Search results for "Mathematical physics"

showing 10 items of 2687 documents

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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Renormalization of relativistic baryon chiral perturbation theory and power counting

2003

We discuss a renormalization scheme for relativistic baryon chiral perturbation theory which provides a simple and consistent power counting for renormalized diagrams. The method involves finite subtractions of dimensionally regularized diagrams beyond the standard $\bar{\rm MS}$ scheme of chiral perturbation theory to remove contributions violating the power counting. This is achieved by a suitable renormalization of the parameters of the most general effective Lagrangian. In addition to simplicity our method has the benefit that it can be easily applied to multiloop diagrams. As an application we discuss the mass and the scalar form factor of the nucleon and compare the results with the e…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear Theory010308 nuclear & particles physicsHigh Energy Physics::LatticeFOS: Physical sciences01 natural sciencesBaryonRenormalizationNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Regularization (physics)0103 physical sciencesEffective lagrangianFunctional renormalization group010306 general physicsNucleonNuclear theoryMathematical physics
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Hadron structure in the description of electromagnetic reactions

2002

The description of electromagnetic reactions at intermediate energies, such as pion electroproduction or (virtual) Compton scattering, traditionally starts from covariant tree-level Feynman diagrams (Born or pole terms). Internal hadron structure is included by means of (on-shell) form factors in the vertices while free propagators are used. To overcome problems with gauge invariance, simple prescriptions, such as, choosing ${F}_{1}^{V}{(q}^{2}{)=F}_{\ensuremath{\pi}}{(q}^{2})$ in pion electroproduction or the ``minimal substitution,'' are used. We discuss the inherent assumptions of such approaches and study the general structure of electromagnetic vertices and propagators for pions and nu…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryHadronCompton scatteringPropagatorVertex (geometry)symbols.namesakePionsymbolsFeynman diagramGauge theoryNuclear ExperimentMathematical physicsPhysical Review C
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Bethe-Salpeter approach for unitarized chiral perturbation theory

2000

The Bethe-Salpeter equation restores exact elastic unitarity in the $s-$ channel by summing up an infinite set of chiral loops. We use this equation to show how a chiral expansion can be undertaken in the two particle irreducible amplitude and the propagators accomplishing exact elastic unitarity at any step. Renormalizability of the amplitudes can be achieved by allowing for an infinite set of counter-terms as it is the case in ordinary Chiral Perturbation Theory. Crossing constraints can be imposed on the parameters to a given order. Within this framework, we calculate the leading and next-to-leading contributions to the elastic $\pi \pi$ scattering amplitudes, for all isospin channels, a…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryNuclear TheoryUnitarityHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesPropagatorOrder (ring theory)FísicaNuclear Theory (nucl-th)RenormalizationScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinMathematical physics
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Universal Bounds for SU(3) Low Energy Constants

2008

In this paper bounds for L_1, L_2 and L_3 are obtained in Chiral Perturbation Theory with three flavours. At the same time we test the compatibility of this theory with axiomatic principles. Following a recent paper we use dispersion relations to write positivity conditions that translate into bounds for the chiral low energy constants. As a first approach we consider the exact SU(3)_V limit and notice that if a common mass of the order of that of the kaon is adopted for the octet of pseudo-Goldstone bosons the bounds have very large O(p^6) corrections. Once the positivity conditions are adapted to account for different masses, we correct the previous bounds for a physical kaon mass and fin…

PhysicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryOctetFOS: Physical sciencesHigh Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)Dispersion relationGoldstone bosonAxiomMathematical physicsBoson
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On the singular behaviour of scattering amplitudes in quantum field theory

2014

We analyse the singular behaviour of one-loop integrals and scattering amplitudes in the framework of the loop--tree duality approach. We show that there is a partial cancellation of singularities at the loop integrand level among the different components of the corresponding dual representation that can be interpreted in terms of causality. The remaining threshold and infrared singularities are restricted to a finite region of the loop momentum space, which is of the size of the external momenta and can be mapped to the phase-space of real corrections to cancel the soft and collinear divergences.

PhysicsNuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesDuality (optimization)FísicaPosition and momentum spaceDual representationScattering amplitudeCausality (physics)Loop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Gravitational singularityQuantum field theoryMathematical physics
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S-waveKK*interactions in a finite volume and thef1(1285)

2015

Lattice QCD simulations provide a promising way to disentangle different interpretations of hadronic resonances, which might be of particular relevance to understand the nature of the so-called XY Z particles. Recent studies have shown that in addition to the well-established naive quark model picture, the axial-vector meson f1(1285) can also be understood as a dynamically generated state built upon the KK ∗ interaction. In this work, we calculate the energy levels of the KK ∗ system in the f1(1285) channel in finite volume using the chiral unitary approach. We propose to calculate the loop function in the dimensional regularization scheme, which is equivalent to the hybrid approach adopted…

PhysicsNuclear and High Energy PhysicsParticle physicsFinite volume methodMesonUnitarity010308 nuclear & particles physicsHigh Energy Physics::LatticeQuark modelLattice field theoryLattice QCD01 natural sciencesDimensional regularization0103 physical sciencesBound state010306 general physicsMathematical physicsPhysical Review D
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Gluon mass through ghost synergy

2011

In this work we compute, at the "one-loop-dressed" level, the nonperturbative contribution of the ghost loops to the self-energy of the gluon propagator, in the Landau gauge. This is accomplished within the PT-BFM formalism, which guarantees the gauge-invariance of the emerging answer. In particular, the contribution of the ghost-loops is automatically transverse, by virtue of the QED-like Ward identities satisfied in this framework. Using as nonperturbative input the available lattice data for the ghost dressing function, we show that the ghost contributions have a rather sizable effect on the overall shape of the gluon propagator, both for $d=3,4$. Then, by exploiting a recently introduce…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPropagatorGluonFormalism (philosophy of mathematics)High Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)Mathematical physics
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Indirect determination of the Kugo-Ojima function from lattice data

2009

We study the structure and non-perturbative properties of a special Green's function, u(q), whose infrared behavior has traditionally served as the standard criterion for the realization of the Kugo-Ojima confinement mechanism. It turns out that, in the Landau gauge, u(q) can be determined from a dynamical equation, whose main ingredients are the gluon propagator and the ghost dressing function, integrated over all physical momenta. Using as input for these two (infrared finite) quantities recent lattice data, we obtain an indirect determination of u(q). The results of this mixed procedure are in excellent agreement with those found previously on the lattice, through a direct simulation of …

PhysicsNuclear and High Energy PhysicsParticle physicsInfraredHigh Energy Physics::LatticeFísicaNonperturbative effectsFOS: Physical sciencesPropagatorQCDGluonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)ConfinementMathematical physics
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