paper

Magnetic Moment of the , and

arXiv:hep-ph/9401345 · doi:10.1016/0370-2693(94)91326-9

Abstract

The magnetic moment of the , and vanish when the charm quark mass is taken to infinity because the light degrees of freedom are in a spin zero configuration. The heavy quark spin-symmetry violating contribution from the light degrees of freedom starts at order , the same order as the contribution from the heavy charm quark. We compute the leading long-distance contribution to the magnetic moments from the spin-symmetry breaking mass splitting in chiral perturbation theory. These are nonanalytic in the pion mass and arise from calculable one-loop graphs. Further, the difference between the magnetic moments of the charged charmed baryons is independent of the charm quark mass and of the subleading local counterterm.

10 pages, 1 uuencoded figure included, uses harvmac and epsf, CMU-HEP 94-06

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