Search results for "PROPAGATOR"

showing 10 items of 173 documents

Effects of divergent ghost loops on the Green’s functions of QCD

2013

In the present work we discuss certain characteristic features encoded in some of the fundamental QCD Green's functions, whose origin can be traced back to the nonperturbative masslessness of the ghost field, in the Landau gauge. Specifically, the ghost loops that contribute to these Green's functions display infrared divergences, akin to those encountered in the perturbative treatment, in contradistinction to the gluonic loops, whose perturbative divergences are tamed by the dynamical generation of an effective gluon mass. In d=4, the aforementioned divergences are logarithmic, thus causing a relatively mild impact, whereas in d=3 they are linear, giving rise to enhanced effects. In the ca…

High Energy Physics - TheoryQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsToy modelLogarithmHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPropagatorIntegral equationGluonHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)Lattice (order)Quantum electrodynamicsPhysical Review D
researchProduct

Born amplitudes in QCD from scalar diagrams

2005

We review recent developments for the calculation of Born amplitudes in QCD. This includes the computation of gluon helicity amplitudes from MHV vertices and an approach based on scalar propagators and a set of three- and four-valent vertices. The latter easily generalizes to amplitudes with any number of quark pairs. The quarks may be massless or massive.

High Energy Physics - TheoryQuantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsParticle physicsComputationHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyScalar (physics)PropagatorFOS: Physical sciencesHelicityAtomic and Molecular Physics and OpticsGluonMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::Experiment
researchProduct

The Nielsen identities for the two-point functions of QED and QCD

1994

We consider the Nielsen identities for the two-point functions of full QCD and QED in the class of Lorentz gauges. For pedagogical reasons the identities are first derived in QED to demonstrate the gauge independence of the photon self-energy, and of the electron mass shell. In QCD we derive the general identity and hence the identities for the quark, gluon and ghost propagators. The explicit contributions to the gluon and ghost identities are calculated to one-loop order, and then we show that the quark identity requires that in on-shell schemes the quark mass renormalisation must be gauge independent. Furthermore, we obtain formal solutions for the gluon self-energy and ghost propagator i…

High Energy Physics - TheoryQuarkPhotonPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeLorentz transformationNuclear TheoryFOS: Physical sciences01 natural sciencesHigh Energy Physics::Theorysymbols.namesakeIdentity (mathematics)0103 physical sciences010306 general physicsEngineering (miscellaneous)Mathematical physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPropagatorGauge (firearms)GluonHigh Energy Physics - Theory (hep-th)symbolsHigh Energy Physics::ExperimentZeitschrift für Physik C Particles and Fields
researchProduct

Chiral symmetry breaking with lattice propagators

2010

We study chiral symmetry breaking using the standard gap equation, supplemented with the infrared-finite gluon propagator and ghost dressing function obtained from large-volume lattice simulations. One of the most important ingredients of this analysis is the non-abelian quark-gluon vertex, which controls the way the ghost sector enters into the gap equation. Specifically, this vertex introduces a numerically crucial dependence on the ghost dressing function and the quark-ghost scattering amplitude. This latter quantity satisfies its own, previously unexplored, dynamical equation, which may be decomposed into individual integral equations for its various form factors. In particular, the sca…

High Energy Physics - TheoryQuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Lattice field theoryFísicaFOS: Physical sciencesPropagatorIntegral equationScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum mechanicsSymmetry breakingQuantum field theoryChiral symmetry breakingMathematical physicsPhysical Review D
researchProduct

Bicoherent-State Path Integral Quantization of a non-Hermitian Hamiltonian

2020

We introduce, for the first time, bicoherent-state path integration as a method for quantizing non-hermitian systems. Bicoherent-state path integrals arise as a natural generalization of ordinary coherent-state path integrals, familiar from hermitian quantum physics. We do all this by working out a concrete example, namely, computation of the propagator of a certain quasi-hermitian variant of Swanson's model, which is not invariant under conventional $PT$-transformation. The resulting propagator coincides with that of the propagator of the standard harmonic oscillator, which is isospectral with the model under consideration by virtue of a similarity transformation relating the corresponding…

High Energy Physics - TheorySwanson modelFOS: Physical sciencesGeneral Physics and AstronomyPT symmetrysymbols.namesakeFeynman diagramHarmonic oscillatorMathematical PhysicsNon-hermitian hamiltoniansMathematical physicsPhysicsQuantum PhysicsQuantization (signal processing)PropagatorMathematical Physics (math-ph)Bicoherent statesHermitian matrixIsospectralHigh Energy Physics - Theory (hep-th)Path integral quantizationPath integral formulationsymbolsPseudo-bosonsQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)
researchProduct

Multi-boson block factorization of fermions

2017

The numerical computations of many quantities of theoretical and phenomenological interest are plagued by statistical errors which increase exponentially with the distance of the sources in the relevant correlators. Notable examples are baryon masses and matrix elements, the hadronic vacuum polarization and the light-by-light scattering contributions to the muon g-2, and the form factors of semileptonic B decays. Reliable and precise determinations of these quantities are very difficult if not impractical with state-of-the-art standard Monte Carlo integration schemes. I will review a recent proposal for factorizing the fermion determinant in lattice QCD that leads to a local action in the g…

High Energy Physics::Latticeaction: local01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Vacuum polarizationcorrelation functionQuantum Chromodynamics Lattice gauge theory Computational PhysicsMonte CarloBosonPhysicsform factorPhysicsHigh Energy Physics - Lattice (hep-lat)lattice field theoryPropagatorpropagator [quark]hep-phParticle Physics - Latticestatistical [error]Lattice QCDFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - Phenomenologyerror: statisticalquark: factorizationquark: propagatorMonte Carlo integrationQuarkParticle physicsQC1-999fermion: determinantdeterminant [fermion]FOS: Physical scienceshep-latbaryon: massHigh Energy Physics - LatticeFactorization0103 physical sciencesmagnetic moment [muon]hadronic [vacuum polarization]010306 general physicsnumerical calculationsParticle Physics - Phenomenologymuon: magnetic moment010308 nuclear & particles physicsvacuum polarization: hadronicHigh Energy Physics::Phenomenologyphoton photon: scatteringB: decaylocal [action]Fermiondecay [B]mass [baryon]scattering [photon photon]gauge field theoryHigh Energy Physics::Experimentfactorization [quark]
researchProduct

Vanishing of certain cuts or residues of loop integrals with higher powers of the propagators

2019

Starting from two-loops, there are Feynman integrals with higher powers of the propagators. They arise from self-energy insertions on internal lines. Within the loop-tree duality approach or within methods based on numerical unitarity one needs (among other things) the residue when a raised propagator goes on-shell. We show that for renormalised quantities in the on-shell scheme these residues can be made to vanish already at the integrand level.

Loop (topology)PhysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)UnitarityFeynman integralScheme (mathematics)Shell (structure)FOS: Physical sciencesPropagatorDuality (optimization)Mathematical physicsPhysical Review D
researchProduct

Effect ofmconbquark chromomagnetic interaction and on-shell two-loop integrals with two masses

1999

The effect of non-zero c quark mass on b quark HQET Lagrangian, up to 1/mb level, is calculated at two loops. The results are expressed in terms of dilogarithmic functions of mc/mb. This calculation involves on-shell two-loop propagator-type diagrams with two different masses, mb and mc. A general algorithm for reducing such Feynman integrals to the basis of two nontrivial and two trivial integrals is constructed.

Loop (topology)PhysicsNuclear and High Energy PhysicsParticle physicsBasis (linear algebra)BibliographyShell (structure)PropagatorCharm (quantum number)Bottom quarkCharm quarkPhysical Review D
researchProduct

oneloop 2.0 — A program package calculating one-loop integrals

1997

We present an improved version of our program package oneloop which -- written as a package for MAPLE -- solves one-loop Feynman integrals. The package is calculating one-, two- and three-point functions both algebraically and numerically to any tensor rank. In addition to the original version oneloop 2.0 also calculates infrared divergent integrals. Higher powers of propagator terms and the $O(\eps)$ parts relevant for two-loop calculations are now supported.

MaplePhysicsParticle physicsFeynman integralTensor rankFOS: Physical sciencesGeneral Physics and AstronomyPropagatorengineering.materialLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and ArchitectureComputer Science::Mathematical SoftwareengineeringMathematical physicsComputer Physics Communications
researchProduct

Unitarized Chiral Perturbation Theory in a finite volume: scalar meson sector

2011

We develop a scheme for the extraction of the properties of the scalar mesons f0(600), f0(980), and a0(980) from lattice QCD data. This scheme is based on a two-channel chiral unitary approach with fully relativistic propagators in a finite volume. In order to discuss the feasibility of finding the mass and width of the scalar resonances, we analyze synthetic lattice data with a fixed error assigned, and show that the framework can be indeed used for an accurate determination of resonance pole positions in the multi-channel scattering.

Nuclear and High Energy PhysicsChiral perturbation theoryeffect [threshold]MesonNuclear TheoryHigh Energy Physics::LatticeFOS: Physical scienceschiral [perturbation theory]f0(980)a0(980)Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)relativistic [propagator]unitarityddc:530energy levelsScalar mesonnumerical calculationsMathematical physicsPhysicsFinite volume methodScatteringscalar [resonance]High Energy Physics - Lattice (hep-lat)PropagatorFísicascalar mesonLattice QCDf0(600)boundary conditionpole [resonance]High Energy Physics - Phenomenologyfinite size
researchProduct