Higher order solitons in non-paraxial optics

D. Dakova, V. Slavchev, A. Dakova, L. Kovachev, I. Bozhikoliev
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引用次数: 1

Abstract

In last two decades actively are studied the phenomena resulting from the evolution of ultrashort optical pulses in nonlinear dispersive media. The well-known (1+1D) nonlinear Schrödinger equation (NSE) describes very well the propagation of narrow-band optical pulses (Δω<<ω0). Nowadays, it is quite easy to obtain broad-band phase-modulated femtosecond laser pulses or to reach the attosecond region where Δω≈ω0. To explore their behavior it is necessary to use the more general nonlinear amplitude equation (NAE). In local time coordinate system it differs from the standard NSE with two additional non-paraxial terms. In present paper, by using the NAE, it is investigated the dynamics of higher order non-paraxial solitons. It is shown that the peak of soliton is linearly shifted in time domain. This temporal shift is observed in the frames of non-paraxial optics, even when the higher order nonlinear and dispersive effects are neglected.
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非近轴光学中的高阶孤子
近二十年来,人们对非线性色散介质中超短光脉冲的演化现象进行了积极的研究。众所周知的(1+1D)非线性Schrödinger方程(NSE)很好地描述了窄带光脉冲(Δω<<ω0)的传播。目前,获得宽带相位调制飞秒激光脉冲或达到Δω≈ω0的阿秒区域是很容易的。为了探究它们的行为,有必要使用更一般的非线性振幅方程(NAE)。在地方时坐标系中,它与标准NSE有两个附加的非近轴项不同。本文利用NAE研究了高阶非副轴孤子的动力学。结果表明,孤子的峰值在时域上呈线性位移。即使忽略高阶非线性和色散效应,也可以在非傍轴光学的框架中观察到这种时间位移。
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