Search results for "Qcd"

showing 10 items of 614 documents

Search for the Standard Model Higgs boson in the two photon decay channel with the ATLAS detector at the LHC

2011

A search for the Standard Model Higgs boson in the two photon decay channel is reported, using 1.08 fb−11.08 fb[superscript −1] of proton–proton collision data at a centre-of-mass energy of 7 TeV recorded by the ATLAS detector. No significant excess is observed in the investigated mass range of 110–150 GeV. Upper limits on the cross-section times branching ratio of between 2.0 and 5.8 times the Standard Model prediction are derived for this mass range.

Nuclear and High Energy PhysicsParticle physicsPhotonFOS: Physical sciencesElementary particleFotonesddc:500.201 natural sciencesMassless Particles530Nnlo QCDHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified Theoryddc:530CollisionsHigh Energy Physics010306 general physicsNuclear ExperimentBosonPhysicsLarge Hadron ColliderATLAS detector010308 nuclear & particles physicsBranching fractionParton DistributionsSettore FIS/01 - Fisica SperimentaleFísicaATLASHadron CollidersMassless particleATLAS; LHC; Higgs bosonstandard model Higgs bosonHiggs bosonFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Exclusive heavy vector meson electroproduction to NLO in collinear factorisation

2021

We compute the exclusive electroproduction, $\gamma^* p \rightarrow V p$, of heavy quarkonia $V$ to NLO in the collinear factorisation scheme, which has been formally proven for this process. The inclusion of an off-shell virtuality $Q^2$ carried by the photon extends the photoproduction phase space of the exclusive heavy quarkonia observable to electroproduction kinematics. This process is relevant for diffractive scattering at HERA and the upcoming EIC, as well as at the proposed LHeC and FCC.

Nuclear and High Energy PhysicsParticle physicsPhotonNuclear TheoryFOS: Physical sciencesQC770-798hiukkasfysiikka01 natural sciences114 Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)FactorizationNuclear and particle physics. Atomic energy. RadioactivityNLO Computations0103 physical sciencesVector mesonNuclear Experiment010306 general physicsPhysics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyObservableHERAQCD PhenomenologyHigh Energy Physics - PhenomenologyPhase spaceHigh Energy Physics::Experiment
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Measuring the top energy asymmetry at the LHC: QCD and SMEFT interpretations

2020

The energy asymmetry in top-antitop-jet production is an observable of the top charge asymmetry designed for the LHC. We perform a realistic analysis in the boosted kinematic regime, including effects of the parton shower, hadronization and expected experimental uncertainties. Our predictions at particle level show that the energy asymmetry in the Standard Model can be measured with a significance of $3\sigma$ during Run 3, and with more than $5\sigma$ significance at the HL-LHC. Beyond the Standard Model the energy asymmetry is a sensitive probe of new physics with couplings to top quarks. In the framework of the Standard Model Effective Field Theory, we show that the sensitivity of the en…

Nuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard Modelmedia_common.quotation_subjectFOS: Physical sciences01 natural sciences7. Clean energyAsymmetryStandard ModelHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Hadron-Hadron scattering (experiments)0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsParton showermedia_commonParticle Physics - PhenomenologyPhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicshep-exHigh Energy Physics::Phenomenologyhep-phQCDHadronizationHigh Energy Physics - PhenomenologyTop physicsBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentParticle Physics - Experiment
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Consistent searches for SMEFT effects in non-resonant dijet events

2018

We investigate the bounds which can be placed on generic new-physics contributions to dijet production at the LHC using the framework of the Standard Model Effective Field Theory, deriving the first consistently-treated EFT bounds from non-resonant high-energy data. We recast an analysis searching for quark compositeness, equivalent to treating the SM with one higher-dimensional operator as a complete UV model. In order to reach consistent, model-independent EFT conclusions, it is necessary to truncate the EFT effects consistently at order $1/\Lambda^2$ and to include the possibility of multiple operators simultaneously contributing to the observables, neither of which has been done in prev…

Nuclear and High Energy PhysicsParticle physicsTevatronFOS: Physical sciencesParameter space01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Perturbative QCD0103 physical sciencesEffective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsLinear combinationPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyEffective Field TheoriesTechnicolor and Composite ModelsObservableWeinberg angleHigh Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798Journal of High Energy Physics
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Top-quark production in proton–nucleus and nucleus–nucleus collisions at LHC energies and beyond

2015

Single and pair top-quark production in proton-lead (p-Pb) and lead-lead (Pb-Pb) collisions at the CERN Large Hadron Collider (LHC) and future circular collider (FCC) energies, are studied with next-to-leading-order perturbative QCD calculations including nuclear parton distribution functions. At the LHC, the pair-production cross sections amount to sigma(t-tbar) = 3.4 mub in Pb-Pb at sqrt(s) = 5.5 TeV, and sigma(t-tbar) = 60 nb in p-Pb at sqrt(s) = 8.8 TeV. At the FCC energies of sqrt(s) = 39 and 63 TeV, the same cross sections are factors of 90 and 55 times larger respectively. In the leptonic final-state t-tbar --> W+b W-bbar --> b bbar l+l- nu+nu-, after typical acceptance and eff…

Nuclear and High Energy PhysicsParticle physicsTop quarkNuclear TheoryProtontop-quark productionFOS: Physical sciencesParton114 Physical sciences7. Clean energyFuture Circular ColliderHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CHANNELPAIRNuclear Experiment (nucl-ex)LEPTONNuclear ExperimentNuclear ExperimentParticle Physics - PhenomenologyPhysicsPP COLLISIONSLarge Hadron Colliderta114ROOT-S=7 TEVp–Pb collisionsHigh Energy Physics::PhenomenologyPerturbative QCDBOSONATLASPRODUCTION CROSS-SECTIONFINAL-STATESlcsh:QC1-999GluonHigh Energy Physics - PhenomenologyPb–Pb collisionsJETSHigh Energy Physics::Experimentlcsh:PhysicsLeptonPhysics Letters B
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Glueball enhancement by color deconfinement

2007

5 pages, 4 figures.-- PACS nrs.: 14.80.-j; 24.80.+y; 25.75.Nq.-- ISI Article Identifier: 000245333000063.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0609219

Nuclear and High Energy PhysicsParticle physics[PACS] Nuclear tests of fundamental interactions and symmetriesNuclear Theory[PACS] Quark deconfinement quark-gluon plasma production and phase transitions in heavy-ion collisionsHigh Energy Physics::LatticeFOS: Physical sciencesDeconfinementQuantum chromodynamics (QCD)Nuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Color confinementNuclear ExperimentNuclear theoryQuantum chromodynamicsPhysicsQuark confinementGlueball[PACS] Other particles (including hypothetical)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyColor modelHeavy ion-nucleus reactions
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The Deuteron Spin-dependent Structure Function g1(d) and its First Moment

2007

We present a measurement of the deuteron spin-dependent structure function g1d based on the data collected by the COMPASS experiment at CERN during the years 2002-2004. The data provide an accurate evaluation for Gamma_1^d, the first moment of g1d(x), and for the matrix element of the singlet axial current, a0. The results of QCD fits in the next to leading order (NLO) on all g1 deep inelastic scattering data are also presented. They provide two solutions with the gluon spin distribution function Delta G positive or negative, which describe the data equally well. In both cases, at Q^2 = 3 (GeV/c)^2 the first moment of Delta G is found to be of the order of 0.2 - 0.3 in absolute value.

Nuclear and High Energy PhysicsParticle physicsg(1)FOS: Physical sciencesAbsolute valuespinspin structure function g101 natural sciencesCOMPASSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)polarised deep inelastic scatteringdeep inelastic scatteringstructure function0103 physical sciencesCOMPASS experimentA(1)polarised deep inelastic scattering; COMPASS; spin structure function g1; QCD analysisSinglet state010306 general physicsSpin-½Quantum chromodynamicsPhysics010308 nuclear & particles physicsDeep inelastic scatteringGluonQCD analysisDistribution functionHigh Energy Physics::ExperimentParticle Physics - Experiment
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Jet transverse fragmentation momentum from h–h correlations in pp and p–Pb collisions

2016

QCD color coherence phenomena, like angular ordering, can be studied by looking at jet fragmentation. As the jet is fragmenting, it is expected to go through two different phases. First, there is QCD branching that is calculable in perturbative QCD. Next, the produced partons hadronize in a non-perturbative way later in a hadronization process. The jet fragmentation can be studied using the method of two particle correlations. A useful observable is the jet transverse fragmentation momentum $j_{\mathrm{T}}$, which describes the angular width of the jet. In this contribution, a differential study will be presented in which separate $j_{\mathrm{T}}$ components for branching and hadronization …

Nuclear and High Energy PhysicsParticle physicsp–PbFOS: Physical sciencesmomentumPartonppnucl-ex01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)ALICEjetfragmentationbranching0103 physical sciencesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)showeringNuclear Experiment010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsta114hep-ex010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPerturbative QCDObservableNuclear matterQCDHadronizationtransverseTransverse planeHigh Energy Physics::ExperimenthadronizationParticle Physics - ExperimentCoherence (physics)Nuclear and Particle Physics Proceedings
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Pion-photon transition distribution amplitudes in the Nambu-Jona-Lasinio model

2007

12 pages, 6 figures.-- PACS nrs.: 13.60.-r; 11.10.St; 12.38.Lg; 24.10.Jv.-- ISI Article Identifier: 000251327200049.-- ArXiv pre-print available at: http://arxiv.org/abs/0707.3366

Nuclear and High Energy PhysicsPhotonBethe–Salpeter equationHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciences[PACS] Relativistic models of nucleiPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelBound stateVirtual Compton-scatteringCovariant transformation[PACS] Photon and charged-lepton interactions with hadrons[PACS] Bound and unstable statesMathematical physicsQuantum chromodynamicsPhysicsHigh Energy Physics::PhenomenologyGeneralized Parton distributions[PACS] Bound and unstable states; Bethe-Salpeter equations[PACS] Other nonperturbative calculations in QCDHigh Energy Physics - PhenomenologyAmplitudeQuantum electrodynamicsBethe-Salpeter equationsFísica nuclear
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Gluon mass generation in the massless bound-state formalism

2013

We present a detailed, all-order study of gluon mass generation within the massless bound-state formalism, which constitutes the general framework for the systematic implementation of the Schwinger mechanism in non-Abelian gauge theories. The main ingredient of this formalism is the dynamical formation of bound states with vanishing mass, which give rise to effective vertices containing massless poles; these latter vertices, in turn, trigger the Schwinger mechanism, and allow for the gauge-invariant generation of an effective gluon mass. This particular approach has the conceptual advantage of relating the gluon mass directly to quantities that are intrinsic to the bound-state formation its…

Nuclear and High Energy PhysicsRenormalizationBethe–Salpeter equationHigh Energy Physics::LatticeBackground field methodFOS: Physical sciencesPinch techniqueRenormalizationTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeGauge symmetriesQuantum mechanicsGauge theory3-gluon vertexPhysicsBackground field methodDynamical symmetry breakingGlueballsPhysicsHigh Energy Physics - Lattice (hep-lat)Mass generationInvarianceHigh Energy Physics::PhenomenologyPropagatorQCDGluonMassless particleHigh Energy Physics - PhenomenologyFísica nuclear
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