2017
DOI: 10.1038/s41598-017-16533-9
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Robust generation of entangled state via ground-state antiblockade of Rydberg atoms

Abstract: We propose a mechanism of ground-state antiblockade of Rydberg atoms, which is then exploited to prepare two-atom entangled state via three different kinds of pulses. First we use the pulses in the form of sin2 and cos2 functions and obtain a maximally entangled state at an accurate interaction time. Then the method of stimulated Raman adiabatic passage (STIRAP) is adopted for the entanglement generation, which is immune to the fluctuations of revelent parameters but requires a long time. Finally we capitalize… Show more

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Cited by 18 publications
(18 citation statements)
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References 41 publications
(30 reference statements)
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“…For the second set of data, we consider an initial state where the qubits are in an entangled state. The qubits form Rydberg atom pairs under the condition of Rydberg blockades [50][51][52][53][54] which implies that both the qubits cannot be simultaneously excited to Rydberg states. This is done by first preparing both the qubits in |00 state.…”
Section: Resultsmentioning
confidence: 99%
“…For the second set of data, we consider an initial state where the qubits are in an entangled state. The qubits form Rydberg atom pairs under the condition of Rydberg blockades [50][51][52][53][54] which implies that both the qubits cannot be simultaneously excited to Rydberg states. This is done by first preparing both the qubits in |00 state.…”
Section: Resultsmentioning
confidence: 99%
“…Ω 2 1p /4∆ 1 |1 1 1|, Ω2 m cos 2 ωt/4∆ 1 |r 1 r|, Ω 2 2p /4∆ 2 |1 2 1|, and Ω 2 2r /4∆ 2 |r 2 r|. These unwanted energy shifts can be eliminated through some manners, such as auxiliary fields [65], detuning compensations [66], and phase corrections [67].…”
Section: Discussionmentioning
confidence: 99%
“…[15,16] and experimentally verified by Weidemüller group in 87 Rb atoms [17], occurs when the interaction induced energetic shift can be well compensated by the laser detuning to the Rydberg level, triggering many interesting applications then. For instance it enables the implementation of an accurate one-step quantum logic gate [18] or a maximal entanglement [19,20], facilitating excitation dynamics even in thermal atoms beyond the frozen limit [21][22][23] or in anisotropic interacting systems due to partial resonance [24]. Besides, some nontrivial facilitation approaches, such as relying on inhomogeneous broadening on blue-detuned atoms with attractive interactions [25], avoided crossings between collective manybody states [26,27], or seeded avalanche dynamics in offresonant Rydberg atoms [28], have been proposed, providing more prospects for observing strongly correlated excitation growth in ultracold Rydberg gases [29][30][31].…”
Section: Introductionmentioning
confidence: 99%