级联二次谐波产生中的色散波

M. Bache, O. Bang, W. Krolikowski, F. Wise
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引用次数: 0

摘要

光孤子是一种非色散非线性波,通过群速度色散(GVD)和非线性之间的平衡来支撑。所谓的色散波是与这些孤子相位匹配的线性波,并且经常在超连续体产生中发现[1,2]。色散波波长可以从相位匹配条件预测到孤子波[3]。这个相位匹配点通常被解释为位于不再支持孤子的地方,即GVD改变符号的地方。然而,在现实中,色散波是在产生的孤子的总色散为变号的波长处发现的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Dispersive waves in fs cascaded second-harmonic generation
Optical solitons are nondispersive nonlinear waves that are supported through a balance between group-velocity dispersion (GVD) and nonlinearity. The so-called dispersive waves are linear waves phase-matched to these solitons, and are often found in supercontimuum generation [1, 2]. The dispersive wave wavelength can be predicted from a phase-matching condition to the solitonic wave [3]. This phase-matching point is often interpreted as being located where solitons are no longer supported, i.e. where the GVD changes sign. However, in reality the dispersive wave is found at the wavelength where the total dispersion of the generated soliton is changing sign.
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