在无序的二维绝缘体中,自旋轨道合激子的量子混乱特征
V A Stephanovich1, E V Kirichenko1, K Książek1
1Institute of Physics, <a href="https://ror.org/04gbpnx96">University of Opole</a>, Oleska 48, 45-052, Opole, Poland.
Physical review. E
|September 19, 2024
概括
我们探讨了扰乱和自旋轨道合 (SOC) 如何影响二维半导体中的激子光谱. 它们的联合效应可以诱导量子混乱特征,可通过SOC,库伦相互作用和分数障碍来控制.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子力学就是量子力学.
- 材料科学是一种材料科学.
背景情况:
- 2D半导体中的激发光谱对于光电子应用至关重要.
- 众所周知,扰乱和旋转轨道合 (SOC) 影响电子属性.
- 了解它们的相互作用是设计新型量子设备的关键.
研究的目的:
- 为了研究混乱和SOC在2D半导体中的激电谱上的协同效应.
- 探索这些系统中量子混乱特征的出现.
- 为了确定这些混乱行为的控制机制.
主要方法:
- 在施罗丁格方程中使用 Riesz 分数导数对混乱的现象学建模.
- 分析和数值方法来解决修改的施罗丁格方程.
- 激子能量水平和相邻水平距离分布的分析.
主要成果:
- 分数乱和SOC的结合效应与普通系统相比,显著改变了刺激子光谱.
- 邻近水平距离的非波伊森统计表明量子混乱的出现.
- 列维指数 μ 描述了分数失序的程度.
结论:
- 障碍和SOC协同作用可以诱导和控制二维半导体激发光谱中的量子混乱特征.
- 分数计算提供了一种新的方法来模拟障碍效应.
- 可调节的量子混乱为先进的量子信息技术开辟了可能性.
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