Engineering long-range interactions between high-
n, $n \ge $ 300, strontium Rydberg atoms in a beam
We investigate the effect of series perturbation on the second-order dipole-dipole interactions between strontium atoms in the
5sns(1S0) and
5snp(1P1) Rydberg states as a means of engineering long-range interactions between atoms. The series perturbation in these atoms enables modifying the strength and the sign of the interaction by varying the principal quantum number
n of the Rydberg electron. We utilize experimentally available data to estimate the importance of perturber states, and find that van der Waals interaction between two strontium atoms in the
5snp(1P1) states shows strong peaks outside the anticipated hydrogenic
n11 scaling. We identify this to be the result of the perturbation of
5snd(1D2) intermediate states by the
4d2(1D2) and
4dn′s(1D2) states in the
n<20 range. This demonstrates that divalent atoms offer a unique advantage for generating substantially stronger or weaker inter-atomic interactions than those that can be achieved using alkali metal atoms. This is due to the highly perturbed spectra of divalent atoms and other multivalent atoms that can persist up to high
n. Such irregularities can be especially useful in engineering asymmetric Ry blockade requiring the simultaneous presence of both ``weak'' and ``strong'' interactions.
We investigate the effect of series perturbation on the second order dipole-dipole interactions between strontium atoms in
5sns(1S0) and
5snp(1P1) Rydberg states as a means of engineering long-range interactions between atoms in a way that gives an exceptional level of control over the strength and the sign of the interaction by changing
n. We utilize experimentally available data to estimate the importance of perturber states at low
n, and find that van der Waals interaction between two strontium atoms in the
5snp(1P1) states shows strong peaks outside the usual hydrogenic
n11 scaling. We identify this to be the result of the perturbation of
5snd(1D2) intermediate states by the
4d2(1D2) and
4dn′s(1D2) states in the
n<20 range. This demonstrates that divalent atoms in general present a unique advantage for creating substantially stronger or weaker interaction strengths than those can be achieved using alkali metal atoms due to their highly perturbed spectra that can persist up to high-
n.