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Surface Polariton-Like s-Polarized Waveguide Modes in Switchable Dielectric Thin Films on Polar Crystals

机译:极性晶体上可切换介电薄膜中的表面极化类似s极化的波导模式

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摘要

Surface phonon polaritons (SPhPs) and surface plasmon polaritons (SPPs), evanescent modes supported by media with negative permittivity, are a fundamental building block of nanophotonics. These modes are unmatched in terms of field enhancement and spatial confinement, and dynamical all-optical control can be achieved, e.g., by employing phase-change materials. However, the excitation of surface polaritons in planar structures is intrinsically limited to p-polarization. On the contrary, waveguide modes in high-permittivity films can couple to both p- and s-polarized light, and in thin films, their confinement can become comparable to surface polaritons. Here, it is demonstrated that the s-polarized waveguide mode in a thin Ge3Sb2Te6 (GST) film features a similar dispersion, confinement, and electric field enhancement as the SPhP mode of the silicon carbide (SiC) substrate, while even expanding the allowed frequency range. Moreover, it is experimentally shown that switching the GST film grants nonvolatile control over the SPhP and the waveguide mode dispersions. An analytical model is provided for the description of the GST/SiC waveguide mode and it is shown that the concept is applicable to the broad variety of polar crystals throughout the infrared spectral range. As such, complementarily to the polarization-limited surface polaritons, the s-polarized waveguide mode constitutes a promising additional building block for nanophotonic applications.
机译:表面声子极化子(SPhPs)和表面等离激元极化子(SPPs)是具有负介电常数的介质所支持的渐逝模式,是纳米光子学的基本组成部分。这些模式在场增强和空间限制方面是无与伦比的,并且可以例如通过使用相变材料来实现动态全光控制。但是,平面结构中表面极化子的激发本质上仅限于p极化。相反,高介电常数薄膜中的波导模式可以耦合到p偏振和s偏振光,而在薄膜中,其局限性可以与表面极化子媲美。在此证明,Ge3Sb2Te6(GST)薄膜中的s极化波导模式具有与碳化硅(SiC)衬底的SPhP模式相似的色散,约束和电场增强,甚至扩展了允许的频率范围。此外,实验表明,切换GST膜可对SPhP和波导模式色散进行非易失性控制。提供了用于描述GST / SiC波导模式的分析模型,结果表明该概念适用于整个红外光谱范围内的多种极性晶体。这样,作为偏振受限的表面极化子的补充,s极化波导模式构成了纳米光子应用中有希望的附加构件。

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