在振荡波导阵列中观察π单子
Antonina A Arkhipova1, Yiqi Zhang2, Yaroslav V Kartashov3
1Institute of Spectroscopy, Russian Academy of Sciences, Troitsk 108840, Russia; Faculty of Physics, Higher School of Economics, Moscow 105066, Russia.
Science bulletin
|August 12, 2023
概括
研究人员观察到Floquet系统中的新型拓状态,称为异常pi模式. 这些模式导致了光子波导阵列中拓性pi单子的创建.
科学领域:
- 拓性光子学是一个专业的专业.
- 非线性光学是一种非线性光学.
- 量子动力学就是量子动力学.
背景情况:
- 具有时间变化的参数的花束系统允许在静态系统中缺少的新型拓相.
- Su-Schrieffer-Heeger网格在边缘呈现异常的pi模式,即使在微不足道和非微不足道的拓阶段之间定期过渡时也是如此.
研究的目的:
- 在Floquet Su-Schrieffer-Heeger波导阵列中实验观察光子异常pi模式.
- 从这些模式中演示出一种新的拓性pi单子类.
主要方法:
- 在非线性光学介质中使用1D和2D阵列的周期振荡波导.
- 研究光子异常pi模式的行为,并在高光学功率下分叉拓学pi单子.
主要成果:
- 在1D和2D波导阵列的边缘和角落对光子异常pi模式的实验观测.
- 展示了一种新类的拓性pi单子,它们是具有振荡形状的非线性Floquet状态.
- 在1D和2D数组中,pi单子的稳定传播,2D数组实现了Floquet光子高阶拓绝缘体.
结论:
- 光子异常pi模式可以在振荡波导阵列中实现.
- 拓的pi单元代表了一类新的非线性Floquet状态,具有可调的定位属性.
- 这项工作将Floquet拓相的研究扩展到非线性光学和更高阶拓绝缘体.
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