Coherence of the Borromean three-body F\'orster resonances in Rydberg atoms
Autor: | Ryabtsev, I. I., Beterov, I. I., Tretyakov, D. B., Yakshina, E. A., Entin, V. M., Cheinet, P., Pillet, P. |
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Rok vydání: | 2018 |
Předmět: | |
Zdroj: | Phys. Rev. A 98, 052703 (2018) |
Druh dokumentu: | Working Paper |
DOI: | 10.1103/PhysRevA.98.052703 |
Popis: | We have observed recently the Stark-tuned three-body F\"orster resonances ${\rm 3}\times nP_{3/2} (|M|)\to nS_{1/2} +(n+1)S_{1/2} +nP_{3/2} (|M^{*} |)$ at long-range interactions of a few cold Rb Rydberg atoms [D.B.Tretyakov et al., Phys. Rev. Lett. 119, 173402 (2017)]. The three-body resonance appears at a different dc electric field with respect to the ordinary two-body resonance ${\rm 2}\times nP_{3/2} (|M|)\to nS_{1/2} +(n+1)S_{1/2} $ and corresponds to a transition when the three interacting atoms change their states simultaneously (two atoms go to the $S$ states, and the third atom remains in the $P$ state but changes its moment projection), with the negligible contribution of the two-body resonance to the population transfer. It thus has a Borromean character and represents an effective three-body operator, which can be used to directly control the three-body interactions in quantum simulations and quantum gates implemented with Rydberg atoms. In this paper we theoretically investigate the coherence of such three-body resonances and we show that high-contrast Rabi-like population oscillations are possible for the localized Rydberg atoms in a certain spatial configuration. This paves the way to implementing three-qubit quantum gates and quantum simulations based on three-body Rydberg interactions. Comment: 14 pages, 5 figures. arXiv admin note: substantial text overlap with arXiv:1707.01636 |
Databáze: | arXiv |
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