Grankin A, Brion E, Boddeda R, Ćuk S, Usmani I, Ourjoumtsev A, Grangier P
Laboratoire Charles Fabry, Institut d'Optique Graduate School, CNRS, Université Paris-Saclay, 91127 Palaiseau, France.
Laboratoire Aimé Cotton, Université Paris-Sud, ENS Cachan, CNRS, Université Paris-Saclay, 91405 Orsay Cedex, France.
Phys Rev Lett. 2016 Dec 16;117(25):253602. doi: 10.1103/PhysRevLett.117.253602.
Electromagnetically induced transparency (EIT) in a ladder system involving a Rydberg level is known to yield giant optical nonlinearities for the probe field, even in the few-photon regime. This enhancement is due to the strong dipole-dipole interactions between Rydberg atoms and the resulting excitation blockade phenomenon. In order to study such highly correlated media, ad hoc models or low-excitation assumptions are generally used to tackle their dynamical response to optical fields. Here, we study the behavior of a cavity Rydberg-EIT setup in the nonequilibrium quantum field formalism, and we obtain analytic expressions for elastic and inelastic components of the cavity transmission spectrum, valid up to higher excitation numbers than previously achieved. This allows us to identify and interpret a polaritonic resonance structure, to our knowledge unreported so far.
众所周知,即使在少光子 regime 中,涉及里德堡能级的阶梯系统中的电磁诱导透明(EIT)也会为探测场产生巨大的光学非线性。这种增强是由于里德堡原子之间强烈的偶极 - 偶极相互作用以及由此产生的激发阻塞现象。为了研究这种高度相关的介质,通常使用特殊模型或低激发假设来处理它们对光场的动态响应。在这里,我们在非平衡量子场形式主义中研究腔里德堡 - EIT装置的行为,并获得腔透射谱的弹性和非弹性分量的解析表达式,其有效性可达比以前更高的激发数。这使我们能够识别和解释一种极化激元共振结构,据我们所知,这是迄今为止尚未报道的。