Generation of two colliding pulses with tunable THz-range frequency difference in high-nonlinear photonic crystal fiber

Y. Mazhirina, L. Melnikov, A. Konukhov
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Abstract

Two-wavelength light sources are of interest for THz-range oscillators based on difference frequency generation [1–5], and also for the oscillators, based on the optical rectification [6]. Easy way to produce pulses with frequency difference is the use of dispersion oscillating fiber [7]. We discuss the possibility to use a highly nonlinear photonic crystal fiber for generation the overlapping pulse pairs with the difference of carrier frequencies in THz range from femtosecond pulses train from only one laser. First, each pulse from the laser should be duplicated using beamsplitter. Then the pulses should be launched sequently into photonic crystal fiber. The pulse frequency is to be in anomalous dispersion regions, and pulses are to be high-order solitons. Due to Raman effect these solitons split to fundamental soliton with red shift and other smaller pulses with nonshifted frequency. Due to group velocity dispersion (GVD) the Raman-shifted pulse propagate slower depending on pulse parameters. Thus there exist some definite length in the fiber where Raman-shifted pulse collides with unshifted pulse. This distance and the value of the shift can be controlled by pulse parameters and depend on the fiber parameters. The results of numerical modeling of the nonlinear propagation of multi-soliton pairs of pulses in photonic crystal fiber are presented below.
高非线性光子晶体光纤中两种频率差可调的碰撞脉冲的产生
基于差频产生的太赫兹范围振荡器[1-5]和基于光学整流的振荡器[6]都对双波长光源感兴趣。产生频差脉冲的简单方法是使用色散振荡光纤[7]。讨论了利用高度非线性光子晶体光纤从单束激光发出的飞秒脉冲串产生载流子频率差在太赫兹范围内重叠脉冲对的可能性。首先,应该使用分束器复制激光的每个脉冲。然后将脉冲依次发射到光子晶体光纤中。脉冲频率在异常色散区,脉冲是高阶孤子。由于拉曼效应,这些孤子分裂为具有红移的基本孤子和其他频率未移位的较小脉冲。由于群速度色散(GVD),拉曼位移脉冲的传播速度随脉冲参数的变化而变慢。因此在光纤中存在一定长度的拉曼位移脉冲与未位移脉冲的碰撞。这个距离和位移值可以由脉冲参数控制,并取决于光纤参数。本文给出了脉冲多孤子对在光子晶体光纤中非线性传播的数值模拟结果。
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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