Search results for "PERTURBATION"

showing 10 items of 811 documents

Pinch technique self-energies and vertices to all orders in perturbation theory

2003

The all-order construction of the pinch technique gluon self-energy and quark-gluon vertex is presented in detail within the class of linear covariant gauges. The main ingredients in our analysis are the identification of a special Green's function, which serves as a common kernel to all self-energy and vertex diagrams, and the judicious use of the Slavnov-Taylor identity it satisfies. In particular, it is shown that the ghost-Green's functions appearing in this identity capture precisely the result of the pinching action at arbitrary order. By virtue of this observation the construction of the quark-gluon vertex becomes particularly compact. It turns out that the aforementioned ghost-Green…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaFunction (mathematics)Vertex (geometry)RenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Kernel (statistics)Covariant transformationUniquenessPerturbation theory (quantum mechanics)
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Orderp6chiral couplings from the scalarK  form factor

2004

15 páginas, 2 tablas.-- arXiv:hep-ph/0401080v2

PhysicsNuclear and High Energy PhysicsParticle physicsChannel dispersionChiral perturbation theoryMomentum transferScalar (mathematics)FOS: Physical sciencesFísicaCurvatureQCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PiChiral lagrangiansKaon physicsJournal of High Energy Physics
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Lepton-number violation and right-handed neutrinos in Higgs-less effective theories

2005

Following previous work, we identify a symmetry S_nat that generalizes the concept of custodial symmetry, keeping under control deviations from the Standard Model (SM). To realize S_nat linearly, the space of gauge fields has to be extended. Covariant constraints formulated in terms of spurions reduce S_nat back to SU(2)_L x U(1)_Y. This allows for a covariant introduction of explicit S_nat-breaking parameters. We assume that S_nat is at play in a theory of electroweak symmetry-breaking without a light Higgs particle. We describe some consequences of this assumption, using a non-decoupling effective theory in which the loop expansion procedure is based on both momentum and spurion power cou…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesLepton numberCustodial symmetryStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesEffective field theoryHiggs bosonSymmetry breaking010306 general physics
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Nucleon mass and pion-nucleon sigma term from a chiral analysis of lattice QCD data

2013

The pion mass dependence of the nucleon mass within the covariant SU(2) baryon chiral perturbation theory both without and with explicit Delta(1232) degrees of freedom up to order p(4) is investigated. By fitting to a comprehensive set of lattice QCD data in 2 and 2 + 1 flavors from several collaborations, for pion masses M-pi < 420 MeV, we obtain low energy constants of natural size that are compatible with pion-nucleon scattering data. Our results are consistent with the rather linear pion mass dependence showed by lattice QCD. In the 2 flavor case we have also performed simultaneous fits to nucleon mass and sigma(pi N) data. As a result of our analysis, which encompasses the study of fin…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryOrder (ring theory)Light hadron massesLattice QCD01 natural sciencesResonance (particle physics)Perturbation-theoryBaryonPion0103 physical sciencesHigh Energy Physics::ExperimentFísica nuclearPerturbation theory010306 general physicsNucleonNuclear Experiment
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An exploratory lattice study of decays at next-to-leading order in the chiral expansion

2005

Abstract We present the first direct evaluation of Δ I = 3 / 2 K → π π matrix elements with the aim of determining all the low-energy constants at NLO in the chiral expansion. Our numerical investigation demonstrates that it is indeed possible to determine the K → π π matrix elements directly for the masses and momenta used in the simulation with good precision. In this range however, we find that the matrix elements do not satisfy the predictions of NLO chiral perturbation theory. For the chiral extrapolation we therefore use a hybrid procedure which combines the observed polynomial behavior in masses and momenta of our lattice results, with NLO chiral perturbation theory at lower masses. …

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionExtrapolation01 natural sciencesLattice (order)0103 physical sciencesPiHigh Energy Physics::ExperimentDirect evaluation010306 general physicsNuclear Physics B
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Rare kaon decays

1997

Abstract More and more sophisticated experiments and continuous progress in the theoretical understanding of rare kaon decays have proven how rich this field of particle physics is. This article summarizes the present situation of the phenomenology and the experiments. Prospects for the future are given and discussed. The decays are ordered from the less rare to the very rare. Recently there has been quite some progress concerning the first category of decays presented here, the radiative decays, and tests of chiral perturbation theory. The CP violating decays discussed next are complementary to the KL → 2π decays and offer additional insight into the mechanism of direct CP violation. Decay…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theory010308 nuclear & particles physicsPhysics beyond the Standard Model01 natural sciencesNuclear physics0103 physical sciencesRadiative transferCP violationHigh Energy Physics::Experiment010306 general physicsPhenomenology (particle physics)Progress in Particle and Nuclear Physics
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Error estimates for pi-pi scattering threshold parameters in Chiral Perturbation Theory to two loops

2000

Using the analysis of ChPT to two loops, we perform an error analysis of the threshold and low energy parameters, based on the uncertainties for the one loop low energy parameters and the resonance saturation mechanism. Different sets of one loop low energy constants have been considered.Thus, the predictive power of the effective field theory is quantified on the basis of the present experimental uncertainties.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryBasis (linear algebra)ScatteringFísicaFOS: Physical sciencesResonance (particle physics)Loop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PiEffective field theoryStatistical physicsSaturation (chemistry)
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Chiral approach to the two pion decay of the Roper

2003

Abstract The analysis of Manley and collaborators [1] of the decay of the Roper into two pions requires the introduction of an effective scalar-isosclar ϵ or σ meson in order to describe the s-wave ππ interaction. Here we try to understand at a more fundamental level the origin of this effective channel. In our model the two pions are produced in single pion-baryon-baryon vertices and their re-scattering in the L=0, I=0 channel is explicitly evaluated. For that purpose we use unitarized chiral perturbation theory to obtain the Bethe-Salpeter amplitude for the two pion re-scattering in the appropriate channel. Our model produces invariant mass distributions in agreement with the ones obtaine…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryBethe–Salpeter equationMesonHigh Energy Physics::PhenomenologyNuclear TheoryHadronElementary particleParticle decayPionInvariant massNuclear ExperimentNuclear Physics A
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Chiral Perturbation Theory with tensor sources

2007

23 pages, 1 figure.-- ISI Article Identifier: 000249788800051.-- ArXiv pre-print available at: http://arxiv.org/abs/0705.2948

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryCurrent (mathematics)MesonBar (music)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)SigmaFOS: Physical sciencesQCDSpontaneous Symmetry BreakingHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Nonperturbative EffectssymbolsTensorChiral lagrangiansLagrangianMathematical physics
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The sunset diagram in SU(3) chiral perturbation theory

1996

A general procedure for the calculation of a class of two-loop Feynman diagrams is described. These are two-point functions containing three massive propagators, raised to integer powers, in the denominator, and arbitrary polynomials of the loop momenta in the numerator. The ultraviolet divergent parts are calculated analytically, while the remaining finite parts are obtained by a one-dimensional numerical integration, both below and above the threshold. Integrals of this type occur, for example, in chiral perturbation theory at order p^6.

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryDiagramFOS: Physical sciencesGeneral Physics and AstronomyPropagatorAstronomy and AstrophysicsNumerical integrationLoop (topology)symbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IntegersymbolsOrder (group theory)Feynman diagramMathematical physics
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