Probing the ultrathin limit of hyperbolic metamaterial: nonlocality induced topological transitions (Presentation Recording)

Long Chen, Cheng Zhang, Jing Zhou, L. Guo
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引用次数: 1

Abstract

An ideal hyperbolic metamaterial (HMM), which has a perfect hyperbolic dispersion curve, theoretically can support modes with indefinite wavenumbers, leading to large photon local density of states (LDOS) and many applications such as enhancing light-matter interactions, spontaneous emission and thermal radiation. Here in this presentation, HMMs based on ultrathin metal-dielectric multilayers have been studied by considering the nonlocal response of electrons in metal. Based on the hydrodynamic model of the nonlocal response, we investigate the effect of nonlocality on the performance (dispersion relation, ray refraction, LDOS and spontaneous emission) of HMMs when gradually approaching the ultrathin limit of the unit cell. We show that nonlocality will induce topological transitions of the iso-frequency surfaces and limit the wavenumber as well as LDOS for both type I and type II HMMs. Under nonlocal treatment, the iso-frequency surface of type II HMM transforms from a hyperbola to a bullet shape, while for type I HMM, the surface splits into two branches: a cylindrical-like branch at high k region and an elliptical branch at the low k region. In the high k region, the nonlocality set a cut-off k for the allowed wavenumbers in both type I and type II HMMs. This cut-off k which is defined by the electron Fermi velocity of the metal intrinsically limits the LDOS and light-matter interactions. These results indicate that in the aim of achieving high performance HMMs, merely thinning the constituent films according to the local theories is no longer valid.
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探索双曲超材料的超薄极限:非定域诱导的拓扑跃迁(演讲记录)
理想双曲超材料(HMM)具有完美的双曲色散曲线,理论上可以支持无限波数模式,从而导致大的光子局域态密度(LDOS),并在增强光-物质相互作用、自发发射和热辐射等方面有许多应用。本文通过考虑金属中电子的非局域响应,研究了基于超薄金属-介电层的hmm。基于非局域响应的流体动力学模型,研究了非局域性对薄膜材料在逐渐接近单晶超薄极限时的性能(色散关系、射线折射、LDOS和自发发射)的影响。我们发现非局域性会引起等频表面的拓扑跃迁,并限制了I型和II型hmm的波数和LDOS。在非局部处理下,II型HMM的等频曲面由双曲线转变为子弹形,而I型HMM的等频曲面在高k区域分裂为圆柱状分支,在低k区域分裂为椭圆状分支。在高k区域,非局部性为I型和II型hmm中的允许波数设置了截止k。这个由金属的电子费米速度定义的截止k本质上限制了LDOS和光物质相互作用。这些结果表明,为了实现高性能hmm,仅仅根据局部理论减薄组成膜已不再有效。
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