Strangeness contributions to nucleon form factors
arXiv:nucl-th/0609014 · doi:10.1140/epja/i2006-10409-9
Abstract
We review a recent theoretical determination of the strange quark content of the electromagnetic form factors of the nucleon. These are compared with a global analysis of current experimental measurements in parity-violating electron scattering.
5 pages, 6 figures; Talk presented at the International Workshop "From Parity Violation to Hadronic Structure and more...", Milos, Greece, May 16-20, 2006
References in corpus (24)
- Big Bang Nucleosynthesis (in "The Review of Particle Properties" 2004)
- Strange Quark Contributions to Parity-Violating Asymmetries in the Forward G0 Electron-Proton Scattering Experiment
- Practical all-to-all propagators for lattice QCD
- The Strange Quark Contribution to the Proton's Magnetic Moment
- Physical Nucleon Properties from Lattice QCD
- Measurement of the Proton's Neutral Weak Magnetic Form Factor
- The nucleon axial charge in full lattice QCD
- Precise determination of the strangeness magnetic moment of the nucleon
- Constraints on the Nucleon Strange Form Factors at Q^2 ~ 0.1 GeV^2
- Chiral Analysis of Quenched Baryon Masses
- Convergence of chiral effective field theory
- The Nucleon Anapole Moment and Parity-Violating ep Scattering
- Extracting nucleon strange and anapole form factors from world data
- Lattice Calculation of the Strangeness Magnetic Moment of the Nucleon
- Strange Electric Form Factor of the Proton
- The nucleon electromagnetic form factors from Lattice QCD
- QCD Equalities for Baryon Current Matrix Elements
- Leading Quenching Effects in the Proton Magnetic Moment
- A Lattice QCD Analysis of the Strangeness Magnetic Moment of the Nucleon
- Chiral Symmetry and the Intrinsic Structure of the Nucleon
- In Search of the Chiral Regime
- The Nucleon Anapole Form Factor in Chiral Perturbation Theory to Sub-leading Order
- Flavour singlet physics in lattice QCD with background fields
- Systematic uncertainties in the precise determination of the strangeness magnetic moment of the nucleon