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Polaritons are Not Weakly Interacting: Direct Measurement of the Polariton-Polariton Interaction Strength

机译:polaritons不是弱相互作用:直接测量   polariton-polariton相互作用强度

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摘要

Exciton-polaritons in a microcavity are composite two-dimensional bosonicquasiparticles, arising from the strong coupling between confined light modesin a resonant planar optical cavity and excitonic transitions, typically usingexcitons in semiconductor quantum wells (QWs) placed at the antinodes of thesame cavity. Quantum phenomena such as Bose-Einstein condensation (BEC),quantized vortices, and macroscopic quantum states have been reported attemperatures from tens of Kelvin up to room temperatures, and polaritonicdevices such as spin switches \cite{Amo2010} and optical transistors have alsobeen reported. Many of these effects of exciton-polaritons depend crucially onthe polariton-polariton interaction strength. Despite the importance of thisparameter, it has been difficult to make an accurate experimental measurement,mostly because of the difficulty of determining the absolute densities ofpolaritons and bare excitons. Here we report the direct measurement of thepolariton-polariton interaction strength in a very high-Q microcavitystructure. By allowing polaritons to propagate over 40 $\mu$m to the center ofa laser-generated annular trap, we are able to separate the polariton-polaritoninteractions from polariton-exciton interactions. The interaction strength isdeduced from the energy renormalization of the polariton dispersion as thepolariton density is increased, using the polariton condensation as a benchmarkfor the density. We find that the interaction strength is about two orders ofmagnitude larger than previous theoretical estimates, putting polaritonssquarely into the strongly-interacting regime. When there is a condensate, wesee a sharp transition to a different dependence of the renormalization on thedensity, which is evidence of many-body effects.
机译:微腔中的激子极化子是复合二维的拟准玻色子粒子,是由于共振平面光学腔中的受限光模式与激子跃迁之间的强耦合而产生的,通常使用位于相同腔体波腹处的半导体量子阱(QW)中的激子。据报道,玻色-爱因斯坦凝聚(BEC),量子化涡旋和宏观量子态等量子现象在从数十开尔文到室温的温度范围内都有报道,还报道了诸如自旋开关\ cite {Amo2010}和光学晶体管之类的极化设备。激子-极化子的这些作用中的许多关键取决于极化子-极化子的相互作用强度。尽管此参数很重要,但很难进行精确的实验测量,主要是因为难以确定极化子和裸激子的绝对密度。在这里,我们报告了在非常高Q的微腔结构中对极化子-极化子相互作用强度的直接测量。通过允许极化子传播超过40μm到激光产生的环形阱的中心,我们能够将极化子-极化子相互作用与极化子-激子相互作用分开。使用极化子缩合作为密度的基准,随着极化子密度的增加,相互作用强度由极化子分散体的能量重新归一化得出。我们发现相互作用强度比以前的理论估计值大两个数量级,使极化子平方成为强相互作用体系。当有凝结水时,我们看到重新规范化对密度的不同依赖性急剧过渡,这证明了多体效应。

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