Octet Baryon Magnetic Moments from Lattice QCD: Approaching Experiment from a Three-Flavor Symmetric Point
arXiv:1609.03985 · doi:10.1103/PhysRevD.95.114513
Abstract
Lattice QCD calculations with background magnetic fields are used to determine the magnetic moments of the octet baryons. Computations are performed at the physical value of the strange quark mass, and two values of the light quark mass, one corresponding to the three-flavor symmetric point, where the pion mass is 800 MeV, and the other corresponding to a pion mass of 450 MeV. The moments are found to exhibit only mild pion-mass dependence when expressed in terms of appropriately chosen magneton units- the natural baryon magneton. A curious pattern is revealed among the anomalous baryon magnetic moments which is linked to the constituent quark model, however, careful scrutiny exposes additional features. Relations expected to hold in the large-Nc limit of QCD are studied; and, in one case, a clear preference for the quark model over the large-Nc prediction is found. The magnetically coupled Lambda-Sigma system is treated in detail at the three-flavor symmetric point, with the lattice QCD results comparing favorably with predictions based on SU(3)F symmetry. This analysis enables the first extraction of the isovector transition magnetic polarizability. The possibility that large magnetic fields stabilize strange matter is explored, but such a scenario is found to be unlikely.
30 pages, 18 figures, v2 revision corresponds to published version
References in corpus (13)
- Physics of Strongly Magnetized Neutron Stars
- Light Nuclei and Hypernuclei from Quantum Chromodynamics in the Limit of SU(3) Flavor Symmetry
- Light hadron spectroscopy using domain wall valence quarks on an Asqtad sea
- Proton-proton fusion and tritium -decay from lattice quantum chromodynamics
- Magnetic moments of light nuclei from lattice quantum chromodynamics
- Extracting Nucleon Magnetic Moments and Electric Polarizabilities from Lattice QCD in Background Electric Fields
- On the Feynman-Hellmann Theorem in Quantum Field Theory and the Calculation of Matrix Elements
- Electromagnetic and spin polarisabilities in lattice QCD
- A Feynman-Hellmann approach to the spin structure of hadrons
- Sea contributions to the electric polarizability of the hadrons
- Neutron in a Strong Magnetic Field: Finite Volume Effects
- Reconciling the lattice background field method with nonrelativistic QED: Spinor case
- Photodisintegration of a Bound State on the Torus
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