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半导体量子阱中带电和中性激子的光子回波偏振测量

Polarimetry of photon echo on charged and neutral excitons in semiconductor quantum wells.

作者信息

Poltavtsev S V, Kapitonov Yu V, Yugova I A, Akimov I A, Yakovlev D R, Karczewski G, Wiater M, Wojtowicz T, Bayer M

机构信息

Experimentelle Physik 2, Technische Universität Dortmund, 44221, Dortmund, Germany.

Spin Optics Laboratory, St. Petersburg State University, 198504, St. Petersburg, Russia.

出版信息

Sci Rep. 2019 Apr 5;9(1):5666. doi: 10.1038/s41598-019-42208-8.

Abstract

Coherent optical spectroscopy such as four-wave mixing and photon echo generation deliver rich information on the energy levels involved in optical transitions through the analysis of polarization of the coherent response. In semiconductors, it can be applied to distinguish between different exciton complexes, which is a highly non-trivial problem in optical spectroscopy. We develop a simple approach based on photon echo polarimetry, in which polar plots of the photon echo amplitude are measured as function of the angle φ between the linear polarizations of the two exciting pulses. The rosette-like polar plots reveal a distinct difference between the neutral and charged exciton (trion) optical transitions in semiconductor nanostructures. We demonstrate this experimentally by photon echo polarimetry of a CdTe/(Cd, Mg)Te quantum well. The echoes of the trion and donor-bound exciton are linearly polarized at the angle 2φ with respect to the first pulse polarization and their amplitudes are weakly dependent on φ. While on the exciton the photon echo is co-polarized with the second exciting pulse and its amplitude scales as cosφ.

摘要

诸如四波混频和光子回波产生等相干光学光谱技术,通过对相干响应的极化分析,能够提供有关光学跃迁所涉及能级的丰富信息。在半导体中,它可用于区分不同的激子复合体,这在光谱学中是一个极具挑战性的问题。我们基于光子回波偏振测量法开发了一种简单方法,其中测量光子回波振幅的极坐标图作为两个激发脉冲线性偏振之间角度φ的函数。类似玫瑰花结的极坐标图揭示了半导体纳米结构中中性激子和带电激子(激子三重态)光学跃迁之间的明显差异。我们通过对CdTe/(Cd,Mg)Te量子阱进行光子回波偏振测量实验来证明这一点。激子三重态和施主束缚激子的回波相对于第一个脉冲偏振以2φ角线性偏振,并且它们的振幅对φ的依赖性较弱。而对于激子,光子回波与第二个激发脉冲共偏振,并且其振幅按cosφ缩放。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5f08/6450863/2f74629b49a0/41598_2019_42208_Fig1_HTML.jpg

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