Search results for "Chromodynamics"

showing 10 items of 1030 documents

Space-like (vs. time-like) collinear limits in QCD: Is factorization violated?

2012

We consider the singular behaviour of QCD scattering amplitudes in kinematical configurations where two or more momenta of the external partons become collinear. At the tree level, this behaviour is known to be controlled by factorization formulae in which the singular collinear factor is universal (process independent). We show that this strict (process-independent) factorization is not valid at one-loop and higher-loop orders in the case of the collinear limit in space-like regions (e.g., collinear radiation from initial-state partons). We introduce a generalized version of all-order collinear factorization, in which the space-like singular factors retain some dependence on the momentum a…

High Energy Physics - TheoryNLO COMPUTATIONSNuclear and High Energy PhysicsHADRONIC COLLIDERSCiencias FísicasFOS: Physical sciencesPartonSpace (mathematics)01 natural sciences//purl.org/becyt/ford/1 [https]MomentumHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciences010306 general physicsMathematical physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsFísicaCharge (physics)//purl.org/becyt/ford/1.3 [https]Scattering amplitudeAstronomíaHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Gravitational singularityCIENCIAS NATURALES Y EXACTAS
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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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Triple collinear splitting functions at NLO for scattering processes with photons

2014

We present splitting functions in the triple collinear limit at next-to-leading order. The computation was performed in the context of massless QCD+QED, considering only processes which include at least one photon. Through the comparison of the IR divergent structure of splitting amplitudes with the expected known behavior, we were able to check our results. Besides that we implemented some consistency checks based on symmetry arguments and cross-checked the results among them. Studying photon-started processes, we obtained very compact results.

High Energy Physics - TheoryNLO COMPUTATIONSNuclear and High Energy PhysicsParticle physicsPhotonCiencias FísicasComputationFOS: Physical sciencesContext (language use)01 natural sciences//purl.org/becyt/ford/1 [https]High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsScatteringFísica//purl.org/becyt/ford/1.3 [https]Symmetry (physics)AstronomíaMassless particleHigh Energy Physics - PhenomenologyAmplitudeHigh Energy Physics - Theory (hep-th)CIENCIAS NATURALES Y EXACTASJournal of High Energy Physics
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Heavy quarkonium: progress, puzzles, and opportunities

2011

A golden age for heavy quarkonium physics dawned a decade ago, initiated by the confluence of exciting advances in quantum chromodynamics (QCD) and an explosion of related experimental activity. The early years of this period were chronicled in the Quarkonium Working Group (QWG) CERN Yellow Report (YR) in 2004, which presented a comprehensive review of the status of the field at that time and provided specific recommendations for further progress. However, the broad spectrum of subsequent breakthroughs, surprises, and continuing puzzles could only be partially anticipated. Since the release of the YR, the BESII program concluded only to give birth to BESIII; the $B$-factories and CLEO-c flo…

High Energy Physics - TheoryNuclear TheoryPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeTevatronB-C MESON; QCD SUM-RULES; NUCLEUS COLLISIONSAtomic01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Broad spectrumHigh Energy Physics - Phenomenology (hep-ph)Particle and Plasma Physicseffective field theoryBatavia TEVATRON CollNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentBrookhaven RHIC CollQuantum chromodynamicsPhysicsQuantum PhysicsLarge Hadron ColliderHigh Energy Physics - Lattice (hep-lat)lattice field theoryHERAQuarkoniumNuclear & Particles PhysicsCLEOB-C MESONHigh Energy Physics - PhenomenologyDESY HERA Stordecay [quarkonium]Jefferson LabParticle physicsFOS: Physical sciencesnonrelativistic [quantum chromodynamics]DeconfinementB-factoryNuclear Theory (nucl-th)High Energy Physics - Latticescattering [heavy ion]QCD SUM-RULES0103 physical sciencesNuclearddc:530010306 general physicsEngineering (miscellaneous)Particle Physics - Phenomenologyproduction [quarkonium]BES010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyplasma [quark gluon]FísicaMoleculartetraquarkHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]hadron spectroscopy [meson]hadron spectroscopy [quarkonium]High Energy Physics::Experimentheavy [quarkonium]NUCLEUS COLLISIONSThe European Physical Journal C
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Matter dependence of the four-loop QCD cusp anomalous dimension: from small angles to all angles

2019

We compute the fermionic contributions to the cusp anomalous dimension in QCD at four loops as an expansion for small cusp angle. As a byproduct we also obtain the respective terms of the four-loop HQET wave function anomalous dimension. Our new results at small angles provide stringent tests of a recent conjecture for the exact angle dependence of the matter terms in the four-loop cusp anomalous dimension. We find that the conjecture does not hold for two of the seven fermionic color structures, but passes all tests for the remaining terms. This provides strong support for the validity of the corresponding conjectured expressions with full angle dependence. Taking the limit of large Minkow…

High Energy Physics - TheoryNuclear and High Energy PhysicsConformal anomalyFOS: Physical sciencesConformal map01 natural sciencesTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Perturbative QCD0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityScattering Amplitudes010306 general physicsWave functionQuantum chromodynamicsCusp (singularity)Physics010308 nuclear & particles physicsPerturbative QCDEffective Field TheoriesWilson ’t Hooft and Polyakov loopsScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798Journal of High Energy Physics
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On the zero crossing of the three-gluon vertex

2016

We report on new results on the infrared behaviour of the three-gluon vertex in quenched Quantum Chormodynamics, obtained from large-volume lattice simulations. The main focus of our study is the appearance of the characteristic infrared feature known as 'zero crossing', the origin of which is intimately connected with the nonperturbative masslessness of the Faddeev-Popov ghost. The appearance of this effect is clearly visible in one of the two kinematic configurations analyzed, and its theoretical origin is discussed in the framework of Schwinger-Dyson equations. The effective coupling in the momentum subtraction scheme that corresponds to the three-gluon vertex is constructed, revealing t…

High Energy Physics - TheoryNuclear and High Energy PhysicsLattice simulationsInfraredHigh Energy Physics::LatticeFOS: Physical sciencesThree-gluon vertexKinematicsnonperturbative01 natural sciencesSchwinger–Dyson equations[ PHYS.HTHE ] Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeQuantum mechanicsLattice (order)0103 physical sciencesddc:530Exact locationquantum chromodynamics: quenching010306 general physicsMathematical physicslatticeQuantum chromodynamicsPhysicsZero crossing010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat][PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]High Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)[ PHYS.HLAT ] Physics [physics]/High Energy Physics - Lattice [hep-lat]gluon: vertexcrossingZero crossingghostlcsh:QC1-999GluonDyson-Schwinger equationHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]infrared[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]lcsh:Physics
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Confinement, the gluon propagator and the interquark potential for heavy mesons

2012

The interquark static potential for heavy mesons described by a massive one-gluon exchange interaction obtained from the propagator of the truncated Dyson-Schwinger equations does not reproduced the expected Cornell potential. I show that no formulation based on a finite propagator will lead to confinement of quenched QCD. I propose a mechanism based on a singular nonperturbative coupling constant which has the virtue of giving rise to a finite gluon propagator and (almost) linear confinement. The mechanism can be slightly modified to produce the screened potentials of unquenched QCD.

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeFOS: Physical sciencesMechanism based01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsPhysicsCoupling constantQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExchange interactionPropagatorGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Quark ConfinementChiral-Symmetry BreakingFísica nuclearHigh Energy Physics::ExperimentThe European Physical Journal A
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Numerical Multi-Loop Calculations via Finite Integrals and One-Mass EW-QCD Drell-Yan Master Integrals

2017

We study a recently-proposed approach to the numerical evaluation of multi-loop Feynman integrals using available sector decomposition programs. As our main example, we consider the two-loop integrals for the $\alpha \alpha_s$ corrections to Drell-Yan lepton production with up to one massive vector boson in physical kinematics. As a reference, we evaluate these planar and non-planar integrals by the method of differential equations through to weight five. Choosing a basis of finite integrals for the numerical evaluation with SecDec3 leads to tremendous performance improvements and renders the otherwise problematic seven-line topologies numerically accessible. As another example, basis integ…

High Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsSpeedupDifferential equationFOS: Physical sciences01 natural sciencesVector bosonHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPerturbative QCDlcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsMathematical physicsPhysicsQuantum chromodynamicsBasis (linear algebra)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMassless particleLoop (topology)High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798LeptonQuark Masses and SM Parameters
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Infrared facets of the three-gluon vertex

2021

We present novel lattice results for the form factors of the quenched three-gluon vertex of QCD, in two special kinematic configurations that depend on a single momentum scale. We consider three form factors, two associated with a classical tensor structure and one without tree-level counterpart, exhibiting markedly different infrared behaviors. Specifically, while the former display the typical suppression driven by a negative logarithmic singularity at the origin, the latter saturates at a small negative constant. These exceptional features are analyzed within the Schwinger-Dyson framework, with the aid of special relations obtained from the Slavnov-Taylor identities of the theory. The em…

High Energy Physics - TheoryNuclear and High Energy PhysicsQC1-999High Energy Physics::LatticeFOS: Physical sciencesThree-gluon vertexLattice QCD01 natural sciencesMomentumTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)SingularitySchwinger-Dyson equations0103 physical sciencesTensor010306 general physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsPhysicsHigh Energy Physics - Lattice (hep-lat)Lattice QCDQCDHigh Energy Physics - PhenomenologyLattice (module)High Energy Physics - Theory (hep-th)Vertex (curve)Constant (mathematics)Physics Letters B
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Hadronic light-by-light scattering contribution to the muon $g-2$ from lattice QCD: semi-analytical calculation of the QED kernel

2023

Hadronic light-by-light scattering is one of the virtual processes that causes the gyromagnetic factor $g$ of the muon to deviate from the value of two predicted by Dirac's theory. This process makes one of the largest contributions to the uncertainty of the Standard Model prediction for the muon $(g-2)$. Lattice QCD allows for a first-principles approach to computing this non-perturbative effect. In order to avoid power-law finite-size artifacts generated by virtual photons in lattice simulations, we follow a coordinate-space approach involving a weighted integral over the vertices of the QCD four-point function of the electromagnetic current carried by the quarks. Here we present in detai…

High Energy Physics - TheoryNuclear and High Energy Physicsmagnetic momentn-point function530 Physicsspace Euclidean4FOS: Physical sciences[PHYS.HLAT] Physics [physics]/High Energy Physics - Lattice [hep-lat]nonperturbativeEuclideandimension 4quarkHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)dimensionmuonquantum chromodynamicsquantum electrodynamicsphoton photoncomputerlatticeperturbation theoryphoton photon scatteringeffect nonperturbative[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat][PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]effectHigh Energy Physics - Lattice (hep-lat)scatteringphotonlattice field theoryspace530 Physikcurrent[PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics - PhenomenologyelectromagneticHigh Energy Physics - Theory (hep-th)photon virtualn-point function 4finite size[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]virtual[PHYS.HTHE] Physics [physics]/High Energy Physics - Theory [hep-th]current electromagnetic
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