Search results for "REGULARIZATION"

showing 10 items of 189 documents

Adiabatic regularization and particle creation for spin one-half fields

2013

The extension of the adiabatic regularization method to spin-$1/2$ fields requires a self-consistent adiabatic expansion of the field modes. We provide here the details of such expansion, which differs from the WKB ansatz that works well for scalars, to firmly establish the generalization of the adiabatic renormalization scheme to spin-$1/2$ fields. We focus on the computation of particle production in de Sitter spacetime and obtain an analytic expression of the renormalized stress-energy tensor for Dirac fermions.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Quantum field theory in curved spacetimeFOS: Physical sciencesFísicaGeneral Relativity and Quantum Cosmology (gr-qc)Mathematical Physics (math-ph)Adiabatic quantum computationGeneral Relativity and Quantum CosmologyWKB approximationRenormalizationsymbols.namesakeGeneral Relativity and Quantum CosmologyClassical mechanicsHigh Energy Physics - Theory (hep-th)Dirac fermionRegularization (physics)symbolsAdiabatic processMathematical PhysicsAstrophysics - Cosmology and Nongalactic AstrophysicsMathematical physicsAnsatz
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Towards N=1 Super-Yang-Mills on the Lattice

1997

We consider the lattice regularization of N=1 supersymmetric Yang--Mills theory with Wilson fermions. This formulation breaks supersymmetry at any finite lattice spacing; we discuss how Ward identities can be used to define a supersymmetric continuum limit, which coincides with the point where the gluino becomes massless. As a first step towards the understanding of the zero gluino-mass limit, we present results on the quenched low-lying spectrum of SU(2) N=1 Super-Yang--Mills, at $\beta=2.6$ on a $V=16^3 \times 32$ lattice, in the OZI approximation. Our results, in spite of the quenched and OZI approximations, are in remarkable agreement with theoretical predictions in the supersymmetric t…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsGluinoHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesYang–Mills existence and mass gapParticle Physics - LatticeFermionSupersymmetryMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - LatticeLattice constantHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Regularization (physics)Lattice (order)Mathematical physics
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Gluon mass generation without seagull divergences

2009

Dynamical gluon mass generation has been traditionally plagued with seagull divergences, and all regularization procedures proposed over the years yield finite but scheme-dependent gluon masses. In this work we show how such divergences can be eliminated completely by virtue of a characteristic identity, valid in dimensional regularization. The ability to trigger the aforementioned identity hinges crucially on the particular Ansatz employed for the three-gluon vertex entering into the Schwinger-Dyson equation governing the gluon propagator. The use of the appropriate three-gluon vertex brings about an additional advantage: one obtains two separate (but coupled) integral equations, one for t…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Mass generationHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesPropagatorFísicaIntegral equationEffective nuclear chargeGluonHigh Energy Physics - PhenomenologyDimensional regularizationTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum electrodynamicsRegularization (physics)Nuclear ExperimentAnsatz
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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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Threshold expansion of the sunset diagram

1999

By use of the threshold expansion we develop an algorithm for analytical evaluation, within dimensional regularization, of arbitrary terms in the expansion of the (two-loop) sunset diagram with general masses m_1, m_2 and m_3 near its threshold, i.e. in any given order in the difference between the external momentum squared and its threshold value, (m_1+m_2+m_3)^2. In particular, this algorithm includes an explicit recurrence procedure to analytically calculate sunset diagrams with arbitrary integer powers of propagators at the threshold.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physicsDiagramMathematical analysisFOS: Physical sciencesPropagatorSunsetMomentumHigh Energy Physics - PhenomenologyDimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)IntegerOrder (group theory)Nuclear Physics B
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Polarized triple-collinear splitting functions at NLO for processes with photons

2014

We compute the polarized splitting functions in the triple collinear limit at next-to-leading order accuracy (NLO) in the strong coupling $\alpha_{\rm S}$, for the splitting processes $\gamma \to q \bar{q} \gamma$, $\gamma \to q \bar{q} g$ and $g \to q \bar{q} \gamma$. The divergent structure of each splitting function was compared to the predicted behaviour according to Catani's formula. The results obtained in this paper are compatible with the unpolarized splitting functions computed in a previous article. Explicit results for NLO corrections are presented in the context of conventional dimensional regularization (CDR).

High Energy Physics - TheoryPhysicsParticle physicsNuclear and High Energy PhysicsPhotonBar (music)High Energy Physics::PhenomenologyStructure (category theory)FísicaOrder (ring theory)FOS: Physical sciencesContext (language use)Function (mathematics)High Energy Physics - PhenomenologyDimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentLimit (mathematics)Mathematical physics
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Conformal Symmetry and Differential Regularization of the Three-Gluon Vertex

1992

The conformal symmetry of the QCD Lagrangian for massless quarks is broken both by renormalization effects and the gauge fixing procedure. Renormalized primitive divergent amplitudes have the property that their form away from the overall coincident point singularity is fully determined by the bare Lagrangian, and scale dependence is restricted to $\delta$-functions at the singularity. If gauge fixing could be ignored, one would expect these amplitudes to be conformal invariant for non-coincident points. We find that the one-loop three-gluon vertex function $\Gamma_{\mu\nu\rho}(x,y,z)$ is conformal invariant in this sense, if calculated in the background field formalism using the Feynman ga…

High Energy Physics - TheoryPhysicsQuantum chromodynamicsUltraviolet divergenceHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyVertex functionFOS: Physical sciencesFísicaRenormalizationsymbols.namesakeHigh Energy Physics - Theory (hep-th)Conformal symmetryRegularization (physics)symbolsFeynman diagramGauge fixingMathematical physics
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Dimensional interpolation and the Selberg integral

2019

Abstract We show that a version of dimensional interpolation for the Riemann–Roch–Hirzebruch formalism in the case of a grassmannian leads to an expression for the Euler characteristic of line bundles in terms of a Selberg integral. We propose a way to interpolate higher Bessel equations, their wedge powers, and monodromies thereof to non–integer orders, and link the result with the dimensional interpolation of the RRH formalism in the spirit of the gamma conjectures.

High Energy Physics - TheoryPure mathematicsGeneral Physics and AstronomyFOS: Physical sciencesAlgebraic geometry01 natural sciencesWedge (geometry)Dimensional regularizationsymbols.namesakeMathematics - Algebraic GeometryMathematics::Algebraic GeometryGrassmannianEuler characteristic0103 physical sciencesFOS: Mathematics0101 mathematicsAlgebraic Geometry (math.AG)Mathematical PhysicsMathematics010102 general mathematicsHigh Energy Physics - Theory (hep-th)symbols010307 mathematical physicsGeometry and TopologyMirror symmetryBessel functionInterpolation
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A quasi-finite basis for multi-loop Feynman integrals

2014

We present a new method for the decomposition of multi-loop Euclidean Feynman integrals into quasi-finite Feynman integrals. These are defined in shifted dimensions with higher powers of the propagators, make explicit both infrared and ultraviolet divergences, and allow for an immediate and trivial expansion in the parameter of dimensional regularization. Our approach avoids the introduction of spurious structures and thereby leaves integrals particularly accessible to direct analytical integration techniques. Alternatively, the resulting convergent Feynman parameter integrals may be evaluated numerically. Our approach is guided by previous work by the second author but overcomes practical …

High Energy Physics - TheoryQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsBasis (linear algebra)FOS: Physical sciencesPropagatorHigh Energy Physics - Phenomenologysymbols.namesakeDimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Euclidean geometrysymbolsApplied mathematicsFeynman diagramIntegration by partsReduction (mathematics)Journal of High Energy Physics
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Adiabatic expansions for Dirac fields, renormalization, and anomalies

2018

11 pags.

High Energy Physics - TheoryRenormalizationConformal anomalyFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyRenormalizationGeneral Relativity and Quantum CosmologyDirac fieldFriedmann-Lemaître-Robertson-Walker spacetime0103 physical sciencesMinkowski spaceRenormalization; anomalies010306 general physicsAdiabatic processYukawa couplingMathematical physicsPhysicsMaterialesSpacetime010308 nuclear & particles physicsYukawa potentialAdiabatic expansionCosmologyHigh Energy Physics - Theory (hep-th)Regularization (physics)anomaliesScalar fieldPhysical Review D
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