Search results for "Dimensional regularization"

showing 10 items of 36 documents

The one loop gluon emission light cone wave function

2017

Light cone perturbation theory has become an essential tool to calculate cross sections for various small-$x$ dilute-dense processes such as deep inelastic scattering and forward proton-proton and proton-nucleus collisions. Here we set out to do one loop calculations in an explicit helicity basis in the four dimensional helicity scheme. As a first process we calculate light cone wave function for one gluon emission to one-loop order in Hamiltonian perturbation theory on the light front. We regulate ultraviolet divergences with transverse dimensional regularization and soft divergences with using a cut-off on longitudinal momentum. We show that when all the renormalization constants are comb…

COLLISIONSParticle physicsNuclear TheoryRENORMALIZATIONQUANTUM ELECTRODYNAMICSGeneral Physics and AstronomyFOS: Physical sciencesloop calculations114 Physical sciences01 natural scienceslight cone perturbation theoryRenormalizationNuclear Theory (nucl-th)Dimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)INFINITE-MOMENTUMLight cone0103 physical sciencesSCATTERINGHelicity basis010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsCoupling constantgluon emissionta114010308 nuclear & particles physicsCOLOR GLASS CONDENSATEDeep inelastic scatteringFRONT QCDHelicityEVOLUTIONHigh Energy Physics - PhenomenologyCHROMODYNAMICSQuantum electrodynamicsgluon saturation
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Double collinear splitting amplitudes at next-to-leading order

2013

We compute the next-to-leading order (NLO) QCD corrections to the $1 \to 2$ splitting amplitudes in different dimensional regularization (DREG) schemes. Besides recovering previously known results, we explore new DREG schemes and analyze their consistency by comparing the divergent structure with the expected behavior predicted by Catani's formula. Through the introduction of scalar-gluons, we show the relation among splittings matrices computed using different schemes. Also, we extended this analysis to cover the double collinear limit of scattering amplitudes in the context of QCD+QED.

High Energy Physics - TheoryNLO COMPUTATIONSNuclear and High Energy PhysicsParticle physicsHADRONIC COLLIDERSCiencias FísicasFOS: Physical sciencesContext (language use)01 natural sciences//purl.org/becyt/ford/1 [https]Dimensional regularizationHigh Energy Physics - Phenomenology (hep-ph)Consistency (statistics)0103 physical sciencesLimit (mathematics)010306 general physicsMathematical physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísica//purl.org/becyt/ford/1.3 [https]Scattering amplitudeAstronomíaHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Theory (hep-th)Cover (topology)CIENCIAS NATURALES Y EXACTASJournal of High Energy Physics
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Transcendental numbers and the topology of three-loop bubbles

1999

We present a proof that all transcendental numbers that are needed for the calculation of the master integrals for three-loop vacuum Feynman diagrams can be obtained by calculating diagrams with an even simpler topology, the topology of spectacles.

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsComputationBare massFOS: Physical sciencesMathematical Physics (math-ph)TopologyHigh Energy Physics - PhenomenologyDimensional regularizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Number theoryHigh Energy Physics - Theory (hep-th)Special functionsRegularization (physics)symbolsFeynman diagramAlgebraic numberMathematical PhysicsPhysical Review D
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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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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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Running couplings from adiabatic regularization

2019

We extend the adiabatic regularization method by introducing an arbitrary mass scale $\mu$ in the construction of the subtraction terms. This allows us to obtain, in a very robust way, the running of the coupling constants by demanding $\mu$-invariance of the effective semiclassical (Maxwell-Einstein) equations. In particular, we get the running of the electric charge of perturbative quantum electrodynamics. Furthermore, the method brings about a renormalization of the cosmological constant and the Newtonian gravitational constant. The running obtained for these dimensionful coupling constants has new relevant (non-logarithmic) contributions, not predicted by dimensional regularization.

PhysicsCoupling constantHigh Energy Physics - TheoryNuclear and High Energy PhysicsSemiclassical physicsFOS: Physical sciencesCosmological constantGeneral Relativity and Quantum Cosmology (gr-qc)lcsh:QC1-999General Relativity and Quantum CosmologyRenormalizationGravitational constantDimensional regularizationHigh Energy Physics - Theory (hep-th)Regularization (physics)Adiabatic processlcsh:PhysicsMathematical physics
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