643 research outputs found
Detection of plant stress through multispectral photography
There are no author-identified significant results in this report
Helicity Dependent and Independent Generalized Parton Distributions of the Nucleon in Lattice QCD
A complete description of the nucleon structure in terms of generalized
parton distributions (GPDs) at twist 2 level requires the
measurement/computation of the eight functions H, E, \tilde H, \tilde E, H_T,
E_T, \tilde H_T and \tilde E_T, all depending on the three variables x, \xi and
t. In this talk, we present and discuss our first steps in the framework of
lattice QCD towards this enormous task. Dynamical lattice QCD results for the
lowest three Mellin moments of the helicity dependent and independent GPDs are
shown in terms of their corresponding generalized form factors. Implications
for the transverse coordinate space structure of the nucleon as well as the
orbital angular momentum (OAM) contribution of quarks to the nucleon spin are
discussed in some detail.Comment: 5 pages, 5 figures, Talk presented by Ph.H. at Electron-Nucleus
Scattering VIII, Elba, Italy, June 21-25, 2004; typos corrected, minor change
in wording on p.4&
Transverse Structure of Nucleon Parton Distributions from Lattice QCD
This work presents the first calculation in lattice QCD of three moments of
spin-averaged and spin-polarized generalized parton distributions in the
proton. It is shown that the slope of the associated generalized form factors
decreases significantly as the moment increases, indicating that the transverse
size of the light-cone quark distribution decreases as the momentum fraction of
the struck parton increases.Comment: 4 pages, 1 figur
Quark Contributions to Nucleon Momentum and Spin from Domain Wall fermion calculations
We report contributions to the nucleon spin and momentum from light quarks
calculated using dynamical domain wall fermions with pion masses down to 300
MeV and fine lattice spacing a=0.084 fm. Albeit without disconnected diagrams,
we observe that spin and orbital angular momenta of both u and d quarks are
opposite, almost canceling in the case of the d quark, which agrees with
previous calculations using a mixed quark action. We also present the full
momentum dependence of n=2 generalized form factors showing little variation
with the pion mass.Comment: 7 pages, 5 figures, NT-LBNL-11-020, MIT-CTP-4323. Presented at the
29th International Symposium on Lattice Field Theory (Lattice 2011), Squaw
Valley, California, 10-16 Jul 201
Calculation of the nucleon axial charge in lattice QCD
Protons and neutrons have a rich structure in terms of their constituents,
the quarks and gluons. Understanding this structure requires solving Quantum
Chromodynamics (QCD). However QCD is extremely complicated, so we must
numerically solve the equations of QCD using a method known as lattice QCD.
Here we describe a typical lattice QCD calculation by examining our recent
computation of the nucleon axial charge.Comment: Prepared for Scientific Discovery through Advanced Computing (SciDAC
2006), Denver, Colorado, June 25-29 200
Nucleon structure in the chiral regime with domain wall fermions on an improved staggered sea
Moments of unpolarized, helicity, and transversity distributions,
electromagnetic form factors, and generalized form factors of the nucleon are
presented from a preliminary analysis of lattice results using pion masses down
to 359 MeV. The twist two matrix elements are calculated using a mixed action
of domain wall valence quarks and asqtad staggered sea quarks and are
renormalized perturbatively. Several observables are extrapolated to the
physical limit using chiral perturbation theory. Results are compared with
experimental moments of quark distributions and electromagnetic form factors
and phenomenologically determined generalized form factors, and the
implications on the transverse structure and spin content of the nucleon are
discussed.Comment: Talks of J.W. Negele and D.B. Renner at Lattice 200
Transverse momentum distributions inside the nucleon from lattice QCD
We study transverse momentum dependent parton distribution functions (TMDs) with
non-local operators in lattice QCD, using MILC/LHPC lattices. Results obtained with a simplified
operator geometry show visible dipole deformations of spin-dependent quark momentum densities.United States. Dept. of Energy (grant DE-FG02-94ER40818
Transverse momentum dependent quark densities from Lattice QCD
We study transverse momentum dependent parton distribution functions (TMDs) with nonâlocal operators in lattice QCD, using MILCâLHPC lattices. We discuss the basic concepts of the method, including renormalization of the gauge link. Results obtained with a simplified operator geometry show visible dipole deformations of spinâdependent quark momentum densities.United States. Dept. of Energy (grant DEFG02- 94ER40818
Nucleon Electromagnetic Form Factors from Lattice QCD using 2+1 Flavor Domain Wall Fermions on Fine Lattices and Chiral Perturbation Theory
We present a high-statistics calculation of nucleon electromagnetic form
factors in lattice QCD using domain wall quarks on fine lattices, to
attain a new level of precision in systematic and statistical errors. Our
calculations use lattices with lattice spacing a=0.084 fm for
pion masses of 297, 355, and 403 MeV, and we perform an overdetermined analysis
using on the order of 3600 to 7000 measurements to calculate nucleon electric
and magnetic form factors up to 1.05 GeV. Results are shown
to be consistent with those obtained using valence domain wall quarks with
improved staggered sea quarks, and using coarse domain wall lattices. We
determine the isovector Dirac radius , Pauli radius and
anomalous magnetic moment . We also determine connected contributions
to the corresponding isoscalar observables. We extrapolate these observables to
the physical pion mass using two different formulations of two-flavor chiral
effective field theory at one loop: the heavy baryon Small Scale Expansion
(SSE) and covariant baryon chiral perturbation theory. The isovector results
and the connected contributions to the isoscalar results are compared with
experiment, and the need for calculations at smaller pion masses is discussed.Comment: 44 pages, 40 figure
- âŠ