概括
我们发现,在非线性拓格子中,可以通过合的拓边缘状态 (CTES) 实现对称性破坏. 增加非线性导致从对称到不对称状态的分叉,证明自发对称性破坏 (SSB).
科学领域:
- 非线性物理学 非线性物理学
- 拓式光子学 拓式光子学
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 拓边缘状态提供独特的属性.
- 在许多物理系统中,自发对称性破坏 (SSB) 是至关重要的.
- 非线性效应可以改变拓状态.
研究的目的:
- 在非线性拓格子中提出SSB的一般原则.
- 调查SSB.中的合拓边缘状态 (CTES) 的作用.
- 探索非线性和链间合对CTES的影响.
主要方法:
- 一个非线性拓格子模型的理论分析.
- 使用一个带有两个Su-Schrieffer-Heeger (SSH) 链的光学共振器阵列.
- 在不同的非线性和合下,研究CTES的破坏对称性的分支.
主要成果:
- 对称的CTES经历超临界分叉,非线性增加.
- 从稳定的对称到稳定的不对称状态的过渡发生在一个关键值之后.
- 不对称的CTES在占据主导的侧面呈现出增强的亚晶格极化.
结论:
- 对称性破坏CTES的分叉提供了SSB在非线性拓格中的通用机制.
- 非线性强度和链间合极大地影响CTES的稳定性和性能.
- 这个原则为设计新型拓设备提供了新的途径.
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