Magnetic Dipole, Electric Quadrupole and Magnetic Octupole Moments of the Baryons in Light Cone QCD Sum Rules
arXiv:0811.2670 · doi:10.1140/epjc/s10052-009-0988-0
Abstract
Due to the very short life time of the baryons, a direct measurement on the electromagnetic moments of these systems is almost impossible in the experiment and can only be done indirectly. Although only for the magnetic dipole moments of and systems there are some experimental data, the theoretical, phenomenological and lattice calculations could play crucial role. In present work, the magnetic dipole () , electric quadrupole () and magnetic octupole () moments of these baryons are computed within the light cone QCD sum rules. The results are compared with the predictions of the other phenomenological approaches, lattice QCD and existing experimental data.
21 Pages, 3 Figures and 2 Tables
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Cited by in corpus (9)
- Electromagnetic structure of the lowest-lying decuplet resonances in covariant chiral perturbation theory
- Electromagnetic properties of the Delta(1232) and decuplet baryons in the self-consistent SU(3) chiral quark-soliton model
- Electric Quadrupole and Magnetic Octupole Moments of the Light Decuplet Baryons Within Light Cone QCD Sum Rules
- Electromagnetic form factors of the baryon decuplet with flavor SU(3) symmetry breaking
- Quadrupole moments of low lying baryons with spin 1/2^+, spin 3/2^+, and spin 3/2^+ \to 1/2^+ transitions
- Radiative pion photoproduction in covariant chiral perturbation theory
- Sea contribution to the charge radii and quadrupole moment of baryons
- Baryon quadrupole moment in the 1/N(c) expansion of QCD
- Structure of the baryon and the kaon cloud