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ROUND-TRIP MODEL OF QUADRATIC CAVITY SOLITON TRAPPING

机译:二次腔孤子圈圆模型

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In recent years a considerable interest has been focused on theoretical and experimental studies of spatial dissipative structures in nonlinear optical resonators. Cavity soliton (CS) can be created and destroyed by localised pulses of light, and can thus be used to store images or information. The ability to control and manipulate CS has been proposed in the pioneering paper for the case of two-level medium. The problem of stationary soliton solution has been numerically and analytically investigated mostly in the case of the semiconductor optical resonators and cubic nonlinear cavity. Note that the quadratic non- inearity provides a wide range of new opportunities. For instance, the threshold of pattern formation in a degenerate OPO was considered. Some authors concentrate their attention on the CS interaction. The problem of soliton stability in OPO is discussed in. The most complicated case of SHG configuration with driving fieid corresponding to the fundamental frequency (FF) was studied in. It was found that the quadratic CS can appear due to modulation instability of the steady-state solution. It should be emphasized that trapping dynamics of CS is not investigated sufficiently. The authors of all papers mentioned above used the mean-field approach valid for the case of negligibly small variations of harmonic parameters in a round-trip time. However, to study spatial quadratic solitons dynamics in a long cavity with essential losses and detunings, it is necessary to develop more adequate theory than the mean-field model. For instance, it is important in the case of ring cavity considered in. In this paper we study intracavity quadratic solitons by means of numerical modelling based on the round-trip approach. In the frameworks of this model the bulk medium equations for forward and backward waves are used. In the case of stationary plane wave solution we compare the results obtained for both round-trip and mean-field models. A domain of cavity fines where the mean-field approach is valid was numerically investigated. Trapping time has been shown to decrease due to the inclination of seeded beam. The critical angle depending on the seeded beam width was obtained.
机译:近年来,相当大的兴趣已集中在非线性光学谐振器中的空间耗散结构的理论和实验研究上。腔孤子(CS)可以通过局部光脉冲来创建和破坏,因此可以用来存储图像或信息。在开创性论文中,针对两层介质,已经提出了控制和操纵CS的能力。静态孤子解的问题已经在数值和分析上进行了研究,主要是在半导体光谐振器和立方非线性腔的情况下。请注意,二次非earearness提供了广泛的新机会。例如,考虑了退化的OPO中图案形成的阈值。一些作者将注意力集中在CS交互上。讨论了OPO中孤子稳定性的问题。研究了最复杂的SHG配置,其驱动电场对应于基频(FF)。发现二次CS可能是由于稳态的调制不稳定性而出现的。状态解决方案。应该强调的是,对CS的俘获动力学的研究还不够充分。上面提到的所有论文的作者都使用了均值场方法,这种方法适用于在往返时间内谐波参数的微小变化可忽略不计的情况。但是,要研究具有实质性损耗和失谐的长腔中的空间二次孤子动力学,有必要发展比均值场模型更充分的理论。例如,在考虑环形腔的情况下,这一点很重要。在本文中,我们通过基于往返方法的数值模型研究腔内二次孤子。在该模型的框架中,使用了正向和反向波的体介质方程。在平稳平面波解的情况下,我们比较了往返模型和均场模型的结果。数值研究了平均场法有效的型腔区域。已经显示,由于播种束的倾斜,陷印时间减少了。获得取决于种子束宽度的临界角。

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