Second Harmonic and Sum Frequency Generation in Sub-Micron 3D Photonic Crystal Microcavities

J. F. Young, M. Mccutcheon, G. Rieger, D. Dalacu, S. Frederick, P. Poole, Robin L. Williams
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Abstract

The second harmonic radiation emitted into the top half space from three dimensionally localized modes of L3 defect cavities in InP-based planar photonic crystals is studied using both CW and pulsed excitation. The far field harmonic radiation patterns observed from modes with resonant wavelengths ~ 1550 nm, excited by a tunable CW laser with less than 1 mW power, reveal strong local field enhancement (> 1000 X). A detailed comparison with FDTD modeling allows us to conclude that the bulk InP second order susceptibility tensor dominates the second order response of these microcavities. When a broadband, sub picoseconds source is used to simultaneously excite two of the microcavity modes, the harmonic spectrum in general consists of three contributions, the second harmonic from each of the excited modes, and a third peak due to the second order (sum frequency) mixing of the two modes. By using short and long pulse excitation simultaneously, we demonstrate how the emission frequency due to sum frequency processes can be used to continuously tune the harmonic emission frequency dependent on the occupation of various cavity modes.
亚微米三维光子晶体微腔中二次谐波和和频的产生
利用连续波激发和脉冲激发,研究了基于inp的平面光子晶体中L3缺陷腔三维局域模式向上半空间发射的二次谐波辐射。在谐振波长~ 1550 nm的模式下,在功率小于1 mW的可调谐连续波激光激发下,远场谐波辐射图显示出强的局部场增强(> 1000倍)。通过与FDTD模型的详细比较,我们可以得出这样的结论:体InP二阶磁化率张量主导了这些微腔的二阶响应。当使用宽带亚皮秒源同时激发两个微腔模式时,谐波谱通常由三个贡献组成,即每个激励模式的二次谐波,以及两个模式的二阶(和频率)混合产生的第三个峰。通过同时使用短脉冲和长脉冲激励,我们演示了如何利用和频过程产生的发射频率,根据不同腔模的占用情况,连续调谐谐波发射频率。
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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