Search results for "53"

showing 10 items of 2908 documents

Measurement of the cross section for hard exclusive π0 muoproduction on the proton

2020

Physics letters / B B805, 135454 (2020). doi:10.1016/j.physletb.2020.135454

Quantum chromodynamics; Muoproduction; Hard exclusive meson production; Generalised Parton Distributions; COMPASSPhotongeneralized parton distributionProtonPartonmeasured [cross section]01 natural sciencesCOMPASSGeneralised Parton DistributionPhoton polarization[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQuantum chromodynamicsPhysicsRange (particle radiation)Large Hadron ColliderCOMPASS; Generalised Parton Distributions; Hard exclusive meson production; Muoproduction; Quantum chromodynamicslcsh:QC1-999ddc:angular dependencebeam [muon]polarization [photon]Nuclear and High Energy Physicsexclusive reactionliquid: target [hydrogen]transverse [polarization]polarization: longitudinalinterferenceHard exclusive meson productionContext (language use)Muoproductionleptoproduction [pi0]530Nuclear physicspi0: leptoproductionGeneralised Parton Distributionshydrogen: liquid: target0103 physical sciencespolarization: transverseddc:530010306 general physicslongitudinal [polarization]010308 nuclear & particles physicsmuon: beamcross section: measuredphoton: polarizationHigh Energy Physics::Experimentlcsh:PhysicsQuantum chromodynamicsexperimental results
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Fabrication of a planar micro Penning trap and numerical investigations of versatile ion positioning protocols

2009

We describe a versatile planar Penning trap structure, which allows one to dynamically modify the trapping configuration almost arbitrarily. The trap consists of 37 hexagonal electrodes, each with a circumcircle diameter of 300 μm, fabricated in a gold-on-sapphire lithographic technique. Every hexagon can be addressed individually, thus shaping the electric potential. The fabrication of such a device with clean room methods is demonstrated. We illustrate the variability of the device by a detailed numerical simulation of a lateral and a vertical transport and simulate trapping in racetrack and artificial crystal configurations. The trap may be used for ions or electrons, as a versatile cont…

Quantum opticsQuantum PhysicsFabricationMaterials sciencebusiness.industryAtomic Physics (physics.atom-ph)DDC 530 / PhysicsGeneral Physics and AstronomyPhysics::OpticsFOS: Physical sciencesElectronPenning trapIonenfallePhysics - Atomic PhysicsTrap (computing)PlanarOptoelectronicsTrapped ionsddc:530Electric potentialPhysics::Atomic PhysicsQuantum informationbusinessQuantum Physics (quant-ph)
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Two-Loop Planar Corrections to Heavy-Quark Pair Production in the Quark-Antiquark Channel

2009

We evaluate the planar two-loop QCD diagrams contributing to the leading color coefficient of the heavy-quark pair production cross section, in the quark-antiquark annihilation channel. We obtain the leading color coefficient in an analytic form, in terms of one- and two-dimensional harmonic polylogarithms of maximal weight 4. The result is valid for arbitrary values of the Mandelstam invariants s and t, and of the heavy-quark mass m. Our findings agree with previous analytic results in the small-mass limit and numerical results for the exact amplitude.

QuarkNuclear and High Energy PhysicsParticle physics530 PhysicsHigh Energy Physics::LatticeFOS: Physical sciencesHarmonic (mathematics)10192 Physics Institute01 natural sciencesCross section (physics)High Energy Physics - Phenomenology (hep-ph)NLO Computations0103 physical sciencesHeavy Quark PhysicsLimit (mathematics)3106 Nuclear and High Energy Physics010306 general physicsPhysicsQuantum chromodynamicsAnnihilation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyPair productionAmplitude[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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Light hadrons from lattice QCD with light (u, d), strange and charm dynamical quarks

2010

We present results of lattice QCD simulations with mass-degenerate up and down and mass-split strange and charm (N_f = 2+1+1) dynamical quarks using Wilson twisted mass fermions at maximal twist. The tuning of the strange and charm quark masses is performed at two values of the lattice spacing a~0.078 fm and a~0.086 fm with lattice sizes ranging from L~1.9 fm to L~2.8 fm. We measure with high statistical precision the light pseudoscalar mass m_PS and decay constant f_PS in a range 270 < m_PS < 510 MeV and determine the low energy parameters f_0, l_3 and l_4 of SU(2) chiral perturbation theory. We use the two values of the lattice spacing, several lattice sizes as well as different values of…

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHigh Energy Physics::LatticeHadronCharm quarkFOS: Physical sciencesLattice QCD2 FLAVORS01 natural sciencesCHIRAL PERTURBATION-THEORYCharm quarkLattice constantHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeTWISTED MASS FERMIONSChiral perturbation theoryWILSON QUARKS0103 physical sciencesddc:530ALGORITHM010306 general physicsSCALEPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaFermionLattice QCDSIMULATIONSPseudoscalarHigh Energy Physics - PhenomenologyLattice gauge theoryChiral LagrangiansYANG-MILLS THEORYHigh Energy Physics::ExperimentPHASE-STRUCTUREMESONChiral lagrangiansLight hadronsJournal of High Energy Physics
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Dynamical twisted mass fermions with light quarks

2007

We present results of dynamical simulations with 2 flavours of degenerate Wilson twisted mass quarks at maximal twist in the range of pseudo scalar masses from 300 to 550 MeV. The simulations are performed at one value of the lattice spacing a \lesssim 0.1 fm. In order to have O(a) improvement and aiming at small residual cutoff effects, the theory is tuned to maximal twist by requiring the vanishing of the untwisted quark mass. Precise results for the pseudo scalar decay constant and the pseudo scalar mass are confronted with chiral perturbation theory predictions and the low energy constants F, \bar{l}_3 and \bar{l}_4 are evaluated with small statistical errors.

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMONTE-CARLO ALGORITHMCHIRAL PERTURBATION-THEORY; MONTE-CARLO ALGORITHM; GROSS-NEVEU MODEL; YANG-MILLS THEORY; LATTICE QCD; PHASE-STRUCTURE; WILSON QUARKS; HMC ALGORITHM; GAUGE ACTIONS; 2 FLAVORSHigh Energy Physics::LatticeLattice field theoryScalar (mathematics)FOS: Physical sciences2 FLAVORSGAUGE ACTIONS01 natural sciences7. Clean energyCHIRAL PERTURBATION-THEORYLATTICE QCDHigh Energy Physics - LatticeGross–Neveu modelWILSON QUARKS0103 physical sciencesddc:530Twist010306 general physicsPhysics010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyFísicaGROSS-NEVEU MODELFermionLattice QCDSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciYANG-MILLS THEORYPHASE-STRUCTUREHMC ALGORITHM
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Dirac and Pauli form factors from lattice QCD

2011

We present a comprehensive analysis of the electromagnetic form factors of the nucleon from a lattice simulation with two flavors of dynamical O(a)-improved Wilson fermions. A key feature of our calculation is that we make use of an extensive ensemble of lattice gauge field configurations with four different lattice spacings, multiple volumes, and pion masses down to m_\pi ~ 180 MeV. We find that by employing Kelly-inspired parametrizations for the Q^2-dependence of the form factors, we are able to obtain stable fits over our complete ensemble. Dirac and Pauli radii and the anomalous magnetic moments of the nucleon are extracted and results at light quark masses provide evidence for chiral …

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice field theoryNuclear TheoryFOS: Physical sciences7. Clean energy01 natural sciencessymbols.namesakePauli exclusion principleHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Quantum field theory010306 general physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FermionLattice QCDJHigh Energy Physics - PhenomenologysymbolsNucleon
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Quark and gluon distributions and $\alpha_{s}$ from nucleon structure functions at low $x$

1993

Abstract The Q2 dependence of the structure functions F2p and F2d recently measured by the NMC is compared with the predictions of perturbative QCD at next-to-leading order. Good agreement is observed, leading to accurate determinations of the quark and gluon distributions in the range 0.008 ⩽ × ⩽ 0.5. The strong coupling constant is measured from the low x data; the result agrees with previous determinations.

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::Latticedeep inelastic scattering: muon deuteronmuon deuteron: deep inelastic scatteringPARTON DENSITIESJet (particle physics)530CROSS-SECTIONSNuclear physicsnumerical calculations: interpretation of experimentsstrong interaction: coupling constant90: 280 GeVDEEP INELASTIC-SCATTERING; LEADING ORDER; QUANTUM CHROMODYNAMICS; PERTURBATION-THEORY; PARTON DENSITIES; CROSS-SECTIONS; FREEDOM; MSBAR; JET; NMCdeep inelastic scattering: muon pp: structure functionNMCCoupling constantQuantum chromodynamicsPhysicsQUANTUM CHROMODYNAMICSLEADING ORDERHigh Energy Physics::Phenomenologydeuteron: structure functiongluon: momentum spectrumperturbation theory: higher-orderPerturbative QCDDeep inelastic scatteringquark: momentum spectrumFREEDOMGluondependence: momentum transferJETMSBARmuon p: deep inelastic scatteringPERTURBATION-THEORYDEEP INELASTIC-SCATTERINGHigh Energy Physics::Experimentcoupling constant: strong interactionNucleonParticle Physics - Experiment
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Nucleon structure from Lattice QCD using a nearly physical pion mass

2014

We report the first Lattice QCD calculation using the almost physical pion mass mpi=149 MeV that agrees with experiment for four fundamental isovector observables characterizing the gross structure of the nucleon: the Dirac and Pauli radii, the magnetic moment, and the quark momentum fraction. The key to this success is the combination of using a nearly physical pion mass and excluding the contributions of excited states. An analogous calculation of the nucleon axial charge governing beta decay has inconsistencies indicating a source of bias at low pion masses not present for the other observables and yields a result that disagrees with experiment.

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryLattice field theoryFOS: Physical sciencesLattice QCDNuclear Theory (nucl-th)Nucleon structureNuclear physicssymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Pauli exclusion principlePionddc:530Nuclear ExperimentPhysicsQuantum chromodynamicsIsovectorHigh Energy Physics - Lattice (hep-lat)Form factorsLattice QCDHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentNucleonPhysics Letters B
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The Cabibbo angle as a universal seed for quark and lepton mixings

2015

A model-independent ansatz to describe lepton and quark mixing in a unified way is suggested based upon the Cabibbo angle. In our framework neutrinos mix in a "Bi-Large" fashion, while the charged leptons mix as the "down-type" quarks do. In addition to the standard Wolfenstein parameters (lambda, A) two other free parameters are needed to specify the physical lepton mixing matrix. Through this simple assumption one makes specific predictions for the atmospheric angle as well as leptonic CP violation in good agreement with current observations.

QuarkNuclear and High Energy PhysicsParticle physicsPMNS matrixPhysics beyond the Standard ModelPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)ddc:530Mixing (physics)PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaBi-Large mixinglcsh:QC1-999High Energy Physics - PhenomenologyCKM matrixCabibbo angleCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino mixingWolfenstein parameterlcsh:PhysicsLepton
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Parton distributions and lattice QCD calculations: A community white paper

2018

Progress in particle and nuclear physics 100, 107 - 160 (2018). doi:10.1016/j.ppnp.2018.01.007

QuarkNuclear and High Energy PhysicsParticle physicsquark: distribution functiondata analysis methodHigh Energy Physics::LatticeLattice field theoryhadron: spinFOS: Physical sciencesparton: distribution functionPartonLattice QCD01 natural sciences530hard scatteringHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)benchmarkFactorization0103 physical sciencesquantum chromodynamicsquantum chromodynamics: factorizationddc:530010306 general physicsGlobal QCD fitsQuantum chromodynamicsPhysicspolarizationgluon: distribution function010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]High Energy Physics - Lattice (hep-lat)High Energy Physics::Phenomenologylattice field theory[ PHYS.HLAT ] Physics [physics]/High Energy Physics - Lattice [hep-lat]ObservableLattice QCDGluonHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentUnpolarized/polarized parton distribution functions (PDFs)
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