Three-body Förster resonance of a new type in Rydberg atoms. (March 2020)

• Record Type: Journal Article
• Authors: Cheinet, P.; Pham, K.-L; Pillet, P.; Beterov, I.I.; Ashkarin, I.N.; Tretyakov, D.B.; Yakshina, E.A.; Entin, V.M.; Ryabtsev, I.I.
• Is Part Of: Quantum electronics. Volume 50:Number 3(2020)
• Page Start: 213
• Page End: 219
• Publication Date: 2020-03
• Subjects: Rydberg atoms -- interaction -- Förster resonance; Quantum electronics -- Periodicals; 537.5
• DOI: 10.1070/QEL17253
• Languages: English
• ISSNs: 1063-7818

Abstract

Abstract: The three-body Förster resonances 3 × n P3/2 (| M |) → n S1/2 + ( n + 1)S1/2 + n P3/2 (| M *|), controlled by a constant electric field, were realised earlier by the authors in an ensemble of several cold Rydberg Rb atoms. One of the drawbacks of such resonances for potential application in three-qubit quantum gates is the proximity of the two-body Förster resonance 2 × n P3/2 → n S1/2 + ( n + 1)S1/2, as well as the possibility of their implementation only for states with values of the principal quantum numbers n ⩽38. A three-body resonance of a new type, 3 × n P3/2 → n S1/2 + ( n + 1)S1/2 + n P1/2, which can be realised for arbitrary n, is proposed and analysed. Its specific feature is also that the third atom transits into a state with a different total angular momentum J = 1/2, which has no Stark structure, so that the two-body resonance is completely absent. Numerical calculations showed that for not too strong interaction, it is possible to observe coherent three-body oscillations of the populations of collective states, which is of interest for developing new schemes of three-qubit quantum gates controlled by an electric field.