在非线性极子凝聚物中的合波格中的拓边缘和角状态
Tobias Schneider1, Wenlong Gao2, Thomas Zentgraf1,3
1Department of Physics and Center for Optoelectronics and Photonics Paderborn (CeOPP), Paderborn University, 33098 Paderborn, Germany.
Nanophotonics (Berlin, Germany)
|December 5, 2024
概括
我们报告了双波链和2D网格中的新型拓边缘状态. 光学非线性在激发极子系统中诱导这些边缘和角状态的多稳定性.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 拓学物质是一个拓学物质.
- 非线性光学是非线性光学.
背景情况:
- 在各种系统中,拓状态被广泛研究.
- 双波 (DW) 链为探索拓现象提供了一个平台.
- 驱动散射式刺激极子系统表现出独特的量子性质.
研究的目的:
- 为了研究双波 (DW) 链中的拓边缘状态.
- 探索光学非线性对边缘状态形成和稳定性的影响.
- 在二维 (2D) 多波网格中实现更高阶的拓绝缘体角态.
主要方法:
- 使用一个通用的奥布里-安德烈-哈珀 (AAH) 模型来描述DW链.
- 在驱动散流式激电极子系统中采用共振光学激发.
- 通过堆叠DW链来形成多波网格,将系统扩展到2D.
主要成果:
- 在DW链中形成不同的拓边缘状态.
- 由于光学非线性,在边缘状态中观察多稳定性.
- 在2D网格中出现更高层次的拓绝缘体角态.
- 由非线性诱导的局部化引起的多稳定的角态.
结论:
- DW链支持多样化的拓边缘状态.
- 光学非线性引入了多稳定性和新的本地化现象.
- 2D多波格子表现出具有多稳定的角态的高阶拓相.
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