School of Physics and Technology, Center for Nanoscience and Nanotechnology, and Key Laboratory of Artificial Micro- and Nano-structures of Ministry of Education, Wuhan University , Wuhan 430072, China.
The Institute for Advanced Studies, Wuhan University , Wuhan 430072, China.
Nano Lett. 2017 Dec 13;17(12):7803-7808. doi: 10.1021/acs.nanolett.7b04016. Epub 2017 Nov 21.
Coherently adding up signal wave from different locations are a prerequisite for realizing efficient nonlinear optical processes in traditional optical configurations. While nonlinear optical processes in plasmonic waveguides with subwavelength light confinement are in principle desirable for enhancing nonlinear effects, so far it has been difficult to improve the efficiency due to the large momentum mismatch. Here we demonstrate, using remotely excited surface plasmon polaritons (SPPs), axial collimated but transversely divergent second harmonic (SH) generation in a single silver nanowire-monolayer molybdenum disulfide hybrid system. Fourier imaging of the generated SH signal confirms the momentum conservation conditions between the incident and reflected SPPs and reveals distinct features inherent to the 1D plasmonic waveguides: (i) the SH photons are collimated perpendicular to the nanowire axis but are divergent within the perpendicular plane; (ii) the collimation (divergence) is inversely proportional to the length of the active region (lateral confinement of the SPPs); and (iii) the SH emission pattern resembles that of an aligned dipole chain on top of the substrate with an emission peak at the critical angle. Our results pave the way to generate and manipulate SH emission around subwavelength waveguides and open up new possibilities for realizing high efficiency on-chip nonlinear optics.
从不同位置相干地叠加信号波是在传统光学结构中实现有效非线性光学过程的前提。虽然在亚波长光限制的等离子体波导中进行非线性光学过程在增强非线性效应方面是理想的,但由于动量失配大,迄今为止一直难以提高效率。在这里,我们使用远程激发的表面等离激元(SPP),在单个银纳米线-单层二硫化钼杂化系统中实现轴向准直但横向发散的二次谐波(SH)产生。所产生的 SH 信号的傅里叶成像证实了入射和反射 SPP 之间的动量守恒条件,并揭示了 1D 等离子体波导固有的独特特征:(i)SH 光子在垂直于纳米线轴的方向上准直,但在垂直平面内发散;(ii)准直(发散)与活性区域的长度(SPP 的横向限制)成反比;(iii)SH 发射图案类似于在衬底顶部排列的偶极子链,在临界角处有一个发射峰。我们的结果为在亚波长波导周围产生和控制 SH 发射铺平了道路,并为实现高效的片上非线性光学开辟了新的可能性。