Search results for "REGULARIZATION"

showing 10 items of 189 documents

Calculation of theO(? s 2 ) parity-violating structure functions in $$e^ + e^ - \to q\bar qg$$

1986

We calculate the two nonvanishingO(αs2) parity-violating structure functions that contribute to\(e^ + e^ - \xrightarrow{{\gamma ,Z}}q\bar qg\). We discuss how these can be measured. We work with massless quarks and gluons and use dimensional regularization to regularize ultra-violet and infrared singularities. We carefully discuss how to deal withγ5 in the dimensional regularization scheme when infrared singularities are present.

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeElectron–positron annihilationHigh Energy Physics::PhenomenologyElementary particleParity (physics)Massless particleDimensional regularizationQuark–gluon plasmaHigh Energy Physics::ExperimentGravitational singularityQuantum field theoryEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
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Lattice QCD: A Brief Introduction

2014

A general introduction to lattice QCD is given. The reader is assumed to have some basic familiarity with the path integral representation of quantum field theory. Emphasis is placed on showing that the lattice regularization provides a robust conceptual and computational framework within quantum field theory. The goal is to provide a useful overview, with many references pointing to the following chapters and to freely available lecture series for more in-depth treatments of specifics topics.

PhysicsParticle physicsTheoretical physicssymbols.namesakeWilson loopLattice (order)Regularization (physics)Path integral formulationLattice field theorysymbolsLattice QCDQuantum field theoryDirac operator
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Non-Perturbative Renormalization of Lattice Four-Fermion Operators without Power Subtractions

1999

A general non-perturbative analysis of the renormalization properties of $\Delta I=3/2$ four-fermion operators in the framework of lattice regularization with Wilson fermions is presented. We discuss the non-perturbative determination of the operator renormalization constants in the lattice Regularization Independent (RI or MOM) scheme. We also discuss the determination of the finite lattice subtraction coefficients from Ward Identities. We prove that, at large external virtualities, the determination of the lattice mixing coefficients, obtained using the RI renormalization scheme, is equivalent to that based on Ward Identities, in the continuum and chiral limits. As a feasibility study of …

PhysicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciencesFermionRenormalizationOperator (computer programming)High Energy Physics - LatticeRegularization (physics)Lattice (order)Non-perturbativeEngineering (miscellaneous)Mathematical physics
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N3LOHiggs boson and Drell-Yan production at threshold: The one-loop two-emission contribution

2014

In this paper, we study phenomenologically interesting soft radiation distributions in massless QCD. Specifically, we consider the emission of two soft partons off of a pair of lightlike Wilson lines, in either the fundamental or the adjoint representation, at next-to-leading order. Our results are an essential component of the next-to-next-to-next-to-leading order threshold corrections to both Higgs boson production in the gluon fusion channel and Drell-Yan lepton production. Our calculations are consistent with the recently published results for Higgs boson production. As a nontrivial cross-check on our analysis, we rederive a recent prediction for the Drell-Yan threshold cross section us…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsWilson loop010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDrell–Yan process01 natural sciencesGluonMassless particleDimensional regularization0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Use of helicity methods in evaluating loop integrals: A QCD example

1991

We discuss the use of helicity methods in evaluating loop diagrams by analyzing a specific example: the one-loop contribution to e+e- → qqg in massless QCD. By using covariant helicity representations for the spinor and vector wave functions we obtain the helicity amplitudes directly from the Feynman loop diagrams by covariant contraction. The necessary loop integrations are considerably simplified since one encounters only scalar loop integrals after contraction. We discuss crossing relations that allow one to obtain the corresponding one-loop helicity amplitudes for the crossed processes as e.g. qq → (W, Z, γ∗) + g including the real photon cases. As we treat the spin degrees of freedom i…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsSpinorScalar (mathematics)Helicitysymbols.namesakeDimensional regularizationDimensional reductionQuantum electrodynamicssymbolsFeynman diagramCovariant transformationMathematical physicsNuclear Physics B
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Heavy quark pair production in gluon fusion at next-to-next-to-leadingO(αs4)order: One-loop squared contributions

2008

We calculate the next-to-next-to-leading-order $\mathcal{O}({\ensuremath{\alpha}}_{s}^{4})$ one-loop squared corrections to the production of heavy-quark pairs in the gluon-gluon fusion process. Together with the previously derived results on the $q\overline{q}$ production channel, the results of this paper complete the calculation of the one-loop squared contributions of the next-to-next-to-leading-order $\mathcal{O}({\ensuremath{\alpha}}_{s}^{4})$ radiative QCD corrections to the hadroproduction of heavy flavors. Our results, with the full mass dependence retained, are presented in a closed and very compact form, in dimensional regularization.

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)GluonRenormalizationDimensional regularizationPair productionHigh Energy Physics::ExperimentProduction (computer science)Physical Review D
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One-loop amplitudes for four-point functions with two external massive quarks and two external massless partons up toO(ε2)

2006

We present complete analytical O({epsilon}{sup 2}) results on the one-loop amplitudes relevant for the next-to-next-to-leading order (NNLO) quark-parton model description of the hadroproduction of heavy quarks as given by the so-called loop-by-loop contributions. All results of the perturbative calculation are given in the dimensional regularization scheme. These one-loop amplitudes can also be used as input in the determination of the corresponding NNLO cross sections for heavy flavor photoproduction, and in photon-photon reactions.

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyOrder (ring theory)PartonMassless particleRenormalizationDimensional regularizationHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Nuclear ExperimentPhysical Review D
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ON FRACTIONAL RELAXATION

2002

Generalized fractional relaxation equations based on generalized Riemann-Liouville derivatives are combined with a simple short time regularization and solved exactly. The solution involves generalized Mittag-Leer functions. The associated frequency dependent susceptibilities are related to symmetrically broadened ColeCole susceptibilities occurring as Johari Goldstein -relaxation in many glass formers. The generalized susceptibilities exhibit a high frequency wing and strong minimum enhancement.

PhysicsQuantum mechanicsRelaxation (physics)Regularization (mathematics)Scaling and Disordered Systems
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Dimensional Regularization. Ultraviolet and Infrared Divergences

2015

The cornerstone of Quantum Field Theory is renormalization. We shall speak more about in the next chapters. Before, it is necessary to discuss the method. The best and most simple is, of course, dimensional regularization (doesn’t break the symmetries, doesn’t violate the Ward Identities, preserves Lorentz invariance, etc.). When explained consistently, it becomes very simple and clear. Here, we shortly discuss ultraviolet (UV) and infrared (IR) divergences with a few examples. However, in Chap. 8, we shall extensively treat one-loop two and three-point functions and analyse many more examples of IR and UV divergences.

PhysicsRenormalizationDimensional regularizationTheoretical physicsInfraredSimple (abstract algebra)Homogeneous spacemedicineQuantum field theoryLorentz covariancemedicine.disease_causeUltraviolet
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Note on the pragmatic mode-sum regularization method: Translational-splitting in a cosmological background

2021

The point-splitting renormalization method offers a prescription to calculate finite expectation values of quadratic operators constructed from quantum fields in a general curved spacetime. It has been recently shown by Levi and Ori that when the background metric possesses an isometry, like stationary or spherically symmetric black holes, the method can be upgraded into a pragmatic procedure of renormalization that produces efficient numerical calculations. In this note we show that when the background enjoys three-dimensional spatial symmetries, like homogeneous expanding universes, the above pragmatic regularization technique reduces to the well established adiabatic regularization metho…

PhysicsSpacetime010308 nuclear & particles physicsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)16. Peace & justiceIsometry (Riemannian geometry)01 natural sciencesGeneral Relativity and Quantum CosmologyRenormalizationTheoretical physicsQuadratic equationRegularization (physics)0103 physical sciencesMetric (mathematics)Homogeneous space010306 general physicsAdiabatic process
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