni-mainz.de, thrae@uni-wuppertal.de, wittig@kph.uni-mainz.de

Lattice QCDHumanitiesProceedings of The 33rd International Symposium on Lattice Field Theory — PoS(LATTICE 2015)
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Static and non-static vector screening masses

2016

Thermal screening masses of the conserved vector current are calculated both in a weak-coupling approach and in lattice QCD. The inverse of a screening mass can be understood as the length scale over which an external electric field is screened in a QCD medium. The comparison of screening masses both in the zero and non-zero Matsubara frequency sectors shows good agreement of the perturbative and the lattice results. Moreover, at $T\approx 508\mathrm{MeV}$ the lightest screening mass lies above the free result ($2\pi T$), in agreement with the $\mathcal{O}(g^2)$ weak-coupling prediction.

Length scalePhysicsQuantum chromodynamicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice field theoryFOS: Physical sciencesMatsubara frequencyLattice QCDHigh Energy Physics - LatticeLattice (order)Quantum electrodynamicsPerturbation theory (quantum mechanics)Mass screening
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Measurement of the Generalized Polarizabilities of the Proton at Intermediate $Q^2$

2021

Background: Generalized polarizabilities (GPs) are important observables to describe the nucleon structure, and measurements of these observables are still scarce. Purpose: This paper presents details of a virtual Compton scattering (VCS) experiment, performed at the A1 setup at the Mainz Microtron by studying the $e p \to e p \gamma$ reaction. The article focuses on selected aspects of the analysis. Method: The experiment extracted the $P_{LL} -P_{TT} / \epsilon$ and $P_{LT}$ structure functions, as well as the electric and magnetic GPs of the proton, at three new values of the four-momentum transfer squared $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$. Results: We emphasize the importance of the ca…

MAINZ-A1ProtonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]higher-orderHadronic Physics and QCDFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]momentum transfer dependence01 natural scienceselectron p: scatteringNuclear Theory (nucl-th)Cross section (physics)High Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesCalibrationp: structure functionNuclear Experiment (nucl-ex)010306 general physicsMicrotronNuclear ExperimentPhysics010308 nuclear & particles physicsCompton scatteringObservablecross section: measuredcalibrationComputational physicsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]p: polarizabilityelectron p --> electron p photonNucleonCompton scatteringexperimental results
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Measurement of azimuthal asymmetries associated with deeply virtual Compton scattering on a longitudinally polarized deuterium target

2010

Azimuthal asymmetries in exclusive electroproduction of a real photon from a longitudinally polarized deuterium target are measured with respect to target polarization alone and with respect to target polarization combined with beam helicity and/or beam charge. The asymmetries appear in the distribution of the real photons in the azimuthal angle $\phi$ around the virtual photon direction, relative to the lepton scattering plane. The asymmetries arise from the deeply virtual Compton scattering process and its interference with the Bethe-Heitler process. The results for the beam-charge and beam-helicity asymmetries from a tensor polarized deuterium target with vanishing vector polarization ar…

Nuclear and High Energy Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyEVOLUTION KERNELS010308 nuclear & particles physicsGENERALIZED PARTON DISTRIBUTIONS; IMPACT PARAMETER SPACE; ELECTRON STORAGE-RING; EVOLUTION KERNELS; HERA; SPIN; NUCLEON; QCDHERAIMPACT PARAMETER SPACEFOS: Physical sciencesQCD01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ELECTRON STORAGE-RINGSPINGENERALIZED PARTON DISTRIBUTIONS0103 physical sciencesddc:530High Energy Physics::ExperimentSDG 7 - Affordable and Clean EnergyNUCLEON010306 general physics
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Latest predictions from the EbyE NLO EKRT model

2019

We present the latest results from the NLO pQCD + saturation + viscous hydrodynamics (EbyE NLO EKRT) model. The parameters in the EKRT saturation model are fixed by the charged hadron multiplicity in the 0-5 \% 2.76 TeV Pb+Pb collisions. The $\sqrt{s}$, $A$ and centrality dependence of the initial particle production follows then from the QCD dynamics of the model. This allows us to predict the $\sqrt{s}$ and $A$ dependence of the particle production. We show that our results are in an excellent agreement with the low-$p_T$ data from 2.76 TeV and 5.02 TeV Pb+Pb collisions at the LHC as well as with the data from the 200 GeV Au+Au collisions at RHIC. In particular, we study the centrality de…

Nuclear and High Energy PhysicsCOLLISIONSMULTIPLICITIESNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesdissipative fluid dynamicNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsTRANSVERSE ENERGIESNuclear ExperimentNuclear theoryMass numberQuantum chromodynamicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicssaturationHigh Energy Physics::PhenomenologyMultiplicity (mathematics)heavy-ion collisionsCharged particleHigh Energy Physics - PhenomenologyHigh Energy Physics::Experimentperturbative QCD calculationsydinfysiikka
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Broad excitations in a 2+1D overoccupied gluon plasma

2021

Motivated by the initial stages of high-energy heavy-ion collisions, we study excitations of far-from-equilibrium 2+1 dimensional gauge theories using classical-statistical lattice simulations. We evolve field perturbations over a strongly overoccupied background undergoing self-similar evolution. While in 3+1D the excitations are described by hard-thermal loop theory, their structure in 2+1D is nontrivial and nonperturbative. These nonperturbative interactions lead to broad excitation peaks in spectral and statistical correlation functions. Their width is comparable to the frequency of soft excitations, demonstrating the absence of soft quasiparticles in these theories. Our results also su…

Nuclear and High Energy PhysicsCOLLISIONSNuclear TheoryField (physics)FOS: Physical sciencesLattice QCDQC770-798hiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesPerturbative QCDfysikkField theory (psychology)Gauge theory010306 general physicsKINETIC-THEORYUNIVERSAL DYNAMICSPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]MASS SCALENUCLEI010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)kvarkki-gluoniplasmaPerturbative QCDLattice QCDFIELD-THEORY3. Good healthGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsQuark–gluon plasmaQuasiparticleQuark-Gluon PlasmaGAUGE-THEORIESJournal of High Energy Physics
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Properties of the ground-state baryons in chiral perturbation theory

2010

15th High Energy Physics International Conference on Quantum Chromodynamics. Montpellier (FRANCE). JUN 28-JUL 02, 2010

Nuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryLattice field theoryExtrapolationFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)Theoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeChiral perturbation theoryNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyHyperonLattice QCDAtomic and Molecular Physics and OpticsBaryonHigh Energy Physics - PhenomenologyCoupling (physics)Baryon structureGround stateNuclear Physics B - Proceedings Supplements
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