arXiv:2103.13829 · Physical Review A
Long-range additive and nonadditive potentials in a hybrid system: Ground-state atom, excited-state atom, and ion
Pei-Gen Yan, Li-Yan Tang, Zong-Chao Yan, J. F. Babb
Abstract
We report a theoretical study on the long-range additive and nonadditive potentials for a three-body hybrid atom-atom-ion system composed of one ground-$S$-state Li atom, one excited-$P$-state Li atom, and one ground-$S$-state ${\mathrm{Li}}^{+}$ ion, $\mathrm{Li}(2{\phantom{\rule{0.16em}{0ex}}}^{2}S)\text{\ensuremath{-}}\mathrm{Li}(2{\phantom{\rule{0.16em}{0ex}}}^{2}P)\text{\ensuremath{-}}{\mathrm{Li}}^{+}(1{\phantom{\rule{0.16em}{0ex}}}^{1}S$). The interaction coefficients are evaluated with highly accurate wave functions calculated variationally in Hylleraas coordinates. For this hybrid system the three-body nonadditive interactions (appearing in second order) induced by the energy degeneracy and enhanced by the induction effect of the ${\mathrm{Li}}^{+}$ ion through the internal electric field can be strong and even stronger than the two-body additive interactions at the same order. We find that for particular geometries the two-body additive interactions of the system sum to zero, leaving only three-body nonadditive interactions, thus making the present system potentially a platform to explore quantum three-body effects. We also extract by first principles the leading coefficients of the long-range electrostatic, induction, and dispersion energies of ${\text{Li}}_{2}{}^{+}$ electronic states correlating to ${\text{Li}}^{+}(1{\phantom{\rule{0.16em}{0ex}}}^{1}S)\ensuremath{-}\text{Li}(2{\phantom{\rule{0.16em}{0ex}}}^{2}P)$. The results should be especially valuable for the exploration of schemes to create trimers with ultracold atoms and ions in optical lattices.