Ramer Georg, Tuteja Mohit, Matson Joseph R, Davanco Marcelo, Folland Thomas G, Kretinin Andrey, Taniguchi Takashi, Watanabe Kenji, Novoselov Kostya S, Caldwell Joshua D, Centrone Andrea
Physical Measurement Laboratory, National Institute of Standards and Technology, 100 Bureau Dr., Gaithersburg, MD, 20899, USA; Maryland Nanocenter, University of Maryland, College Park, MD, 20742, USA.
Department of Mechanical Engineering, Vanderbilt University, 101 Olin Hall, Nashville, TN, 37212, USA.
Nanophotonics. 2020;9. doi: 10.1515/nanoph-2020-0048.
The anisotropy of hexagonal boron nitride (hBN) gives rise to hyperbolic phonon-polaritons (HPhPs), notable for their volumetric frequency-dependent propagation and strong confinement. For frustum (truncated nanocone) structures, theory predicts five, high-order HPhPs, sets, but only one set was observed previously with far-field reflectance and scattering-type scanning near-field optical microscopy. In contrast, the photothermal induced resonance (PTIR) technique has recently permitted sampling of the full HPhP dispersion and observing such elusive predicted modes; however, the mechanism underlying PTIR sensitivity to these weakly-scattering modes, while critical to their understanding, has not yet been clarified. Here, by comparing conventional contact- and newly developed tapping-mode PTIR, we show that the PTIR sensitivity to those weakly-scattering, high-Q (up to ≈280) modes is, contrary to a previous hypothesis, unrelated to the probe operation (contact or tapping) and is instead linked to PTIR ability to detect tip-launched dark, volumetrically-confined polaritons, rather than nanostructure-launched HPhPs modes observed by other techniques. Furthermore, we show that in contrast with plasmons and surface phonon-polaritons, whose -factors and optical cross-sections are typically degraded by the proximity of other nanostructures, the high- HPhP resonances are preserved even in high-density hBN frustum arrays, which is useful in sensing and quantum emission applications.
六方氮化硼(hBN)的各向异性产生了双曲线声子极化激元(HPhPs),其以与体积相关的频率传播和强限制为显著特征。对于截头圆锥体(截断纳米锥)结构,理论预测有五组高阶HPhPs,但之前通过远场反射和散射型扫描近场光学显微镜仅观察到一组。相比之下,光热诱导共振(PTIR)技术最近能够对完整的HPhP色散进行采样并观察到这些难以捉摸的预测模式;然而,PTIR对这些弱散射模式的灵敏度背后的机制,虽然对理解它们至关重要,但尚未得到阐明。在这里,通过比较传统的接触式和新开发的轻敲模式PTIR,我们表明,与先前的假设相反,PTIR对那些弱散射、高Q值(高达≈280)模式的灵敏度与探针操作(接触或轻敲)无关,而是与PTIR检测由尖端发射的暗的、体积受限的极化激元的能力有关,而不是与其他技术观察到的由纳米结构发射的HPhPs模式有关。此外,我们表明,与等离子体激元和表面声子极化激元不同,它们的品质因数和光学横截面通常会因其他纳米结构的靠近而降低,即使在高密度hBN截头圆锥体阵列中,高Q值的HPhP共振也能得以保留,这在传感和量子发射应用中很有用。