0000000000190317

AUTHOR

John W. Negele

showing 13 related works from this author

Initial nucleon structure results with chiral quarks at the physical point

2014

We report initial nucleon structure results computed on lattices with 2+1 dynamical M\"obius domain wall fermions at the physical point generated by the RBC and UKQCD collaborations. At this stage, we evaluate only connected quark contributions. In particular, we discuss the nucleon vector and axial-vector form factors, nucleon axial charge and the isovector quark momentum fraction. From currently available statistics, we estimate the stochastic accuracy of the determination of $g_A$ and $_{u-d}$ to be around 10%, and we expect to reduce that to 5% within the next year. To reduce the computational cost of our calculations, we extensively use acceleration techniques such as low-eigenmode def…

PhysicsNuclear physicsPhysical pointHigh Energy Physics - LatticeHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesddc:530National laboratory
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Nucleon form factors with light Wilson quarks

2014

Jeremy Green∗,a† Michael Engelhardt,b Stefan Krieg,cd Stefan Meinel,a John Negele,a Andrew Pochinskya and Sergey Syritsyne aCenter for Theoretical Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA bDepartment of Physics, New Mexico State University, Las Cruces, New Mexico 88003, USA cBergische Universitat Wuppertal, D-42119 Wuppertal, Germany dIAS, Julich Supercomputing Centre, Forschungszentrum Julich, D-52425 Julich, Germany eLawrence Berkeley National Laboratory, Berkeley, California 94720, USA E-mail: green@kph.uni-mainz.de, engel@nmsu.edu, s.krieg@fz-juelich.de, smeinel@mit.edu, negele@mit.edu, avp@mit.edu,

Nuclear physicsPhysicsQuarkParticle physicsNucleonNational laboratoryProceedings of 31st International Symposium on Lattice Field Theory LATTICE 2013 — PoS(LATTICE 2013)
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TRANSVERSE MOMENTUM-DEPENDENT PARTON DISTRIBUTIONS FROM LATTICE QCD

2012

Starting from a definition of transverse momentum-dependent parton distributions for semi-inclusive deep inelastic scattering and the Drell-Yan process, given in terms of matrix elements of a quark bilocal operator containing a staple-shaped Wilson connection, a scheme to determine such observables in lattice QCD is developed and explored. Parametrizing the aforementioned matrix elements in terms of invariant amplitudes permits a simple transformation of the problem to a Lorentz frame suited for the lattice calculation. Results for the Sivers and Boer-Mulders transverse momentum shifts are presented, focusing in particular on their dependence on the staple extent and the Collins-Soper evol…

QuarkPhysicsParticle physicsHigh Energy Physics::LatticeLorentz transformationHigh Energy Physics::PhenomenologyObservablePartonLattice QCDDeep inelastic scatteringTransverse planesymbols.namesakeLattice (order)symbolsHigh Energy Physics::ExperimentInternational Journal of Modern Physics: Conference Series
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Lattice QCD calculations of transverse momentum-dependent parton distributions (TMDs)

2016

An ongoing program of evaluating TMD observables within Lattice QCD is reviewed, summarizing recent progress with respect to several challenges faced by such calculations. These lattice calculations are based on a definition of TMDs through hadronic matrix elements of quark bilocal operators containing staple-shaped gauge connections. A parametrization of the matrix elements in terms of invariant amplitudes serves to cast them in the Lorentz frame preferred for a lattice calculation. Data on the naively T-odd Sivers and Boer-Mulders effects as well as the transversity TMD are presented.

QuarkPhysicsParticle physics010308 nuclear & particles physicsPhysicsQC1-999High Energy Physics::LatticeLorentz transformationHadronPartonObservableLattice QCD01 natural sciencesNuclear physicssymbols.namesakeAmplitudeLattice (order)0103 physical sciencessymbolsddc:530010306 general physics
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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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I=1/2 S -wave and P -wave Kπ scattering and the κ and K* resonances from lattice QCD

2020

We present a lattice-QCD determination of the elastic isospin-$1/2$ $S$-wave and $P$-wave $K\ensuremath{\pi}$ scattering amplitudes as a function of the center-of-mass energy using L\"uscher's method. We perform global fits of $K$-matrix parametrizations to the finite-volume energy spectra for all irreducible representations with total momenta up to $\sqrt{3}\frac{2\ensuremath{\pi}}{L}$; this includes irreducible representations (irreps) that mix the $S$- and $P$-waves. Several different parametrizations for the energy dependence of the $K$-matrix are considered. We also determine the positions of the nearest poles in the scattering amplitudes, which correspond to the broad $\ensuremath{\ka…

PhysicsParticle physics010308 nuclear & particles physicsScatteringResonanceLattice QCDFermion01 natural sciencesScattering amplitudePionIrreducible representation0103 physical sciencesNuclear Experiment010306 general physicsEnergy (signal processing)Physical Review D
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ππ and Kπ scattering amplitudes from lattice QCD

2020

PhysicsScattering amplitudeParticle physicsLattice QCDHadron Spectroscopy and Structure
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Quark transverse charge densities in the from lattice QCD

2009

Abstract We extend the formalism relating electromagnetic form factors to transverse quark charge densities in the light-front frame to the case of a spin-3/2 baryon and calculate these transverse densities for the Δ ( 1232 ) isobar using lattice QCD. The transverse charge densities for a transversely polarized spin-3/2 particle are characterized by monopole, dipole, quadrupole, and octupole patterns representing the structure beyond that of a pure point-like spin-3/2 particle. We present lattice QCD results for the Δ-isobar electromagnetic form factors for pion masses down to approximatively 350 MeV for three cases: quenched QCD, two-degenerate flavors of dynamical Wilson quarks, and three…

PhysicsQuantum chromodynamicsQuarkNuclear and High Energy PhysicsParticle physicsPoint particleHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryLattice field theoryCharge densityLattice QCDBaryonPionQuantum electrodynamicsHigh Energy Physics::ExperimentNuclear ExperimentNuclear Physics A
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Computing the nucleon Dirac radius directly at $Q^2=0$

2016

We describe a lattice approach for directly computing momentum derivatives of nucleon matrix elements using the Rome method, which we apply to obtain the isovector magnetic moment and Dirac radius. We present preliminary results calculated at the physical pion mass using a 2HEX-smeared Wilson-clover action. For removing the effects of excited-state contamination, the calculations were done at three source-sink separations and the summation method was used.

PhysicsPionIsovectorMagnetic momentHigh Energy Physics::LatticeLattice (order)Excited stateQuantum electrodynamicsNuclear TheoryGround stateNucleonProceedings of 34th annual International Symposium on Lattice Field Theory — PoS(LATTICE2016)
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Muonic Isotope Shifts in the Even Fe Nuclei

1975

Nuclear physicsPhysicsIsotopeHartree–Fock methodGeneral Physics and AstronomyNuclear binding energyAtomic physicsX ray spectraPhysical Review Letters
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P -wave nucleon-pion scattering amplitude in the Δ(1232) channel from lattice QCD

2021

We determine the $\mathrm{\ensuremath{\Delta}}(1232)$ resonance parameters using lattice QCD and the L\"uscher method. The resonance occurs in elastic pion-nucleon scattering with ${J}^{P}=3/{2}^{+}$ in the isospin $I=3/2$, $P$-wave channel. Our calculation is performed with ${N}_{f}=2+1$ flavors of clover fermions on a lattice with $L\ensuremath{\approx}2.8\text{ }\text{ }\mathrm{fm}$. The pion and nucleon masses are ${m}_{\ensuremath{\pi}}=255.4(1.6)\text{ }\text{ }\mathrm{MeV}$ and ${m}_{N}=1073(5)\text{ }\text{ }\mathrm{MeV}$, respectively, and the strong decay channel $\mathrm{\ensuremath{\Delta}}\ensuremath{\rightarrow}\ensuremath{\pi}N$ is found to be above the threshold. To thorough…

Physics010308 nuclear & particles physicsNuclear TheoryLattice (group)Lattice QCDCoupling (probability)01 natural sciencesScattering amplitudeIsospinIrreducible representation0103 physical sciences010306 general physicsNucleonEnergy (signal processing)Mathematical physicsPhysical Review D
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High-precision calculation of the strange nucleon electromagnetic form factors

2015

We report a direct lattice QCD calculation of the strange nucleon electromagnetic form factors $G_E^s$ and $G_M^s$ in the kinematic range $0 \leq Q^2 \lesssim 1.2\: {\rm GeV}^2$. For the first time, both $G_E^s$ and $G_M^s$ are shown to be nonzero with high significance. This work uses closer-to-physical lattice parameters than previous calculations, and achieves an unprecedented statistical precision by implementing a recently proposed variance reduction technique called hierarchical probing. We perform model-independent fits of the form factor shapes using the $z$-expansion and determine the strange electric and magnetic radii and magnetic moment. We compare our results to parity-violatin…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMagnetic momentNuclear Theory010308 nuclear & particles physicsScatteringLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDStrangeness01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeLattice (order)0103 physical sciencesddc:530010306 general physicsNucleonNuclear Experiment
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Lattice study of the Boer-Mulders transverse momentum distribution in the pion

2013

The Boer-Mulders transverse momentum-dependent parton distribution (TMD) characterizes polarized quark transverse momentum in an unpolarized hadron. Techniques previously developed for lattice calculations of nucleon TMDs are applied to the pion. These techniques are based on the evaluation of matrix elements of quark bilocal operators containing a staple-shaped Wilson connection. Results for the Boer-Mulders transverse momentum shift in the pion, obtained at a pion mass of $m_{\pi} = 518\, \mbox{MeV} $, are presented and compared to corresponding results in the nucleon.

PhysicsQuarkParticle physicsHigh Energy Physics::LatticeHadronHigh Energy Physics::PhenomenologyNuclear TheoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesPartonHigh Energy Physics - PhenomenologyTransverse planeHigh Energy Physics - LatticePionHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Transverse momentumHigh Energy Physics::ExperimentNucleonNuclear Experiment
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