Search results for "Wilson loop"

showing 10 items of 20 documents

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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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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Connection between the pinch technique and the background field method

1995

The connection between the pinch technique and the background field method is further explored. We show by explicit calculations that the application of the pinch technique in the framework of the background field method gives rise to exactly the same results as in the linear renormalizable gauges. The general method for extending the pinch technique to the case of Green's functions with off-shell fermions as incoming particles is presented. As an example, the one-loop gauge independent quark self-energy is constructed. We briefly discuss the possibility that the gluonic Green's functions, obtained by either method, correspond to physical quantities.

PhysicsWilson loop010308 nuclear & particles physicsBackground field methodHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaPropagator01 natural sciencesHigh Energy Physics - Phenomenologysymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Self-energyQuantum electrodynamics0103 physical sciencesPinchsymbolsFeynman diagram010306 general physicsS-matrixPhysical quantityPhysical Review D
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The importance of being rigid: D6-brane model building on with discrete torsion

2013

Model building with rigid D6-branes on the Type IIA orientifold onT 6 =Z2 Z 0 with discrete torsion is considered. The systematic search for models of particle physics is signicantly reduced by proving new symmetries among dierent lattice orientations. Suitable rigid D6-branes without matter in adjoint and symmetric representations are classied, and SO(2N) and USp(2N) gauge factors on orientifold invariant D6-branes are distinguished in terms of their discrete Wilson line and displacement parameters. Constraints on the nonexistence of exotic matter prohibit global completions of local MSSM and leftright symmetric models, while globally dened supersymmetric Pati-Salam models are found. For t…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsTheoretical physicsParticle physicsWilson loopOrientifoldHigh Energy Physics::PhenomenologyExotic matterYukawa potentialSupersymmetryBraneMinimal Supersymmetric Standard ModelNuclear Physics B
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Heavy quark decomposition of the S matrix and its relation to the pinch technique.

1995

We propose a decomposition of the S-matrix into individually gauge invariant sub-amplitudes, which are kinematically akin to propagators, vertices, boxes, etc. This decompsition is obtained by considering limits of the S-matrix when some or all of the external particles have masses larger than any other physical scale. We show at the one-loop level that the effective gluon self-energy so defined is physically equivalent to the corresponding gauge independent self-energy obtained in the framework of the pinch technique. The generalization of this procedure to arbitrary gluonic $n$-point functions is briefly discussed.

QuarkPhysicsHigh Energy Physics - TheoryParticle physicsWilson loop010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::LatticePropagatorFísicaFOS: Physical sciences01 natural sciencesMatrix (mathematics)Self-energyHigh Energy Physics - Theory (hep-th)0103 physical sciencesGauge theoryInvariant (mathematics)010306 general physicsS-matrixMathematical physicsPhysical review. D, Particles and fields
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The two-loop soft function for heavy quark pair production at future linear colliders

2014

We report on the calculation of the threshold soft function for heavy quark pair production in e+ e- annihilation at two-loop order. Our main result is a generalization of the familiar Drell-Yan threshold soft function to the case of non-zero primary quark mass. We set up a framework based on the method of differential equations which allows for the straightforward calculation of the bare soft function to arbitrarily high orders in the dimensional regularization parameter. Remarkably, we find that we can obtain the bare two-loop Drell-Yan soft function from the heavy quark soft function to the order in epsilon required for a two-loop calculation by making simple replacements. We expect that…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsWilson loop010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciences01 natural sciencesBottom quarkMatrix (mathematics)Dimensional regularizationHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesConnection (algebraic framework)010306 general physics
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3-Loop Heavy Flavor Corrections in Deep-Inelastic Scattering with Two Heavy Quark Lines

2014

We consider gluonic contributions to the heavy flavor Wilson coefficients at 3-loop order in QCD with two heavy quark lines in the asymptotic region $Q^2 \gg m_{1(2)}^2$. Here we report on the complete result in the case of two equal masses $m_1 = m_2$ for the massive operator matrix element $A_{gg,Q}^{(3)}$, which contributes to the corresponding heavy flavor transition matrix element in the variable flavor number scheme. Nested finite binomial sums and iterated integrals over square-root valued alphabets emerge in the result for this quantity in $N$ and $x$-space, respectively. We also present results for the case of two unequal masses for the flavor non-singlet OMEs and on the scalar int…

QuarkQuantum chromodynamicsPhysicsParticle physicsWilson loopHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesDeep inelastic scatteringLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Field theory (psychology)High Energy Physics::ExperimentFlavor
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JIMWLK evolution of the odderon

2016

We study the effects of a parity-odd "odderon" correlation in JIMWLK renormalization group evolution at high energy. Firstly we show that in the eikonal picture where the scattering is described by Wilson lines, one obtains a strict mathematical upper limit for the magnitude of the odderon amplitude compared to the parity even pomeron one. This limit increases with N_c, approaching infinity in the infinite N_c limit. We use a systematic extension of the Gaussian approximation including both 2- and 3-point correlations which enables us to close the system of equations even at finite N_c. In the large-N_c limit we recover an evolution equation derived earlier. By solving this equation numeric…

SMALL-X EVOLUTIONWilson loopNuclear TheoryLARGE NUCLEIWilson linesFOS: Physical sciencesField (mathematics)114 Physical sciences01 natural sciencesHIGH-ENERGY SCATTERINGColor-glass condensateRENORMALIZATION-GROUPNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSPomeronHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsquantum chromodynamics0103 physical sciencesEQUATION010306 general physicsPhysicsta114evolution equations010308 nuclear & particles physicsScatteringEikonal equationHERA-DATAHigh Energy Physics::PhenomenologyCOLOR GLASS CONDENSATEodderonRenormalization groupHigh Energy Physics - PhenomenologyAmplitudeJIMWLKPA-COLLISIONSBK EVOLUTION
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Structure of longitudinal chromomagnetic fields in high energy collisions

2014

We compute expectation values of spatial Wilson loops in the forward light cone of high-energy collisions. We consider ensembles of gauge field configurations generated from a classical Gaussian effective action as well as solutions of high-energy renormalization group evolution with fixed and running coupling. The initial fields correspond to a color field condensate exhibiting domain-like structure over distance scales of order the saturation scale. At later times universal scaling emerges at large distances for all ensembles, with a nontrivial critical exponent. Finally, we compare the results for the Wilson loop to the two-point correlator of magnetic fields.

We compute expectation values of spatial Wilson loops in the forward light cone of high-energy collisions. We consider ensembles of gauge field configurations generated from a classical Gaussian effective action as well as solutions of high-energy renormalization group evolution with fixed and running coupling. The initial like structure over distance scales of oder the saturation scale. At later times universal scaling emerges at large distances for all ensembles with a nontrivial critical exponent. Finally we compare the resulats for the Wilson loop to the two-point correlator of magnetic fields. (C) 2014 The Authors. Published by Elsevier BV This is an open access article under the CC BY licenseNuclear and High Energy PhysicsWilson loopLARGE NUCLEINuclear TheoryField (physics)FOS: Physical sciences114 Physical sciences01 natural sciencesColor-glass condensateRENORMALIZATION-GROUPNuclear Theory (nucl-th)GLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)Light cone0103 physical sciencesSCATTERINGGauge theory010306 general physicsSMALL-XEffective actionPhysicsCORRELATORSta114010308 nuclear & particles physicsCOLOR GLASS CONDENSATERenormalization groupEVOLUTIONJIMWLK EQUATIONHigh Energy Physics - PhenomenologySATURATIONQuantum electrodynamicsCritical exponentPhysics Letters B
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JIMWLK and beyond: From concepts to observables

2016

Volume: 112 Host publication title: 6th International Conference on Physics Opportunities at an Electron-Ion Collider The Color Glass Condensate and its associated evolution equation, the JIMWLK equation have applications to many observables far beyond totally inclusive observables. The phenomenology is so rich that little has been done to explore beyond scaling behavior of correlators. We show first examples that exemplify the considerations necessary to access additional information both experimentally and theoretically and demonstrate that the Wilson line correlators appearing throughout make it imperative to consistently take into account that one is dealing with correlators of group el…

ta114Operations research010308 nuclear & particles physicsComputer sciencePhysicsQC1-999scalingCOLOR GLASS CONDENSATEObservable114 Physical sciences01 natural sciencesSTATESMALL X EVOLUTIONColor-glass condensateWilson loopTheoretical physicsODDERONevolution equation0103 physical sciencesEvolution equationcolor glass condensate010306 general physicsScalingN-CEPJ Web of Conferences
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