2016
DOI: 10.1016/bs.aamop.2016.04.005
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Quantum and Nonlinear Optics in Strongly Interacting Atomic Ensembles

Abstract: Coupling light to ensembles of strongly interacting particles has emerged as a promising route toward achieving few photon nonlinearities. One specific way to implement this kind of nonlinearity is to interface light with highly excited atomic Rydberg states by means of electromagnetically induced transparency, an approach which allows freely propagating photons to acquire synthetic interactions of hitherto unprecedented strength. Here, we present an overview of this rapidly developing field, from classical ef… Show more

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Cited by 66 publications
(116 citation statements)
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References 197 publications
(304 reference statements)
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“…One way to achieve the large optical nonlinearities [19,20] required for single photon switching is by means of electromagnetically induced transparency (EIT) [21] with strongly interacting Rydberg states [22] in atomic ensembles (see [23][24][25][26][27][28][29][30][31][32][33][34]). The dissipative optical nonlinearities available with this approach [24,26,28,29,31,35,36] provide a novel mechanism for single-photon detection [37], generation [31] and substraction [38,39] as well as classical switching capabilities, as recently demonstrated in [17,18,37,40].…”
Section: Introductionmentioning
confidence: 99%
“…One way to achieve the large optical nonlinearities [19,20] required for single photon switching is by means of electromagnetically induced transparency (EIT) [21] with strongly interacting Rydberg states [22] in atomic ensembles (see [23][24][25][26][27][28][29][30][31][32][33][34]). The dissipative optical nonlinearities available with this approach [24,26,28,29,31,35,36] provide a novel mechanism for single-photon detection [37], generation [31] and substraction [38,39] as well as classical switching capabilities, as recently demonstrated in [17,18,37,40].…”
Section: Introductionmentioning
confidence: 99%
“…We have considered the conversion of at most one microwave photon to an optical photon, for which the interatomic Rydberg-Rydberg interactions are absent. In the case of multiple photons, however, the long-range interatomic interactions will induce strong non-linearities accompanied by the suppression of multiple Rydberg excitations within the blockade volume associated with each photon [39,40]. This can potentially hinder the microwave photon conversion and optical photon collection due to distortion of the temporal and spatial profile of the emitted radiation.…”
Section: Discussionmentioning
confidence: 99%
“…Here we derive equation (6) of the main text by using an expansion of the Green's function in terms of plane and evanescent waves. The Green's function equation (3) can be written in the angular spectrum representation, i.e.as an integral over k x and k y in Fourier space, as [43] k k k k G r r Q , , i 8…”
Section: Appendix a Green's Function Expansion In Plane And Evanescementioning
confidence: 99%
“…Atomic ensembles constitute an important platform for quantum light-matter interfaces [1], enabling applications from quantum memories [2][3][4][5] and few-photon nonlinear optics [6][7][8][9][10][11] to metrology [12][13][14][15]. In typical experiments, ensembles consist of disordered atomic clouds, with the propagation of light through them modeled phenomenologically by the Maxwell-Bloch equations [16,17].…”
Section: Introductionmentioning
confidence: 99%