Search results for "propagator"

showing 10 items of 173 documents

The scalar pion form factor in two-flavor lattice QCD

2013

We calculate the scalar form factor of the pion using two dynamical flavors of non-perturbatively $\mathcal{O}(a)$-improved Wilson fermions, including both the connected and the disconnected contribution to the relevant correlation functions. We employ the calculation of all-to-all propagators using stochastic sources and a generalized hopping parameter expansion. From the form factor data at vanishing momentum transfer, $Q^2=0$, and two non-vanishing $Q^2$ we obtain an estimate for the scalar radius $\left^\pi_{_{\rm S}}$ of the pion at one value of the lattice spacing and for five different pion masses. Using Chiral Perturbation Theory at next-to-leading order, we find $\left^\pi_{_{\rm S…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Momentum transferScalar (mathematics)Form factor (quantum field theory)FOS: Physical sciencesOrder (ring theory)PropagatorLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - Lattice
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Non-Perturbative Propagators in QCD

1994

Over the last two decades it has become clear that perturbation theory can only give us very limited information about QCD. For example it is not sufficient to describe that most basic of things, the mass spectrum. Although, we may hope one day to gain from the lattice approach numerical confirmation that we have the correct Lagrangian to describe hadronic physics, that day is not at hand. In the meantime it will be argued here, the operator product expansion (OPE) offers us some useful non-perturbative information about the structure of QCD.

PhysicsQuantum chromodynamicssymbols.namesakeTheoretical physicsLattice (order)High Energy Physics::PhenomenologyHadronsymbolsPropagatorLattice QCDOperator product expansionNon-perturbativeLagrangian
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CP properties of the leptonic sector for majorana neutrinos

1983

Abstract The leptonic sector of the electroweak theory is analyzed for massive Majorana neutrinos. For n generations, the Majorana mass lagrangian is diagonalized using the polar reduction to guarantee physical positive masses independently of the CP properties or the choice of the phases of the fields. When CP invariance holds, the CP eigenvalues of the definite mass neutrino fields are determined without commitment to a particular phase choice. For charged current interactions, we find that the observable CP violating phases can be parametrized a la Kobayashi-Maskawa for the vertec. Extra ( n − 1) relative phases of the massive neutrino fields are significant. The extra phases are observa…

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyPropagatorFísicaObservableMAJORANACP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationGeneral Theoretical PhysicsCharged current
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Linear response of homogeneous nuclear matter with energy density functionals

2014

Response functions of infinite nuclear matter with arbitrary isospin asymmetry are studied in the framework of the random phase approximation. The residual interaction is derived from a general nuclear Skyrme energy density functional. Besides the usual central, spin-orbit and tensor terms it could also include other components as new density-dependent terms or three-body terms. Algebraic expressions for the response functions are obtained from the Bethe-Salpeter equation for the particle-hole propagator. Applications to symmetric nuclear matter, pure neutron matter and asymmetric nuclear matter are presented and discussed. Spin-isospin strength functions are analyzed for varying conditions…

Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear Theory010308 nuclear & particles physicsmedia_common.quotation_subjectNuclear TheoryMomentum transferFOS: Physical sciencesFísicaGeneral Physics and AstronomyPropagatorNuclear matter01 natural sciencesAsymmetryNuclear Theory (nucl-th)Isospin0103 physical sciencesNeutronTensorNuclear Experiment010306 general physicsRandom phase approximationmedia_commonMathematical physicsPhysics Reports
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Field propagator of a dressed junction: Fluorescence lifetime calculations in a confined geometry

1997

The study of the fluorescence phenomenon by near-field optical techniques requires one to describe precisely the spontaneous emission change occurring when the fluorescing particle is placed in a complex optical environment. For this purpose, the field susceptibility (also called the field propagator) of a planar junction formed by a cavity bounded by two semi-infinite bodies with arbitrary optical constant is derived within the framework of linear-response theory. The field propagator associated with the junction is then modified in a self-consistent manner to account for the presence of any arbitrary object inside the junction. As a first illustration the alteration of the fluorescence li…

PhysicsField (physics)Physics::OpticsPropagatorDielectricMolecular physicsAtomic and Molecular Physics and OpticsPlanarQuantum mechanicsParticleSpontaneous emissionSPHERESsense organsConstant (mathematics)Physical Review A
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Nonperturbative study of the four gluon vertex

2014

In this paper we study the nonperturbative structure of the SU(3) four-gluon vertex in the Landau gauge, concentrating on contributions quadratic in the metric. We employ an approximation scheme where "one-loop" diagrams are computed using fully dressed gluon and ghost propagators, and tree-level vertices. When a suitable kinematical configuration depending on a single momentum scale $p$ is chosen, only two structures emerge: the tree-level four-gluon vertex, and a tensor orthogonal to it. A detailed numerical analysis reveals that the form factor associated with this latter tensor displays a change of sign (zero-crossing) in the deep infrared, and finally diverges logarithmically. The orig…

High Energy Physics - TheoryPhysicsQuantum chromodynamicsNuclear and High Energy PhysicsHigh Energy Physics - Lattice (hep-lat)Form factor (quantum field theory)FOS: Physical sciencesFísicaPropagatorSymmetry (physics)Vertex (geometry)MomentumHigh Energy Physics - PhenomenologyLattice (module)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)TensorMathematical physicsJournal of High Energy Physics
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Gluon mass generation in the PT-BFM scheme

2006

In this article we study the general structure and special properties of the Schwinger-Dyson equation for the gluon propagator constructed with the pinch technique, together with the question of how to obtain infrared finite solutions, associated with the generation of an effective gluon mass. Exploiting the known all-order correspondence between the pinch technique and the background field method, we demonstrate that, contrary to the standard formulation, the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions. We next present a comprehensive review of several subtle issues relevant to the search …

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodLorentz transformationHigh Energy Physics::LatticeMass generationHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesFísicaRenormalization groupIntegral equationMassless particleHigh Energy Physics - Phenomenologysymbols.namesakeTheoretical physicsDimensional regularizationHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)symbols
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Non-autonomous rough semilinear PDEs and the multiplicative Sewing Lemma

2021

We investigate existence, uniqueness and regularity for local solutions of rough parabolic equations with subcritical noise of the form $du_t- L_tu_tdt= N(u_t)dt + \sum_{i = 1}^dF_i(u_t)d\mathbf X^i_t$ where $(L_t)_{t\in[0,T]}$ is a time-dependent family of unbounded operators acting on some scale of Banach spaces, while $\mathbf X\equiv(X,\mathbb X)$ is a two-step (non-necessarily geometric) rough path of H\"older regularity $\gamma >1/3.$ Besides dealing with non-autonomous evolution equations, our results also allow for unbounded operations in the noise term (up to some critical loss of regularity depending on that of the rough path $\mathbf X$). As a technical tool, we introduce a versi…

60H15 60H05 35K58 32A70Pure mathematicsLemma (mathematics)Rough pathSemigroupMultiplicative functionProbability (math.PR)Banach spacePropagatorParabolic partial differential equationFunctional Analysis (math.FA)Mathematics - Functional AnalysisMathematics - Analysis of PDEsRough partial differential equationsProduct (mathematics)Multiplicative Sewing lemmaFOS: Mathematics/dk/atira/pure/subjectarea/asjc/2600/2603UniquenessRough pathMathematics - ProbabilityAnalysisMathematicsAnalysis of PDEs (math.AP)
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On the evaluation of sunset-type Feynman diagrams

1999

We introduce an efficient configuration space technique which allows one to compute a class of Feynman diagrams which generalize the scalar sunset topology to any number of massive internal lines. General tensor vertex structures and modifications of the propagators due to particle emission with vanishing momenta can be included with only a little change of the basic technique described for the scalar case. We discuss applications to the computation of $n$-body phase space in $D$-dimensional space-time. Substantial simplifications occur for odd space-time dimensions where the final results can be expressed in closed form through rational functions. We present explicit analytical formulas fo…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryComputationScalar (mathematics)FOS: Physical sciencesPropagatorRational functionSunsetNuclear Theory (nucl-th)High Energy Physics - Phenomenologysymbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Phase spacesymbolsFeynman diagramConfiguration spaceNuclear Physics B
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A tree-loop duality relation at two loops and beyond

2010

The duality relation between one-loop integrals and phase-space integrals, developed in a previous work, is extended to higher-order loops. The duality relation is realized by a modification of the customary +i0 prescription of the Feynman propagators, which compensates for the absence of the multiple-cut contributions that appear in the Feynman tree theorem. We rederive the duality theorem at one-loop order in a form that is more suitable for its iterative extension to higher-loop orders. We explicitly show its application to two-and three-loop scalar master integrals, and we discuss the structure of the occurring cuts and the ensuing results in detail.

High Energy Physics - TheoryQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsScalar (mathematics)Duality (mathematics)FOS: Physical sciencesPropagatorFísicaLoop integralDuality relationHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Phase spacesymbolsFeynman diagramMathematical physics
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