Search results for "Summation"

showing 10 items of 97 documents

Transverse-momentum resummation for vector-boson pair production at NNLL+NNLO

2015

We consider the transverse-momentum ($p_T$) distribution of $ZZ$ and $W^+W^-$ boson pairs produced in hadron collisions. At small $p_T$, the logarithmically enhanced contributions due to multiple soft-gluon emission are resummed to all orders in QCD perturbation theory. At intermediate and large values of $p_T$, we consistently combine resummation with the known fixed-order results. We exploit the most advanced perturbative information that is available at present: next-to-next-to-leading logarithmic resummation combined with the next-to-next-to-leading fixed-order calculation. After integration over $p_T$, we recover the known next-to-next-to-leading order result for the inclusive cross se…

Quantum chromodynamicsPhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron Collider530 PhysicsHadronHigh Energy Physics::PhenomenologyFOS: Physical sciences10192 Physics InstituteVector bosonHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)RapidityHigh Energy Physics::ExperimentPerturbation theory (quantum mechanics)Resummation3106 Nuclear and High Energy PhysicsNuclear Experiment
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Determination of alpha_s at NLO*+NNLL from a global fit of the low-z parton-to-hadron fragmentation functions in e+e- and DIS collisions

2014

The QCD coupling alpha_s is determined from a combined analysis of experimental e+e- and e-p jet data confronted to theoretical predictions of the energy evolution of the parton-to-hadron fragmentation functions (FFs) moments --multiplicity, peak, width, skewness-- at low fractional hadron momentum z. The impact of approximate next-to-leading order (NLO*) corrections plus next-to-next-to-leading log (NNLL) resummations, compared to previous LO+NLL calculations, is discussed. A global fit of the full set of existing data, amounting to 360 FF moments at collision energies sqrt(s)~1--200 GeV, results in alpha_s(m_Z^2)=0.1189^{+0.0025}_{-0.0014} at the Z mass.

Quantum chromodynamicsPhysics[PHYS]Physics [physics]Particle physicsta114PhysicsQC1-999HadronHigh Energy Physics::PhenomenologyFOS: Physical sciencesPartonElectronDeep inelastic scatteringHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)parton-to-hadron fragmentationSkewnessHigh Energy Physics::ExperimentResummationMultiplicity (chemistry)Nuclear ExperimentParticle Physics - Phenomenology
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Exclusive radiative Higgs decays as probes of light-quark Yukawa couplings

2015

We present a detailed analysis of the rare exclusive Higgs-boson decays into a single vector meson and a photon and investigate the possibility of using these processes to probe the light-quark Yukawa couplings. We work with an effective Lagrangian with modified Higgs couplings to account for possible new-physics effects in a model-independent way. The h->V\gamma{} decay rate is governed by the destructive interference of two amplitudes, one of which involves the Higgs coupling to the quark anti-quark pair inside the vector meson. We derive this amplitude at next-to-leading order in \alpha_s using QCD factorization, including the resummation of large logarithmic corrections and accounting f…

Quantum chromodynamicsQuarkPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHadronYukawa potentialFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentVector mesonResummationJournal of High Energy Physics
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Renormalization and Scale Evolution of the Soft-Quark Soft Function

2020

Soft functions defined in terms of matrix elements of soft fields dressed by Wilson lines are central components of factorization theorems for cross sections and decay rates in collider and heavy-quark physics. While in many cases the relevant soft functions are defined in terms of gluon operators, at subleading order in power counting soft functions containing quark fields appear. We present a detailed discussion of the properties of the soft-quark soft function consisting of a quark propagator dressed by two finite-length Wilson lines connecting at one point. This function enters in the factorization theorem for the Higgs-boson decay amplitude of the $h\to\gamma\gamma$ process mediated by…

QuarkHigh Energy Physics - TheoryNuclear and High Energy PhysicsHigh Energy Physics::LatticeFOS: Physical sciencesPosition and momentum spaceRenormalizationsymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)FactorizationPerturbative QCDRenormalization Grouplcsh:Nuclear and particle physics. Atomic energy. RadioactivityResummationMathematical physicsPhysicsHigh Energy Physics::PhenomenologyPropagatorEffective Field TheoriesRenormalization groupHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Weierstrass factorization theoremsymbolslcsh:QC770-798High Energy Physics::ExperimentResummation
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Subjet multiplicity of gluon and quark jets reconstructed with thek⊥algorithm inpp¯collisions

2002

The D empty set Collaboration has studied for the first time the properties of hadron-collider jets reconstructed with a successive-combination algorithm based on relative transverse momenta (k(perpendicular to)) of energy clusters. Using the standard value D = 1.0 of the jet-separation parameter in the k(perpendicular to) algorithm, we find that the p(T) of such jets is higher than the E-T of matched jets reconstructed with cones of radius R = 0.7, by about 5 (8) GeV at p(T) approximate to90 (240) GeV. To examine internal jet structure, the k(perpendicular to) algorithm is applied within D = 0.5 jets to resolve any subjets. The multiplicity of subjets in jet samples at roots = 1800 GeV and…

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaMultiplicity (mathematics)RadiusJet (particle physics)Deep inelastic scattering01 natural sciencesGluonNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentResummationNuclear Experiment010306 general physicsAlgorithmEvent generatorPhysical Review D
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Three-Loop Quark Jet Function.

2018

We calculate the massless quark jet function to three-loop order. The quark jet function is a universal ingredient in SCET factorization for many collider and decay processes with quark initiated final state jets. Our three-loop result contributes to the resummation for observables probing the invariant mass of final state quark jets at primed next-to-next-to-next-to-leading-logarithmic accuracy. It represents the first complete three-loop result for a factorization ingredient describing collinear radiation. Furthermore it constitutes a major component of the N-jettiness subtraction method at next-to-next-to-next-to-leading order accuracy, which eventually may enable the calculation of full…

QuarkPhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyObservableJet (particle physics)01 natural scienceslaw.inventionMassless particleFactorizationlaw0103 physical sciencesInvariant massHigh Energy Physics::ExperimentResummation010306 general physicsColliderPhysical review letters
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Effective Field Theories for heavy probes in a hot QCD plasma and in the early universe

2016

International audience; There are many interesting problems in heavy-ion collisions and in cosmology that involve the interaction of a heavy particle with a medium. An example is the dissociation of heavy quarkonium seen in heavy-ion collisions. This was believed to be due to the screening of chromoelectric fields that prevents the heavy quarks from binding, however in the last years several perturbative and lattice computations have pointed out to the possibility that dissociation is due to the finite lifetime of a quarkonium state inside the medium. Regarding cosmology, the study of the behavior of heavy Majorana neutrinos in a hot medium is important to understand if this model can expla…

Quarkcosmological modelParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]QC1-999Populationdissociationquantum chromodynamics: plasma01 natural sciences7. Clean energydark matterCosmologythermalquarkonium: heavyBaryon asymmetryparticle: heavy0103 physical sciencesquantum chromodynamicseffective field theoriesheavy quarkNuclear Experiment010306 general physicseducationMajorana neutrinoslatticeeffective field theory: nonrelativisticQuantum chromodynamicsPhysicseducation.field_of_studyquantum chromodynamics: nonrelativisticquarkonium suppressionta114010308 nuclear & particles physicsPhysicsscreeningquarkonium: suppressionHigh Energy Physics::PhenomenologychromoelectricQuarkoniumheavy ionMAJORANAresummation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]baryon: asymmetryneutrino: Majoranaquarkonium: lifetimeNeutrinoQuark Confinement and the Hadron Spectrum
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Three-particle correlations in QCD parton showers

2011

Three-particle correlations in quark and gluon jets are computed for the first time in perturbative QCD. We give results in the double logarithmic approximation and the modified leading logarithmic approximation. In both resummation schemes, we use the formalism of the generating functional and solve the evolution equations analytically from the steepest descent evaluation of the one-particle distribution. We thus provide a further test of the local parton hadron duality and make predictions for the LHC.

QuarkjetsNuclear and High Energy PhysicsParticle physicsHadronFOS: Physical sciencesParton01 natural sciencespQCDHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesResummation010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDFísicaHadronizationGluonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentLPHDhadronization
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Three-particle correlations in QCD jets and beyond

2011

In this paper, we present a more detailed version of our previous work for three-particle correlations in quark and gluon jets [1]. We give theoretical results for this observable in the double logarithmic approximation and the modified leading logarithmic approximation. In both resummation schemes, we use the formalism of the generating functional and solve the evolution equations analytically from the steepest descent evaluation of the one-particle distribution. In addition, in this paper we include predictions beyond the limiting spectrum approximation and study this observable near the hump of the single inclusive distribution. We thus provide a further test of the local parton hadron d…

QuarkjetsNuclear and High Energy PhysicsParticle physicsLogarithmHadronFOS: Physical sciencesParton01 natural sciencespQCDHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStatistical physicsResummation010306 general physicsQuantum chromodynamicsPhysicsinclusive correlations010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaObservableMLLAGluonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Soft-gluon resummation for boosted top-quark production at hadron colliders

2012

We investigate the production of highly energetic top-quark pairs at hadron colliders, focusing on the case where the invariant mass of the pair is much larger than the mass of the top quark. In particular, we set up a factorization formalism appropriate for describing the differential partonic cross section in the double soft and small-mass limit, and explain how to resum simultaneously logarithmic corrections arising from soft gluon emission and from the ratio of the pair-invariant mass to that of the top quark to next-to-next-to-leading logarithmic accuracy. We explore the implications of our results on approximate next-to-next-to-leading order formulas for the differential cross section…

Scattering cross-sectionPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkLogarithm010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesGluonNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesInvariant massHigh Energy Physics::ExperimentResummation010306 general physics
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