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微腔线中极化激元孤子的后向切伦科夫辐射。

Backward Cherenkov radiation emitted by polariton solitons in a microcavity wire.

机构信息

Department of Physics, University of Bath, Bath, BA2 7AY, UK.

Department of Nanophotonics and Metamaterials, ITMO University, 197101, St. Petersburg, Russia.

出版信息

Nat Commun. 2017 Nov 16;8(1):1554. doi: 10.1038/s41467-017-01751-6.

Abstract

Exciton-polaritons in semiconductor microcavities form a highly nonlinear platform to study a variety of effects interfacing optical, condensed matter, quantum and statistical physics. We show that the complex polariton patterns generated by picosecond pulses in microcavity wire waveguides can be understood as the Cherenkov radiation emitted by bright polariton solitons, which is enabled by the unique microcavity polariton dispersion, which has momentum intervals with positive and negative group velocities. Unlike in optical fibres and semiconductor waveguides, we observe that the microcavity wire Cherenkov radiation is predominantly emitted with negative group velocity and therefore propagates backwards relative to the propagation direction of the emitting soliton. We have developed a theory of the microcavity wire polariton solitons and of their Cherenkov radiation and conducted a series of experiments, where we have measured polariton-soliton pulse compression, pulse breaking and emission of the backward Cherenkov radiation.

摘要

半导体微腔中的激子极化激元形成了一个高度非线性的平台,可用于研究各种界面光学、凝聚态物质、量子和统计物理学的现象。我们表明,微腔波导中皮秒脉冲产生的复杂极化激元模式可以理解为亮极化激子孤子发射的切伦科夫辐射,这是由微腔极化激元色散的独特性所实现的,其具有具有正群速度和负群速度的动量间隔。与光纤和半导体波导不同,我们观察到微腔线切伦科夫辐射主要是在负群速度下发射的,因此相对于发射孤子的传播方向向后传播。我们已经发展了微腔线极化激子孤子及其切伦科夫辐射的理论,并进行了一系列实验,其中我们测量了极化激子孤子脉冲压缩、脉冲破裂和向后的切伦科夫辐射的发射。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/270d/5691178/fc9424ded89d/41467_2017_1751_Fig1_HTML.jpg

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