2013
DOI: 10.1103/physreva.88.033422
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Anisotropic deformation of the Rydberg-blockade sphere in few-atom systems

Abstract: Rydberg blockade sphere persists an intriguing picture by which a number of collective many-body effects caused by the strong Rydberg-Rydberg interactions can be clearly understood and profoundly investigated. In the present work, we develop a new definition for the effective two-atom blockade radius and show that the original spherically shaped blockade surface would be deformed when the real number of atoms increases from two to three. This deformation of blockade sphere reveals spatially anisotropic and shr… Show more

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Cited by 11 publications
(6 citation statements)
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“…To quantitatively estimate s, we find that the single-atom blockade radius can be roughly given by R b = (C 6 /ω) 1/6 [36]. With definitions of R and R b , we can finally arrive at a reduced form of the approximated interaction s, which is [37]…”
Section: C6mentioning
confidence: 99%
“…To quantitatively estimate s, we find that the single-atom blockade radius can be roughly given by R b = (C 6 /ω) 1/6 [36]. With definitions of R and R b , we can finally arrive at a reduced form of the approximated interaction s, which is [37]…”
Section: C6mentioning
confidence: 99%
“…Analysis of the residual double excitation probability reveals it to be higher than expected from calculated blockade strengths. This points to either an overestimation of the van der Waals strength or to a diminution of the blockade through three-body interactions [52,53]. These results underpin the notion that, in order to rely on a robust blockade mechanism in an array of Rydberg atoms, one has to carefully tune the experimental parameters when working with D states.…”
Section: Collective Rabi Oscillationsmentioning
confidence: 92%
“…[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%