Search results for "Names"

showing 10 items of 6843 documents

TRANSVERSE MOMENTUM-DEPENDENT PARTON DISTRIBUTIONS FROM LATTICE QCD

2012

Starting from a definition of transverse momentum-dependent parton distributions for semi-inclusive deep inelastic scattering and the Drell-Yan process, given in terms of matrix elements of a quark bilocal operator containing a staple-shaped Wilson connection, a scheme to determine such observables in lattice QCD is developed and explored. Parametrizing the aforementioned matrix elements in terms of invariant amplitudes permits a simple transformation of the problem to a Lorentz frame suited for the lattice calculation. Results for the Sivers and Boer-Mulders transverse momentum shifts are presented, focusing in particular on their dependence on the staple extent and the Collins-Soper evol…

QuarkPhysicsParticle physicsHigh Energy Physics::LatticeLorentz transformationHigh Energy Physics::PhenomenologyObservablePartonLattice QCDDeep inelastic scatteringTransverse planesymbols.namesakeLattice (order)symbolsHigh Energy Physics::ExperimentInternational Journal of Modern Physics: Conference Series
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Probing the chiral weak Hamiltonian at finite volumes

2006

Non-leptonic kaon decays are often described through an effective chiral weak Hamiltonian, whose couplings ("low-energy constants") encode all non-perturbative QCD physics. It has recently been suggested that these low-energy constants could be determined at finite volumes by matching the non-perturbatively measured three-point correlation functions between the weak Hamiltonian and two left-handed flavour currents, to analytic predictions following from chiral perturbation theory. Here we complete the analytic side in two respects: by inspecting how small ("epsilon-regime") and intermediate or large ("p-regime") quark masses connect to each other, and by including in the discussion the two …

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsChiral perturbation theoryHigh Energy Physics - Lattice (hep-lat)FlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableweak decaysPseudoscalarsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Latticelattice QCDkaon physicssymbolschiral lagrangiansHamiltonian (quantum mechanics)Mathematical physics
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Massive Yang-Mills model and diffractive scattering

1998

We argue that the massive Yang-Mills model of Kunimasa and Goto, Slavnov, and Cornwall, in which massive gauge vector bosons are introduced in a gauge-invariant way without resorting to the Higgs mechanism, may be useful for studying diffractive scattering of strongly interacting particles. We perform in this model explicit calculations of S-matrix elements between quark states, at tree level, one loop, and two loops, and discuss issues of renormalisability and unitarity. In particular, it is shown that the S-matrix element for quark scattering is renormalisable at one-loop order and is only logarithmically non-renormalisable at two loops. The discrepancies in the ultraviolet regime between…

QuarkPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsUnitarityHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaGluonsymbols.namesakePomeronHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentHiggs mechanismParticle Physics - PhenomenologyS-matrixBoson
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About two equivalent descriptions of quark antisymmetrization

1992

We analyze the wave function for a two-hadron system when the quark symmetrization principle is incorporated. Two alternative mathematical descriptions are considered. The representation method of Hund constructs a system of generators of thesinglet⊗singlet type. The method of Young-Froebenius incorporates hidden-color components in order to describe the representation basis. By taking a naive model we show that the two descriptions, are equivalent and thus no physical meaning should be attached to their mathematical differences. The results of our analysis are then applied to the more realisticN-N (deuteron) system. We end by discussing the structure of the Pauli correlations which we comp…

QuarkPhysicsTheoretical physicssymbols.namesakeClassical mechanicsPauli exclusion principleBasis (linear algebra)symbolsSymmetrizationFunction (mathematics)Quantum field theoryRepresentation (mathematics)Wave functionIl Nuovo Cimento A
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QCD exotics versus a standard model Higgs boson

2012

The present collider data put severe constraints on any type of new strongly interacting particle coupling to the Higgs boson. We analyze the phenomenological limits on exotic quarks belonging to nontriplet $SU(3{)}_{C}$ representations and their implications on Higgs searches. The discovery of the standard model Higgs, in the experimentally allowed mass range, would exclude the presence of exotic quarks coupling to it. Thus, such QCD particles could only exist provided that their masses do not originate in the SM Higgs mechanism.

QuarkQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaElementary particleCoupling (probability)Standard ModelHiggs fieldsymbols.namesakeHiggs bosonsymbolsHigh Energy Physics::ExperimentHiggs mechanism
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Gauge-invariant on-shellZ 2 in QED, QCD and the effective field theory of a static quark

1991

We calculate theon-shell fermion wave-function renormalization constantZ 2 of a general gauge theory, to two loops, inD dimensions and in an arbitrary covariant gauge, and find it to be gauge-invariant. In QED this is consistent with the dimensionally regularized version of the Johnson-Zumino relation: d logZ 2/da 0=i(2π)−D e 0 2 ∫d D k/k 4=0. In QCD it is, we believe, a new result, strongly suggestive of the cancellation of the gauge-dependent parts of non-abelian UV and IR anomalous dimensions to all orders. At the two-loop level, we find that the anomalous dimension γ F of the fermion field in minimally subtracted QCD, withN L light-quark flavours, differs from the corresponding anomalou…

QuarkQuantum chromodynamicsPhysicsParticle physicsFermionic fieldPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFermionRenormalizationsymbols.namesakeEffective field theorysymbolsCovariant transformationGauge theoryEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
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Semileptonic decays of double heavy baryons in a relativistic constituent three-quark model

2009

We study the semileptonic decays of double heavy baryons using a manifestly Lorentz covariant constituent three-quark model. We present complete results on transition form factors between double-heavy baryons for finite values of the heavy quark/baryon masses and in the heavy quark symmetry limit which is valid at and close to zero recoil. Decay rates are calculated and compared to each other in the full theory, keeping masses finite, and also in the heavy quark limit.

QuarkSemileptonic decayNuclear and High Energy PhysicsParticle physicsLorentz transformationHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesLorentz covariance01 natural sciencesNuclear physicssymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsQuark modelHigh Energy Physics::PhenomenologyVertex functionCharmed baryonsBaryonHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::Experiment
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Scattering and gluon emission in a color field : a light-front Hamiltonian approach

2021

We develop a numerical method to nonperturbatively study scattering and gluon emission of a quark from a colored target using a light-front Hamiltonian approach. The target is described as a classical color field, as in the color glass condensate effective theory. The Fock space of the scattering system is restricted to the |q⟩+|qg⟩ sectors, but the time evolution of this truncated system is solved exactly. This method allows us to study the interplay between coherence and multiple scattering in gluon emission. It could be applied both to studying subeikonal effects in high-energy scattering and to understanding jet quenching in a hot plasma.

Quarkelectron-ion collisionsNuclear TheoryField (physics)High Energy Physics::LatticeFOS: Physical scienceshiukkasfysiikka114 Physical sciences01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesquantum chromodynamicsEffective field theory010306 general physicsquantum field theoryPhysics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyTime evolutionGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicssymbolskvanttiväridynamiikkakvanttikenttäteoriaHamiltonian (quantum mechanics)relativistic heavy-ion collisions
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Planar Mappings of Finite Distortion

2010

We review recent results on planar mappings of finite distortion. This class of mappings contains all analytic functions and quasiconformal mappings.

Quasiconformal mappingClass (set theory)Mathematics::Complex VariablesApplied MathematicsMathematical analysisDistortion (mathematics)symbols.namesakePlanarComputational Theory and MathematicsJacobian matrix and determinantsymbolsCoincidence pointAnalysisAnalytic functionMathematicsComputational Methods and Function Theory
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Oligophenylenevinylenes in Spatially Confined Nanochannels: Monitoring Intermolecular Interactions by UV/Vis and Raman Spectroscopy

2008

Perhydrotriphenylene-based channel-forming inclusion compounds (ICs) and thin films made of polyphenylenevinylene (PPV)-type oligomers with terminal alkoxy groups are investigated and compared in a combined experimental and theoretical approach. Interchromophore interactions and host-guest interactions are elucidated by UV/Vis and Raman spectroscopy. The impact of the local environment of the chromophore on the optical and photophysical properties is discussed in light of quantum-chemical calculations. In stark contrast to thin films where preferential side-by-side orientation leads to quenching of photoluminescence (PL) via non-emissive traps, the ICs are found to be attractive materials f…

Quenching (fluorescence)Materials sciencePhotoluminescenceIntermolecular forceAnalytical chemistryChromophoreCondensed Matter PhysicsPhotochemistryElectronic Optical and Magnetic MaterialsBiomaterialssymbols.namesakeUltraviolet visible spectroscopynanochannels inclusion compoundsElectrochemistryAlkoxy groupsymbolsThin filmRaman spectroscopyFIS/03 - FISICA DELLA MATERIA
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