Search results for "quantum chromodynamics"

showing 10 items of 1027 documents

The strange-quark mass from QCD sum rules in the pseudoscalar channel

1997

QCD Laplace transform sum rules, involving the axial-vector current divergences, are used in order to determine the strange quark mass. The two-point function is known in QCD up to four loops in perturbation theory, and up to dimension-six in the non-perturbative sector. The hadronic spectral function is reconstructed using threshold normalization from chiral symmetry, together with experimental data for the two radial excitations of the kaon. The result for the running strange quark mass, in the $\bar{MS}$ scheme at a scale of 1 ${GeV}^{2}$ is: ${\bar m}_{s}(1 GeV^{2}) = 155 \pm 25 {MeV}$.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsQCD sum rulesStrange quarkLaplace transformHigh Energy Physics::LatticeHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)PseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentPerturbation theoryNuclear Experiment
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QCD vacuum condensates from tau-lepton decay data

2006

The QCD vacuum condensates in the Operator Product Expansion are extracted from the final ALEPH data on vector and axial-vector spectral functions from $\tau$-decay. Weighted Finite Energy Sum Rules are employed in the framework of both Fixed Order and Contour Improved Perturbation Theory. An overall consistent picture satisfying chirality constraints can be achieved only for values of the QCD scale below some critical value $\Lambda\simeq350 {MeV}$. For larger values of $\Lambda$, perturbation theory overwhelms the power corrections. A strong correlation is then found between $\Lambda$ and the resulting values of the condensates. Reasonable accuracy is obtained up to dimension $d=8$, beyon…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsQCD vacuumDimension (graph theory)FOS: Physical sciencesOrder (ring theory)LambdaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Operator product expansionPerturbation theory (quantum mechanics)LeptonJournal of High Energy Physics
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NLO corrections to processes with electroweak bosons at hadron colliders

2015

For many processes with electroweak bosons in the final state, next-to-leading order QCD and, in some cases, electroweak corrections have been calculated for differential cross sections at hadron colliders. The calculational techniques and some phenomenological implications are reviewed in this contribution. Processes discussed include vector boson fusion and vector boson scattering, production of two and three electroweak bosons, potentially with jets, (VV j, VV jj and VVV events) and some Higgs production processes. All QCD corrections are implemented in the publicly available VBFNLO program package.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsScatteringHigh Energy Physics::PhenomenologyElectroweak interactionHadronHiggs bosonHigh Energy Physics::ExperimentTechnicolorBosonVector bosonNuclear and Particle Physics Proceedings
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Prospects of medium tomography using back-to-back hadron correlations

2006

We discuss the prospects of extracting information about the bulk QCD matter distribution and evolution on the basis of hard hadronic back-to-back correlations in ultrarelativistic heavy-ion collisions. Using both hydrodynamical and parametrized evolution models for the spacetime evolution of the produced matter, which have been tested against RHIC data, we study six different setups for the spacetime dependence of hard-parton energy losses. Assuming that the energy loss of hard partons traversing the medium is radiative and calculable in the BDMPS formalism, we adjust one parameter, the quenching power scale, to the measured R_AA in each of the setups and study the systematic variations of…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsSpace timeCritical phenomenaHadronFOS: Physical sciencesObservablePartonNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferNuclear ExperimentQCD matter
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Charmonium properties in hot quenched lattice QCD

2012

We study the properties of charmonium states at finite temperature in quenched QCD on large and fine isotropic lattices. We perform a detailed analysis of charmonium correlation and spectral functions both below and above $T_c$. Our analysis suggests that both S wave states ($J/\psi$ and $\eta_c$) and P wave states ($\chi_{c0}$ and $\chi_{c1}$) disappear already at about $1.5 T_c$. The charm diffusion coefficient is estimated through the Kubo formula and found to be compatible with zero below $T_c$ and approximately $1/\pi T$ at $1.5 T_c\lesssim T\lesssim 3 T_c$.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsSpectral representationNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesLattice QCDRenormalizationNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeKubo formulaLattice (order)Condensed Matter::SuperconductivityQuark–gluon plasmaCondensed Matter::Strongly Correlated ElectronsHigh Energy Physics::ExperimentNuclear theory
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Order-$\alpha_s^3$ determination of the strange quark mass

1996

We present a QCD sum rule calculation of the strange-quark mass including four-loop QCD corrections to the correlator of scalar currents. We obtain $\bar m_s(1$ GeV$)=205.5\pm 19.1$ MeV.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsStrange quarkHigh Energy Physics::LatticeScalar (mathematics)Nuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyOrder (group theory)High Energy Physics::ExperimentSum rule in quantum mechanicsNuclear Experiment
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NNLL momentum-space threshold resummation in direct top quark production at the LHC

2014

We update the theoretical precision of the total cross section for direct top quark production at the LHC by extending the threshold resummation to the next-to-next-to-leading logarithmic accuracy.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkLarge Hadron ColliderLogarithmHigh Energy Physics::PhenomenologyFOS: Physical sciencesPosition and momentum spaceHigh Energy Physics - ExperimentNonlinear Sciences::Chaotic DynamicsCross section (physics)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Production (computer science)Resummation
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Scrutinizing the Green's functions of QCD: Lattice meets Schwinger-Dyson

2009

Proceedings of the International Workshop Light Cone 2009 (LC2009): Relativistic Hadronic and Particle Physics. Sao Jose dos Campos, Brazil, July 8-13, 2009.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsTruncationHigh Energy Physics::LatticeMass generationHigh Energy Physics::PhenomenologyEquations of motionFOS: Physical sciencesFísicaFunction (mathematics)Atomic and Molecular Physics and OpticsGluonHigh Energy Physics - PhenomenologyLattice (module)Theoretical physicsHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Gauge theory
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Gauge-invariant resummation formalism for two-point correlation functions

1996

The consistent description of unstable particles, renormalons, or other Schwinger--Dyson-type of solutions within the framework of perturbative gauge field theories necessitates the definition and resummation of off-shell Green's functions, which must respect several crucial physical requirements. A formalism is presented for resummation of off-shell two-point correlation functions, which is mainly based on arguments of analyticity, unitarity, gauge invariance and renormalizability. The analytic results obtained with various methods, including the background field gauges and the pinch technique are confronted with the physical requirements imposed; to one-loop order the pinch technique appr…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaRenormalization groupRenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Gauge theoryPerturbation theory (quantum mechanics)UniquenessResummationPhysical Review D
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Effective field theory description of the pion form factor

1997

7 páginas, 2 figuras.-- PACS: 14.40.Aq; 13.40.Gp; 13.6O.Fz; 12.39.Fe.-- arXiv:hep-ph/9707347v1

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityHigh Energy Physics::PhenomenologyHadronForm factor (quantum field theory)FOS: Physical sciencesFísicaOrder (ring theory)Expression (computer science)Form factorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionChiral perturbation theoryPionEffective field theoryHigh Energy Physics::ExperimentNuclear Experiment
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