Multilayer, Nonlinear Arrow Waveguides for Surface Emitted Sum-Frequency Mixing

R. Normandin, H. Dai, S. Janz, A. Delâge, J. Brown, F. Chatenoud
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Abstract

When used with conventional communication optical fibers, with a typical core diameter of 8µm, conventional channel waveguides geometries need to present similar thicknesses for good mode overlaps between the two. This has been a difficult goal to achieve with semiconductor waveguides due to their high index of refraction. The waveguides were typically much thinner than the fiber core and, consequently, input efficiencies were quite low. This problem was addressed some time ago with the demonstration of the antiresonant reflecting waveguide (ARROW) geometry(1). Although these are intrinsically leaky waveguides quite acceptable losses were feasible in silicon(2) and GaAs(3) geometries. On the other hand when dealing with nonlinear interactions in semiconductor waveguides, it was realised quickly that in other to maintain acceptable overall efficiencies the waveguide thickness had to be kept unreasonably small (4). This obviously led to input coupling difficulties. In our previous work, presented two years ago at this topical meeting (5), we demonstrated a new multilayer AIGaAs waveguide geometry with surface harmonic emission efficiencies well above what was possible in uniform films. This led to the development of several devices (6,7) such as correlators, spectrometers and intracavity diode laser second harmonic generators(8). However, little attention has been given to the problem of fiber input coupling to the nonlinear waveguide. We present the first results, to our knowledge, of multi-layer core ARROW waveguides and their use in nonlinear harmonic generation. There has been little mention of the ARROW geometry in a nonlinear context, with the recent exception of inter-guide coupling(9), since they tend to be thick guiding structures.
用于表面发射和频混合的多层非线性箭头波导
当与传统通信光纤一起使用时,典型的芯径为8 μ m,传统通道波导的几何形状需要呈现相似的厚度,以实现两者之间良好的模式重叠。由于半导体波导的高折射率,这一直是一个难以实现的目标。波导通常比光纤芯薄得多,因此,输入效率相当低。这个问题在前一段时间通过反谐振反射波导(箭头)几何(1)的演示得到了解决。虽然这些本质上是漏波导,但在硅(2)和砷化镓(3)几何结构中,可接受的损耗是可行的。另一方面,当处理半导体波导中的非线性相互作用时,人们很快意识到,为了保持可接受的整体效率,波导厚度必须保持不合理的小(4)。这显然会导致输入耦合困难。在我们之前的工作中,在两年前的专题会议上,我们展示了一种新的多层AIGaAs波导几何结构,其表面谐波发射效率远高于均匀薄膜。这导致了几个设备的发展(6,7),如相关器,光谱仪和腔内二极管激光二次谐波发生器(8)。然而,对非线性波导的光纤输入耦合问题的研究却很少。我们提出了第一个结果,据我们所知,多层核心箭头波导及其在非线性谐波产生中的应用。除了最近的导轨间耦合(9)外,在非线性环境中很少提到ARROW几何结构,因为它们往往是厚的导向结构。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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