Search results for "PERTURBATIVE QCD"

showing 10 items of 174 documents

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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Weak and strong coupling equilibration in nonabelian gauge theories

2015

We present a direct comparison studying equilibration through kinetic theory at weak coupling and through holography at strong coupling in the same set-up. The set-up starts with a homogeneous thermal state, which then smoothly transitions through an out-of-equilibrium phase to an expanding system undergoing boost-invariant flow. This first apples-to-apples comparison of equilibration provides a benchmark for similar equilibration processes in heavy-ion collisions, where the equilibration mechanism is still under debate. We find that results at weak and strong coupling can be smoothly connected by simple, empirical power-laws for the viscosity, equilibration time and entropy production of t…

High Energy Physics - TheoryNuclear and High Energy Physicsquark-gluon plasmaNuclear TheoryeducationNuclear TheoryFOS: Physical sciences114 Physical sciencesperturbative QCD01 natural sciencesNuclear Theory (nucl-th)ViscosityHigh Energy Physics - Phenomenology (hep-ph)AdS-CFT correspondencePhase (matter)0103 physical sciencesGauge theoryNuclear Experiment010306 general physicsCouplingPhysicsta114010308 nuclear & particles physicsEntropy productionkvarkki-gluoniplasmaHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Flow (mathematics)Quantum electrodynamicsKinetic theory of gasesStrong couplingParticle Physics - Theoryholography and quark-gluon plasmasJournal of High Energy Physics
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Pentagon functions for massless planar scattering amplitudes

2018

Loop amplitudes for massless five particle scattering processes contain Feynman integrals depending on the external momentum invariants: pentagon functions. We perform a detailed study of the analyticity properties and cut structure of these functions up to two loops in the planar case, where we classify and identify the minimal set of basis functions. They are computed from the canonical form of their differential equations and expressed in terms of generalized polylogarithms, or alternatively as one-dimensional integrals. We present analytical expressions and numerical evaluation routines for these pentagon functions, in all kinematical configurations relevant to five-particle scattering …

High Energy Physics - TheoryParticle physicsNuclear and High Energy PhysicsDifferential equation530 PhysicsFOS: Physical sciencesBasis function10192 Physics Institute01 natural sciencesMomentumHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesPerturbative QCDCanonical formlcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsScattering AmplitudesMathematical physicsPhysics010308 nuclear & particles physicsScatteringScattering amplitudeMassless particlePentagonHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798Journal of High Energy Physics
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Causal representation of multi-loop Feynman integrands within the loop-tree duality

2021

The numerical evaluation of multi-loop scattering amplitudes in the Feynman representation usually requires to deal with both physical (causal) and unphysical (non-causal) singularities. The loop-tree duality (LTD) offers a powerful framework to easily characterise and distinguish these two types of singularities, and then simplify analytically the underling expressions. In this paper, we work explicitly on the dual representation of multi-loop Feynman integrals generated from three parent topologies, which we refer to as Maximal, Next-to-Maximal and Next-to-Next-to-Maximal loop topologies. In particular, we aim at expressing these dual contributions, independently of the number of loops an…

High Energy Physics - TheoryPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDuality (mathematics)PropagatorDual representation01 natural sciencesAlgebraHigh Energy Physics - Phenomenologysymbols.namesakeIntegerSimple (abstract algebra)Perturbative QCD0103 physical sciencessymbolslcsh:QC770-798Feynman diagramlcsh:Nuclear and particle physics. Atomic energy. RadioactivityGravitational singularityScattering Amplitudes010306 general physicsRepresentation (mathematics)Duality in Gauge Field TheoriesJournal of High Energy Physics
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QCD sum rule determination of the charm-quark mass

2011

QCD sum rules involving mixed inverse moment integration kernels are used in order to determine the running charm-quark mass in the $\bar{MS}$ scheme. Both the high and the low energy expansion of the vector current correlator are involved in this determination. The optimal integration kernel turns out to be of the form $p(s) = 1 - (s_0/s)^2$, where $s_0$ is the onset of perturbative QCD. This kernel enhances the contribution of the well known narrow resonances, and reduces the impact of the data in the range $s \simeq 20 - 25 GeV^2$. This feature leads to a substantial reduction in the sensitivity of the results to changes in $s_0$, as well as to a much reduced impact of the experimental u…

High Energy Physics - TheoryQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsQCD sum rulesParticle physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesOrder (ring theory)InversePerturbative QCDFísicaHigh Energy Physics - ExperimentCharm quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)High Energy Physics::ExperimentSum rule in quantum mechanicsSensitivity (control systems)
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Quark–hadron duality: Pinched kernel approach

2016

Hadronic spectral functions measured by the ALEPH collaboration in the vector and axial-vector channels are used to study potential quark-hadron duality violations (DV). This is done entirely in the framework of pinched kernel finite energy sum rules (FESR), i.e. in a model independent fashion. The kinematical range of the ALEPH data is effectively extended up to $s = 10\; {\mbox{GeV}^2}$ by using an appropriate kernel, and assuming that in this region the spectral functions are given by perturbative QCD. Support for this assumption is obtained by using $e^+ e^-$ annihilation data in the vector channel. Results in both channels show a good saturation of the pinched FESR, without further nee…

High Energy Physics - TheoryQuarkNuclear and High Energy PhysicsParticle physicsAlephHadronFOS: Physical sciencesGeneral Physics and AstronomyDuality (optimization)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciences010306 general physicsPhysicsQCD sum rulesAnnihilation010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPerturbative QCDAstronomy and AstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Kernel (statistics)High Energy Physics::ExperimentModern Physics Letters A
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Latest predictions from the EbyE NLO EKRT model

2019

We present the latest results from the NLO pQCD + saturation + viscous hydrodynamics (EbyE NLO EKRT) model. The parameters in the EKRT saturation model are fixed by the charged hadron multiplicity in the 0-5 \% 2.76 TeV Pb+Pb collisions. The $\sqrt{s}$, $A$ and centrality dependence of the initial particle production follows then from the QCD dynamics of the model. This allows us to predict the $\sqrt{s}$ and $A$ dependence of the particle production. We show that our results are in an excellent agreement with the low-$p_T$ data from 2.76 TeV and 5.02 TeV Pb+Pb collisions at the LHC as well as with the data from the 200 GeV Au+Au collisions at RHIC. In particular, we study the centrality de…

Nuclear and High Energy PhysicsCOLLISIONSMULTIPLICITIESNuclear TheoryHadronFOS: Physical scienceshiukkasfysiikka7. Clean energy01 natural sciences114 Physical sciencesdissipative fluid dynamicNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsTRANSVERSE ENERGIESNuclear ExperimentNuclear theoryMass numberQuantum chromodynamicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicssaturationHigh Energy Physics::PhenomenologyMultiplicity (mathematics)heavy-ion collisionsCharged particleHigh Energy Physics - PhenomenologyHigh Energy Physics::Experimentperturbative QCD calculationsydinfysiikka
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Broad excitations in a 2+1D overoccupied gluon plasma

2021

Motivated by the initial stages of high-energy heavy-ion collisions, we study excitations of far-from-equilibrium 2+1 dimensional gauge theories using classical-statistical lattice simulations. We evolve field perturbations over a strongly overoccupied background undergoing self-similar evolution. While in 3+1D the excitations are described by hard-thermal loop theory, their structure in 2+1D is nontrivial and nonperturbative. These nonperturbative interactions lead to broad excitation peaks in spectral and statistical correlation functions. Their width is comparable to the frequency of soft excitations, demonstrating the absence of soft quasiparticles in these theories. Our results also su…

Nuclear and High Energy PhysicsCOLLISIONSNuclear TheoryField (physics)FOS: Physical sciencesLattice QCDQC770-798hiukkasfysiikka01 natural sciences114 Physical sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesPerturbative QCDfysikkField theory (psychology)Gauge theory010306 general physicsKINETIC-THEORYUNIVERSAL DYNAMICSPhysics:Matematikk og Naturvitenskap: 400::Fysikk: 430 [VDP]MASS SCALENUCLEI010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)kvarkki-gluoniplasmaPerturbative QCDLattice QCDFIELD-THEORY3. Good healthGluonHigh Energy Physics - PhenomenologyQuantum electrodynamicsQuark–gluon plasmaQuasiparticleQuark-Gluon PlasmaGAUGE-THEORIESJournal of High Energy Physics
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Vacuum correlators at short distances from lattice QCD

2021

Non-perturbatively computing the hadronic vacuum polarization at large photon virtualities and making contact with perturbation theory enables a precision determination of the electromagnetic coupling at the $Z$ pole, which enters global electroweak fits. In order to achieve this goal ab initio using lattice QCD, one faces the challenge that, at the short distances which dominate the observable, discretization errors are hard to control. Here we address challenges of this type with the help of static screening correlators in the high-temperature phase of QCD, yet without incurring any bias. The idea is motivated by the observations that (a) the cost of high-temperature simulations is typica…

Nuclear and High Energy PhysicsHigh Energy Physics::Latticepolecostshep-latFOS: Physical sciencesLattice QCDQC770-798nonperturbativeoperator product expansion53001 natural sciences7. Clean energythermal [correlation function]lattice [perturbation theory]High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivityprecision measurement [electroweak interaction]quantum chromodynamics0103 physical sciencesPerturbative QCDhadronic [vacuum polarization]ddc:530010306 general physicsParticle Physics - Phenomenology010308 nuclear & particles physicsscreeningComputer Science::Information RetrievalphotonHigh Energy Physics - Lattice (hep-lat)lattice field theorytemperaturehep-phParticle Physics - LatticeHigh Energy Physics - Phenomenologyelectromagnetic [coupling]flavor [quark]Journal of High Energy Physics
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Revisiting the D-meson hadroproduction in general-mass variable flavour number scheme

2018

We introduce a novel realization of the open heavy-flavour hadroproduction in general-mass variable flavour number scheme at next-to-leading order in perturbative QCD. The principal novelty with respect to the earlier works is in the treatment of small-transverse-momentum limit, which has been a particularly challenging kinematic region in the past. We show that by a suitable choice of scheme, it is possible to obtain a well-behaved description of the open heavy-flavour hadroproduction cross sections from zero up to asymptotically high transverse momentum. We contrast our calculation with the available D$^0$-meson data as measured by the LHCb and ALICE collaborations at the LHC, finding a v…

Nuclear and High Energy PhysicsParticle physicsFRAGMENTATION FUNCTIONSFlavourFOS: Physical sciences114 Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)HEAVY-QUARK PRODUCTION0103 physical sciencesD mesonSCATTERINGlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNUCLEAR COLLISIONSLimit (mathematics)QCD ANALYSIS010306 general physicsVariable (mathematics)PhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyContrast (statistics)Perturbative QCDQCD phenomenologyHigh Energy Physics - PhenomenologyPARTON DISTRIBUTIONSlcsh:QC770-798High Energy Physics::ExperimentLHCHADRON-COLLISIONSMATTERRealization (systems)TO-LEADING ORDER
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