半导体中适当色散裁剪是形成孤子的先决条件

U. Peschel, T. Peschel, F. Lederer
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引用次数: 0

摘要

具有聚焦非线性的材料中存在明亮孤子需要异常色散(GVD < 0),在超过零色散波长的熔融石英光纤中可以满足这一条件。不幸的是,由于半导体的非共振非线性(低于带隙的一半)表现出巨大的正常GVD (D≈1000ps2/km),从而阻止了明亮孤子的形成,因此对全光学元件相当有吸引力。因此,有很大的兴趣来确定智能设备的概念,允许错误的材料分散的过度补偿。这些概念可以用来避免非线性AlGaAs定向耦合器中实验观察到的脉冲破裂,通过使用时间孤子[1]。此外,时空物体(光弹)[2]也可以研究,因为在适当设计的平面波导结构中,衍射、异常色散和聚焦非线性会发生所需的相互作用。由于半导体波导的器件长度被限制在2英寸左右,因此当脉冲长度为几百秒时,异常色散应超过数千ps2/km。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Proper Dispersion Tailoring in Semiconductors as Prerequisite for Soliton Formation
Bright solitons to exist in materials with a focusing nonlinearity require an anomalous dispersion (GVD < 0). This condition can be met in fused silica fibers beyond the zero-dispersion wavelength. Unfortunately, semiconductors that are fairly attractive for all-optical elements because of their large off-resonant nonlinearities (below half the band gap) exhibit a huge normal GVD (D≈1000ps2/km) thus prohibiting the formation of bright solitons. Hence, there is a great deal of interest to identify smart device concepts that allow for the overcompensation of the wrong material dispersion. Such concepts could be used to avoid the experimentally observed pulse break up in nonlinear AlGaAs directional couplers by using temporal solitons [1]. Moreover, spatio-temporal objects (light bullets) [2] could be studied because the required interplay of diffraction, anomalous dispersion and focusing nonlinearity would occur in properly designed planar waveguide structures. Because the device length of semiconductor waveguides is limited to about 2" the anomalous dispersion should exceed some thousands of ps2/km for pulse lengths of some hundred fs.
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