2019
DOI: 10.1103/physreva.99.033826
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Unidirectional and controllable higher-order diffraction by a Rydberg electromagnetically induced grating

Abstract: A method for diffracting the weak probe beam into unidirectional and higher-order directions is proposed via a novel Rydberg electromagnetically induced grating, providing a new way for the implementations of quantum devices with cold Rydberg atoms. The proposed scheme utilizes a suitable and position-dependent adjustment to the two-photon detuning besides the modulation of the standing-wave coupling field, bringing a in-phase modulation which can change the parity of the dispersion. We observe that when the m… Show more

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Cited by 38 publications
(23 citation statements)
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“…In contrast with previous studies [47][48][49], the transmission function, (9), depends not only on the linear potential but also on the nonlocal nonlinear potential and the intensity of the probe field.…”
Section: A General Results For Raman-nath Diffractioncontrasting
confidence: 73%
See 1 more Smart Citation
“…In contrast with previous studies [47][48][49], the transmission function, (9), depends not only on the linear potential but also on the nonlocal nonlinear potential and the intensity of the probe field.…”
Section: A General Results For Raman-nath Diffractioncontrasting
confidence: 73%
“…In addition to fundamental interest, the exploration of optical PT symmetry has facilitated various applications, including nonreciprocal light propagation and unidirectional invisibility [33][34][35], coherent perfect absorbers [36][37][38], giant light amplification [39], singlemode lasers [40,41], supersensitive sensors [42,43], and so on [44]. The combined effects of PT symmetry and optical gratings in the linear optics regime lead to many interesting phenomena, such as beam rectification and dynamic localization [45], spatially asymmetric light diffraction [46][47][48][49], and a new class of self-imaging Talbot effects [50].…”
Section: Introductionmentioning
confidence: 99%
“…Cooperative nonlinear gratings allow one to distinguish light fields of different photon statistics with the dipole blockade effect of Rydberg atoms [41,42], while non-Hermitian gratings typically result in asymmetric diffraction patterns that can be tuned through the out-of-phase interplay of phase and amplitude modulations [43][44][45][46]. Unidirectional and controlled higher-order diffraction, through non-Hermitian modulations on EIG structures built from Rydberg atoms driven beyond the dipole blockade regime, has also been reported [47]. Most of the above works hinge, however, on 1D Hermitian or non-Hermitian EIG structures.…”
Section: Introductionmentioning
confidence: 99%
“…The appearance of EIG with Rydberg atoms has also been discussed in Refs. 23 , 24 . It is worth mentioning that, in case of Rydberg atoms, one can obtain the phenomenon of EIG for the excited states wherein strong optical nonlinear effect is induced due to dipole-dipole interaction.…”
Section: Introductionmentioning
confidence: 99%