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Observation of the Borromean Three-Body Förster Resonances for Three Interacting Rb Rydberg Atoms. / Tretyakov, D. B.; Beterov, I. I.; Yakshina, E. A. и др.

в: Physical Review Letters, Том 119, № 17, 173402, 27.10.2017, стр. 173402.

Результаты исследований: Научные публикации в периодических изданияхстатьяРецензирование

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Tretyakov DB, Beterov II, Yakshina EA, Entin VM, Ryabtsev II, Cheinet P и др. Observation of the Borromean Three-Body Förster Resonances for Three Interacting Rb Rydberg Atoms. Physical Review Letters. 2017 окт. 27;119(17):173402. 173402. doi: 10.1103/PhysRevLett.119.173402

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BibTeX

@article{28ca7c3812784b8cbfe0018d2bbd664c,
title = "Observation of the Borromean Three-Body F{\"o}rster Resonances for Three Interacting Rb Rydberg Atoms",
abstract = "Three-body F{\"o}rster resonances at long-range interactions of Rydberg atoms were first predicted and observed in Cs Rydberg atoms by Faoro et al. [Nat. Commun. 6, 8173 (2015)NCAOBW2041-172310.1038/ncomms9173]. In these resonances, one of the atoms carries away an energy excess preventing the two-body resonance, leading thus to a Borromean type of F{\"o}rster energy transfer. But they were in fact observed as the average signal for the large number of atoms N1. In this Letter, we report on the first experimental observation of the three-body F{\"o}rster resonances 3×nP3/2(|M|)→nS1/2+(n+1)S1/2+nP3/2(|M∗|) in a few Rb Rydberg atoms with n=36, 37. We have found here clear evidence that there is no signature of the three-body F{\"o}rster resonance for exactly two interacting Rydberg atoms, while it is present for N=3-5 atoms. This demonstrates the assumption that three-body resonances can generalize to any Rydberg atom. As such resonance represents an effective three-body operator, it can be used to directly control the three-body interactions in quantum simulations and quantum information processing with Rydberg atoms.",
keywords = "STRONG-FIELD REGIME, COLLISIONS, GAS",
author = "Tretyakov, {D. B.} and Beterov, {I. I.} and Yakshina, {E. A.} and Entin, {V. M.} and Ryabtsev, {I. I.} and P. Cheinet and P. Pillet",
note = "Publisher Copyright: {\textcopyright} 2017 American Physical Society.",
year = "2017",
month = oct,
day = "27",
doi = "10.1103/PhysRevLett.119.173402",
language = "English",
volume = "119",
pages = "173402",
journal = "Physical Review Letters",
issn = "0031-9007",
publisher = "American Physical Society",
number = "17",

}

RIS

TY - JOUR

T1 - Observation of the Borromean Three-Body Förster Resonances for Three Interacting Rb Rydberg Atoms

AU - Tretyakov, D. B.

AU - Beterov, I. I.

AU - Yakshina, E. A.

AU - Entin, V. M.

AU - Ryabtsev, I. I.

AU - Cheinet, P.

AU - Pillet, P.

N1 - Publisher Copyright: © 2017 American Physical Society.

PY - 2017/10/27

Y1 - 2017/10/27

N2 - Three-body Förster resonances at long-range interactions of Rydberg atoms were first predicted and observed in Cs Rydberg atoms by Faoro et al. [Nat. Commun. 6, 8173 (2015)NCAOBW2041-172310.1038/ncomms9173]. In these resonances, one of the atoms carries away an energy excess preventing the two-body resonance, leading thus to a Borromean type of Förster energy transfer. But they were in fact observed as the average signal for the large number of atoms N1. In this Letter, we report on the first experimental observation of the three-body Förster resonances 3×nP3/2(|M|)→nS1/2+(n+1)S1/2+nP3/2(|M∗|) in a few Rb Rydberg atoms with n=36, 37. We have found here clear evidence that there is no signature of the three-body Förster resonance for exactly two interacting Rydberg atoms, while it is present for N=3-5 atoms. This demonstrates the assumption that three-body resonances can generalize to any Rydberg atom. As such resonance represents an effective three-body operator, it can be used to directly control the three-body interactions in quantum simulations and quantum information processing with Rydberg atoms.

AB - Three-body Förster resonances at long-range interactions of Rydberg atoms were first predicted and observed in Cs Rydberg atoms by Faoro et al. [Nat. Commun. 6, 8173 (2015)NCAOBW2041-172310.1038/ncomms9173]. In these resonances, one of the atoms carries away an energy excess preventing the two-body resonance, leading thus to a Borromean type of Förster energy transfer. But they were in fact observed as the average signal for the large number of atoms N1. In this Letter, we report on the first experimental observation of the three-body Förster resonances 3×nP3/2(|M|)→nS1/2+(n+1)S1/2+nP3/2(|M∗|) in a few Rb Rydberg atoms with n=36, 37. We have found here clear evidence that there is no signature of the three-body Förster resonance for exactly two interacting Rydberg atoms, while it is present for N=3-5 atoms. This demonstrates the assumption that three-body resonances can generalize to any Rydberg atom. As such resonance represents an effective three-body operator, it can be used to directly control the three-body interactions in quantum simulations and quantum information processing with Rydberg atoms.

KW - STRONG-FIELD REGIME

KW - COLLISIONS

KW - GAS

UR - http://www.scopus.com/inward/record.url?scp=85032510460&partnerID=8YFLogxK

U2 - 10.1103/PhysRevLett.119.173402

DO - 10.1103/PhysRevLett.119.173402

M3 - Article

C2 - 29219438

AN - SCOPUS:85032510460

VL - 119

SP - 173402

JO - Physical Review Letters

JF - Physical Review Letters

SN - 0031-9007

IS - 17

M1 - 173402

ER -

ID: 8673718