非赫米提散射系统中复杂时延的超通用统计

Nadav Shaibe, Jared M. Erb, Steven M. Anlage
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引用次数: 0

摘要

通量守恒系统的维格纳-史密斯(Wigner-Smith)时间延迟是一个实量,用于度量激发在相互作用区域的驻留时间。时间延迟在非赫米提系统中的复杂泛化仍处于发展阶段,特别是其在复杂混沌散射系统短波长极限中的统计特性尚未得到研究。根据实验测得的一维图形、二维台球和三维空腔的多端口散射($S$)矩阵,我们计算了复维格纳-史密斯($\tau_{WS}$)以及每个单独的反射($\tau_{xx}$)和透射($\tau_{xy}$)时延。计算了每个端口之间的复合反射时延差($\tau_{\delta R}$),并为表现出非互易散射的系统引入了透射时延差($\tau_{\delta T}$)。大时延与相干完美吸收、无反射散射、慢光和单向隐形有关。我们证明了这些时间延迟量的实部和虚部分布的大延迟尾部是超普遍的,与实验参数无关:均匀衰减 $\eta$、散射通道数 $M$、波传播维度 $\mathcal{D}$和戴森对称类 $\beta$。这种超普遍性与已确立的单元散射系统的时间延迟统计形成了直接对比,在单元散射系统中,$\tau_{WS}$分布的尾部明确取决于$M$和$\beta$的值。由于波方程的直接类比,本文描述的时延统计适用于短波长极限的任何非赫米梯波混沌散射系统,如量子图、电磁、光学和声学谐振器等。
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Superuniversal Statistics of Complex Time-Delays in Non-Hermitian Scattering Systems
The Wigner-Smith time-delay of flux conserving systems is a real quantity that measures how long an excitation resides in an interaction region. The complex generalization of time-delay to non-Hermitian systems is still under development, in particular, its statistical properties in the short-wavelength limit of complex chaotic scattering systems has not been investigated. From the experimentally measured multi-port scattering ($S$)-matrices of one-dimensional graphs, a two-dimensional billiard, and a three-dimensional cavity, we calculate the complex Wigner-Smith ($\tau_{WS}$), as well as each individual reflection ($\tau_{xx}$) and transmission ($\tau_{xy}$) time-delays. The complex reflection time-delay differences ($\tau_{\delta R}$) between each port are calculated, and the transmission time-delay differences ($\tau_{\delta T}$) are introduced for systems exhibiting non-reciprocal scattering. Large time-delays are associated with coherent perfect absorption, reflectionless scattering, slow light, and uni-directional invisibility. We demonstrate that the large-delay tails of the distributions of the real and imaginary parts of each of these time-delay quantities are superuniversal, independent of experimental parameters: uniform attenuation $\eta$, number of scattering channels $M$, wave propagation dimension $\mathcal{D}$, and Dyson symmetry class $\beta$. This superuniversality is in direct contrast with the well-established time-delay statistics of unitary scattering systems, where the tail of the $\tau_{WS}$ distribution depends explicitly on the values of $M$ and $\beta$. Due to the direct analogy of the wave equations, the time-delay statistics described in this paper are applicable to any non-Hermitian wave-chaotic scattering system in the short-wavelength limit, such as quantum graphs, electromagnetic, optical and acoustic resonators, etc.
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