Search results for "Chromodynamics"

showing 10 items of 1030 documents

A strategy to study the role of the charm quark in explaining the Delta{I}=1/2 rule

2004

We present a strategy designed to separate several possible origins of the well-known enhancement of the Delta{I}=1/2 amplitude in non-leptonic kaon decays. In particular, we seek to disentangle the contribution of physics at the typical QCD scale (soft-gluon exchange) from the effects at the scale of the charm quark mass. This is achieved by considering QCD with an unphysically light charm quark, so that the theory possesses an approximate SU(4)_L x SU(4)_R chiral symmetry. By computing the relevant operator matrix elements and monitoring their values as the charm quark mass departs from the SU(4)-symmetric situation, the role of the charm quark can be assessed. We study the influence of t…

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeLattice (group)FOS: Physical sciencesScale (descriptive set theory)weak decaysCharm quarkHigh Energy Physics - Phenomenology (hep-ph)lattice QCDHigh Energy Physics - Latticefield theory gauge theory lattice kaon decayskaon physicschiral lagrangiansLimit (mathematics)Quantum chromodynamicsPhysicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFIS/02 - FISICA TEORICA MODELLI E METODI MATEMATICIHigh Energy Physics - PhenomenologyAmplitudeOperator matrixHigh Energy Physics::Experiment
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Chiral Symmetry of Baryons

2001

We study chiral symmetry aspects of the positive and negative parity baryons by identifying them with linear representations of the chiral group $SU(N_{f}) \otimes SU(N_{f})$. It is shown that there are two distinctive schemes: naive and mirror assignments. We construct linear sigma models for baryons in the two assignments and examine their physical implications. Then we investigate properties of the naive and mirror nucleons microscopically by using QCD interpolating fields. Finally, we propose experiments to distinguish the two chiral assignments for the nucleon.

Nuclear and High Energy PhysicsParticle physicsChiral perturbation theoryPhysics and Astronomy (miscellaneous)Spontaneous symmetry breakingmedia_common.quotation_subjectHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesAsymmetryGroup representationPionHigh Energy Physics - Phenomenology (hep-ph)Nambu–Jona-Lasinio modelNuclear Experimentmedia_commonChiral anomalyQuantum chromodynamicsPhysicsChiral symmetryHigh Energy Physics::PhenomenologySigmaParity (physics)BaryonHigh Energy Physics - PhenomenologyChiral symmetry breakingNucleon
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Measurement of $ZZ$ production in $pp$ collisions at $\sqrt{s}=7$ TeV and limits on anomalous $ZZZ$ and $ZZ\gamma$ couplings with the ATLAS detector

2013

Journal of High Energy Physics 2013.3 (2013): 128 reproduced by permission of Scuola Internazionale Superiore di Studi Avanzati (SISSA)

Nuclear and High Energy PhysicsParticle physicsCiências Naturais::Ciências FísicasPhysics::Instrumentation and Detectors:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2Hadron-hadron scattering01 natural sciences7. Clean energy530High Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsQCCiencias ExactasBosonPhysicsQuantum chromodynamicsGauge bosonMuonLarge Hadron ColliderScience & TechnologyHadron-Hadron ScatteringATLAS detector010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleATLAS experimentHigh Energy Physics::PhenomenologyFísicaNEW PHYSICSATLASZZ productionsZ BOSONHADRON-HADRON COLLISIONSPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::ExperimentLHCNeutrinoParticle Physics - Experiment
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QCD Induced Di-boson Production in Association with Two Jets at NLO QCD

2016

We discuss results for di-boson plus two jets production processes at the LHC at NLO QCD. Issues related to the scale choice are reviewed. We focus on the distributions of the invariant mass and rapidity separation of the two hardest jets and show, for $W^\pm \gamma jj$ and $Z\gamma jj$ production, how the contribution from the radiative decays of the massive gauge bosons can be significantly reduced.

Nuclear and High Energy PhysicsParticle physicsCollider physicsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRadiative transferInvariant massRapidity010306 general physicsBosonmulti-boson productionQuantum chromodynamicsPhysicsGauge bosonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyCollider PhysicsHigh Energy Physics::Experimentmulti-leg at NLO QCDNuclear and Particle Physics Proceedings
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The pion transition form factor and the pion distribution amplitude

2010

Recent BaBar data on the pion transition form factor, whose Q(2)-dependence is much steeper then predicted by asymptotic Quantum Chromodynamics (QCD), have caused a renewed interest in its theoretical description. We present here a formalism based on a model-independent description for low photon virtuality and a high photon virtuality description based on QCD, which match at a scale Q(0). The high photon virtuality description incorporates a flat pion distribution amplitude, phi(x) = 1, at the matching scale Q(0) and QCD evolution from Q(0) to Q > Q(0). The flat pion distribution is connected, through soft pion theorems and chiral symmetry, to the pion valence parton distribution at the sa…

Nuclear and High Energy PhysicsParticle physicsDistribution (number theory)Scale (ratio)High Energy Physics::LatticeFOS: Physical sciencesPartonAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesPartícules (Física nuclear)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesTwist010306 general physicsNuclear ExperimentPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyForm factor (quantum field theory)High Energy Physics - PhenomenologyAmplitudeFísica nuclearHigh Energy Physics::Experiment
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Power Corrections to Event Shapes with Mass-Dependent Operators

2013

We introduce an operator depending on the "transverse velocity'' r that describes the effect of hadron masses on the leading 1/Q power correction to event-shape observables. Here, Q is the scale of the hard collision. This work builds on earlier studies of mass effects by Salam and Wicke [J. High Energy Phys. 05 (2001) 061] and of operators by Lee and Sterman [Phys. Rev. D 75, 014022 (2007)]. Despite the fact that different event shapes have different hadron mass dependence, we provide a simple method to identify universality classes of event shapes whose power corrections depend on a common nonperturbative parameter. We also develop an operator basis to show that at a fixed value of Q, the…

Nuclear and High Energy PhysicsParticle physicsExponentiationFOS: Physical sciences01 natural sciencesOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesRenormalonsResummationFactorization010306 general physicsMathematical physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsMultiplicative functionObservableUniversality (dynamical systems)HadronizationHigh Energy Physics - PhenomenologyQCD correctionsE&E-annihilationDistributionsResummationJet cross-sectionsQuantum chromodynamics
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Evaluating the double parton scattering contribution to Mueller-Navelet jets production at the LHC

2015

We propose a model to study the importance of double parton scattering (DPS) in Mueller-Navelet jets production at the LHC which is consistent with the BFKL framework used to compute the single parton scattering contribution to this process. We study this model in kinematics corresponding to existing and possible future measurements at the LHC and estimate the importance of this DPS contribution on relevant observables for this process, namely the cross section and the azimuthal correlation of the jets.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesParton01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesRapidity010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyObservableHigh Energy Physics - Phenomenologydouble parton scatteringHigh Energy Physics::ExperimentLHCPhoton scattering
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A QCD analysis of LHCb D-meson data in p plus Pb collisions

2020

We scrutinize the recent LHCb data for D$^0$-meson production in p+Pb collisions within a next-to-leading order QCD framework. Our calculations are performed in the SACOT-$m_{\rm T}$ variant of the general-mass variable-flavour-number scheme (GM-VFNS), which has previously been shown to provide a realistic description of the LHC p+p data. Using the EPPS16 and nCTEQ15 nuclear parton distribution functions (PDFs) we show that a very good agreement is obtained also in the p+Pb case both for cross sections and nuclear modification ratios in the wide rapidity range covered by the LHCb data. Encouraged by the good correspondence, we quantify the impact of these data on the nuclear PDFs by the Hes…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesPartonhiukkasfysiikka01 natural sciences114 Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesD mesonRapiditylcsh:Nuclear and particle physics. Atomic energy. Radioactivityheavy ion phenomenology010306 general physicsParton showerNuclear ExperimentParticle Physics - PhenomenologyPhysicsQuantum chromodynamicsLarge Hadron Collider010308 nuclear & particles physicshep-phHeavy Ion PhenomenologyGluonHigh Energy Physics - Phenomenologylcsh:QC770-798High Energy Physics::Experiment
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Fingerprints of heavy scales in electroweak effective Lagrangians

2017

The couplings of the electroweak effective theory contain information on the heavy-mass scales which are no-longer present in the low-energy Lagrangian. We build a general effective Lagrangian, implementing the electroweak chiral symmetry breaking $SU(2)_L\otimes SU(2)_R\to SU(2)_{L+R}$, which couples the known particle fields to heavier states with bosonic quantum numbers $J^P=0^\pm$ and $1^\pm$. We consider colour-singlet heavy fields that are in singlet or triplet representations of the electroweak group. Integrating out these heavy scales, we analyze the pattern of low-energy couplings among the light fields which are generated by the massive states. We adopt a generic non-linear realiz…

Nuclear and High Energy PhysicsParticle physicsFísica-Modelos matemáticosHiggs PhysicsFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryFísica matemáticaPartículas (Física nuclear)lcsh:Nuclear and particle physics. Atomic energy. RadioactivityElectromagnetismoSymmetry breakingSinglet state010306 general physicsParticles (Nuclear physics)Huellas dactilares.PhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionCromodinámica cuántica.Technicolor and Composite ModelsQuantum numberLagrangian functions.High Energy Physics - PhenomenologyFingerprints.Simetría (Física)Beyond Standard ModelChiral LagrangiansQuantum chromodynamics.Higgs bosonlcsh:QC770-798Chiral symmetry breakingSymmetry (Physics)Lagrange Funciones de.Journal of High Energy Physics
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Measurement of theZZproduction cross section inpp¯collisions ats=1.96  TeV

2016

The ZZ production cross section in proton-proton collisions at 13 TeV center-of-mass energy is measured using 3.2 fb⁻¹ of data recorded with the ATLAS detector at the Large Hadron Collider. The considered Z boson candidates decay to an electron or muon pair of mass 66-116 GeV. The cross section is measured in a fiducial phase space reflecting the detector acceptance. It is also extrapolated to a total phase space for Z bosons in the same mass range and of all decay modes, giving 16.7 +2.2 −2.0 (stat.) +0.9 −0.7 (syst.) +1.0 −0.7 (lumi.) pb. The results agree with standard model predictions.

Nuclear and High Energy PhysicsParticle physicsGeneral Physics and AstronomyElectron7. Clean energy01 natural sciencesStandard ModelNuclear physicsCross section (physics)0103 physical sciencesNuclear Experiment010306 general physicsBosonQuantum chromodynamicsPhysicsMuonLarge Hadron Collider010308 nuclear & particles physicsDetectorHigh Energy Physics::PhenomenologySigmaPhase spaceHigh Energy Physics::ExperimentProduction (computer science)LeptonBar (unit)Physical Review D
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