Abstract

Quantum Monte Carlo calculations of electromagnetic moments and transitions are reported for $A\ensuremath{\le}9$ nuclei. The realistic Argonne ${v}_{18}$ two-nucleon and Illinois-7 three-nucleon potentials are used to generate the nuclear wave functions. Contributions of two-body meson-exchange current (MEC) operators are included for magnetic moments and $M1$ transitions. The MEC operators have been derived in both a standard nuclear physics approach and a chiral effective field theory formulation with pions and nucleons including up to one-loop corrections. The two-body MEC contributions provide significant corrections and lead to very good agreement with experiment. Their effect is particularly pronounced in the $A=9$, $T=3/2$ systems, in which they provide up to $\ensuremath{\sim}20%$ ($\ensuremath{\sim}40%$) of the total predicted value for the ${}^{9}$Li (${}^{9}$C) magnetic moment.

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