Finite-volume and partial quenching effects in the magnetic polarizability of the neutron
arXiv:1312.5781 · doi:10.1103/PhysRevD.89.054511
Abstract
There has been much progress in the experimental measurement of the electric and magnetic polarizabilities of the nucleon. Similarly, lattice QCD simulations have recently produced dynamical QCD results for the magnetic polarizability of the neutron approaching the chiral regime. In order to compare the lattice simulations with experiment, calculation of partial quenching and finite-volume effects is required prior to an extrapolation in quark mass to the physical point. These dependencies are described using chiral effective field theory. Corrections to the partial quenching effects associated with the sea-quark-loop electric charges are estimated by modelling corrections to the pion cloud. These are compared to the uncorrected lattice results. In addition, the behaviour of the finite-volume corrections as a function of pion mass is explored. Box sizes of approximately 7 fm are required to achieve a result within 5% of the infinite-volume result at the physical pion mass. A variety of extrapolations are shown at different box sizes, providing a benchmark to guide future lattice QCD calculations of the magnetic polarizabilities. A relatively precise value for the physical magnetic polarizability of the neutron is presented, beta_n = 1.93(11)stat(8)sys x 10^-4 fm^3, which is in agreement with current experimental results.
Published in Phys. Rev. D, 25 March 2014. Systematic error analysis updated
References in corpus (8)
- Using effective field theory to analyse low-energy Compton scattering data from protons and light nuclei
- Compton scattering from the proton in an effective field theory with explicit Delta degrees of freedom
- Electromagnetic and spin polarisabilities in lattice QCD
- Chiral extrapolation of nucleon magnetic form factors
- Chiral extrapolation of octet-baryon charge radii
- Magnetic moments of vector, axial, and tensor mesons in lattice QCD
- Strange magnetic form factor of nucleon in heavy baryon chiral effective approach at next to leading order
- A Method to Extract Charged Hadron Properties from Lattice QCD in Magnetic Fields
Cited by in corpus (25)
- Baryons as relativistic three-quark bound states
- Meson masses in electromagnetic fields with Wilson fermions
- Nucleon Polarizabilities: from Compton Scattering to Hydrogen Atom
- Nucleon Polarisabilities at and Beyond Physical Pion Masses
- Pion magnetic polarisability using the background field method
- Light-quark contributions to the magnetic form factor of the Lambda(1405)
- Magnetic polarisability of the nucleon using a Laplacian mode projection
- Nucleon electromagnetic form factors with non-local chiral effective Lagrangian
- Constraining nucleon strangeness
- Neutron magnetic polarisability with Landau mode operators
- Finite volume effects on the electric polarizability of neutral hadrons in lattice QCD
- Pion in a uniform background magnetic field with clover fermions
- Electromagnetic form factors of octet baryons with the nonlocal chiral effective theory
- Strange form factors of nucleon with nonlocal chiral effective Lagrangian
- The spin of the proton in chiral effective field theory
- Chiral Effective Theory Methods and their Application to the Structure of Hadrons from Lattice QCD
- Generalized parton distributions of sea quarks in the proton from nonlocal chiral effective theory
- Nucleon polarizabilities in covariant baryon chiral perturbation theory with explicit degrees of freedom
- Chiral extrapolation of the charged-pion magnetic polarizability with Padé approximant
- Chiral extrapolation of the magnetic polarizability of the neutral pion
- Chiral extrapolation of nucleon axial charge in effective field theory
- Singlet baryons in the graded symmetry approach to partially quenched QCD
- Chiral Analysis of the Nucleon Mass and Sigma Commutator
- Magnetic Polarisability of Octet Baryons via Lattice QCD
- Sea quark contributions to nucleon electromagnetic form factors with the nonlocal chiral effective Lagrangian