Department of Applied Physics, Stanford University, Stanford, California 94305, United States.
SLAC National Accelerator Laboratory, Menlo Park, California 94025, United States.
Nano Lett. 2022 Oct 26;22(20):8389-8393. doi: 10.1021/acs.nanolett.2c02819. Epub 2022 Sep 16.
Sharp resonances can strongly modify the electromagnetic response of matter. A classic example is the Reststrahlen effect - high reflectivity in the mid-infrared in many polar crystals near their optical phonon resonances. Although this effect in bulk materials has been studied extensively, a systematic treatment for finite thickness remains challenging. Here we describe, experimentally and theoretically, the Reststrahlen response in hexagonal boron nitride across more than 5 orders of magnitude in thickness, down to a monolayer. We find that the high reflectivity plateau of the Reststrahlen band evolves into a single peak as the material enters the optically thin limit, within which two distinct regimes emerge: a strong-response regime dominated by coherent radiative decay and a weak-response regime dominated by damping. We show that this evolution can be explained by a simple two-dimensional sheet model that can be applied to a wide range of thin media.
尖锐的共振可以强烈改变物质的电磁响应。一个经典的例子是瑞利后向散射效应——在许多极性晶体的中红外附近,在光学声子共振附近具有高反射率。尽管这种在体材料中的效应已经被广泛研究,但对于有限厚度的系统处理仍然具有挑战性。在这里,我们通过实验和理论描述了六方氮化硼在超过 5 个数量级的厚度范围内的瑞利后向散射响应,厚度低至单层。我们发现,随着材料进入光学薄限,瑞利后向散射带的高反射率平台演变成一个单峰,在这个范围内出现了两个不同的区域:一个由相干辐射衰减主导的强响应区和一个由阻尼主导的弱响应区。我们表明,这种演化可以用一个简单的二维片模型来解释,该模型可以应用于广泛的薄介质。