Nonadiabatic nonlinear non-Hermitian quantized pumping

Motohiko Ezawa, Natsuko Ishida, Yasutomo Ota, Satoshi Iwamoto
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Abstract

We analyze a quantized pumping in a nonlinear non-Hermitian photonic system with nonadiabatic driving. The photonic system is made of a waveguide array, where the distances between adjacent waveguides are modulated. It is described by the Su-Schrieffer-Heeger model together with a saturated nonlinear gain term and a linear loss term. A topological interface state between the topological and the trivial phases is stabilized by the combination of a saturated nonlinear gain term and a linear loss term. We study the pumping of the topological interface state. We define the transfer-speed ratio ω/Ω by the ratio of the pumping speed ω of the center of mass of the wave packet to the driving speed Ω of the topological interface. It is quantized topologically as ω/Ω=1 in the adiabatic limit. It remains to be quantized dynamically unless the driving is not too fast even in the nonadiabatic regime. On the other hand, the wave packet collapses and there is no quantized pumping when the driving is too fast. In addition, the stability against disorder is more enhanced by stronger nonlinearity.

Abstract Image

非绝热非线性非赫米提量化泵浦
我们分析了非绝热驱动的非线性非赫米提光子系统中的量化抽运。该光子系统由波导阵列组成,相邻波导之间的距离受到调制。该系统由 Su-Schrieffer-Heeger 模型以及饱和非线性增益项和线性损耗项来描述。通过饱和非线性增益项和线性损耗项的组合,拓扑相与三相之间的拓扑界面状态得以稳定。我们研究了拓扑界面状态的泵送。我们用波包质心的抽运速度 ω 与拓扑界面的驱动速度 ω 之比来定义传递速度比 ω/Ω。在绝热极限中,它在拓扑学上被量化为 ω/ω=1。即使在非绝热状态下,除非驱动速度不是太快,否则它仍然是动态量子化的。另一方面,当驱动速度过快时,波包会坍缩,没有量子化抽运。此外,较强的非线性会增强抗失调的稳定性。
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CiteScore
8.60
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