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Bulletin of the American Physical Society

Engineering long-range interactions between high-$n$, $n \ge $ 300, strontium Rydberg atoms in a beam

Robert Fields, R. Brienza, F. B. Dunning, S. Yoshida, Joachim Burgdörfer

Published May 30, 2019• 0 citations
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Controlling the interactions of very-high-n strontium Rydberg atoms

Robert Fields, F. B. Dunning, Shintaro Yoshida +1 more

Bulletin of the American Physical Society•Jun 6, 2017•0 citations

Tuning long-range interactions in Sr Rydberg atoms: the effect of series perturbations

Türker Topçu, Andrei Derevianko

We investigate the effect of series perturbation on the second-order dipole-dipole interactions between strontium atoms in the $5sns({^1}S_0)$ and $5snp({^1}P_1)$ 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 $5snp({^1}P_1)$ states shows strong peaks outside the anticipated hydrogenic $n^{11}$ scaling. We identify this to be the result of the perturbation of $5snd({^1}D_2)$ intermediate states by the $4d^2({^1}D_2)$ and $4dn's({^1}D_2)$ 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.

arXiv:1505.07152•May 26, 2015•1 citation

Long-range Rydberg-Rydberg interactions at very-high nnn

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Bulletin of the American Physical Society•May 29, 2018•0 citations

L-changing through very-long-range interactions in high-n, n∼300, Rydberg-Rydberg collisions

S. Yoshida, Joachim Burgdörfer, G. Fields +2 more

Synopsis State-changing in thermal-energy collisions between strontium atoms in high-n, n∼300, n1F3 Rydberg states is studied in an atomic beam and analyzed using classical trajectory Monte Carlo simulations. The L-changing cross section is large, ∼10-4 cm2, much greater than the corresponding “hard-sphere” cross section.

Journal of Physics Conference Series•Jan 1, 2020•0 citations

State changing through very-long-range interactions in high- n, n >= 300, Rydberg-Rydberg collisions

S. Yoshida, Joachim Burgdörfer, Robert Fields +2 more

APS•May 1, 2019•0 citations

Rydberg blockade with multivalent atoms: effect of Rydberg series perturbation on van der Waals interactions

Türker Topçu, Andrei Derevianko

We investigate the effect of series perturbation on the second order dipole-dipole interactions between strontium atoms in $5sns({^1}S_0)$ and $5snp({^1}P_1)$ 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 $5snp({^1}P_1)$ states shows strong peaks outside the usual hydrogenic $n^{11}$ scaling. We identify this to be the result of the perturbation of $5snd({^1}D_2)$ intermediate states by the $4d^2({^1}D_2)$ and $4dn's({^1}D_2)$ 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-$n$.

•May 26, 2015•0 citations
Engineering long-range interactions between high-nnn, $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)5sns({^1}S_0)5sns(1S0​) and 5snp(1P1)5snp({^1}P_1)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 nnn 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)5snp({^1}P_1)5snp(1P1​) states shows strong peaks outside the anticipated hydrogenic n11n^{11}n11 scaling. We identify this to be the result of the perturbation of 5snd(1D2)5snd({^1}D_2)5snd(1D2​) intermediate states by the 4d2(1D2)4d^2({^1}D_2)4d2(1D2​) and 4dn′s(1D2)4dn's({^1}D_2)4dn′s(1D2​) states in the n<20n<20n<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 nnn. 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)5sns({^1}S_0)5sns(1S0​) and 5snp(1P1)5snp({^1}P_1)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 nnn. We utilize experimentally available data to estimate the importance of perturber states at low nnn, and find that van der Waals interaction between two strontium atoms in the 5snp(1P1)5snp({^1}P_1)5snp(1P1​) states shows strong peaks outside the usual hydrogenic n11n^{11}n11 scaling. We identify this to be the result of the perturbation of 5snd(1D2)5snd({^1}D_2)5snd(1D2​) intermediate states by the 4d2(1D2)4d^2({^1}D_2)4d2(1D2​) and 4dn′s(1D2)4dn's({^1}D_2)4dn′s(1D2​) states in the n<20n<20n<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-nnn.