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Spatiotemporal solitary modes in a twisted cylinder waveguide shell with the self-focusing Kerr nonlinearity

机译:具有自聚焦Kerr非线性的扭曲圆柱波导壳中的时空孤立模

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We study the spatiotemporal solitary modes that propagate in a hollow twisted cylinder waveguide pipe with a self-focusing Kerr nonlinearity. Three generic solitary modes, one belonging to the zero-harmonic (OH) and the other two belonging to the first-harmonic (1H), are found in the first rotational Brillouin zone. The OH solitary modes can be termed as a quasi-1D (one-dimensional) temporal soliton. Their characteristics depend only on the energy flow. The 1H solitary mode can be termed a quasi-2D (two-dimensional) bullet, whose width is much narrower than the angular domain of the waveguide. In contrast to the OH mode, the characteristics of the 1H solitary mode depend on both their energy flow and the rotating speed of the waveguide. We demonstrate numerically that the 1H solitary modes are stable when their energy flow is smaller than the threshold norm of the Townes soliton. The boundaries of the bistable area for these two types of solitary modes are predicted by the analyses via two-mode approximation. This prediction is in accordance with the numerical findings. We also demonstrate analytically that the 1H solitary mode of this system can be applied to emulate the nonlinear dynamics of solitary modes with 1D Rashba spin-orbit (SO) coupling by optics. Two degenerated states of the 1H solitary mode, semi-dipole and mixed mode, are found from this setting via the mechanism of SO coupling. Collisions between the pair of these two types of solitary modes are also discussed in the paper. The pair of the OH solitary mode features only the elastic collision, whereas the pair of 1H solitary modes can feature both elastic and inelastic collision when the total energy flow of the two modes are smaller or close to the threshold norm of the Townes soliton. (C) 2018 Elsevier B.V. All rights reserved.
机译:我们研究具有自聚焦Kerr非线性的中空扭曲圆柱波导管道中传播的时空孤立模式。在第一个旋转布里渊区中发现了三种通用的孤立模式,一个属于零谐波(OH),另外两个属于一阶谐波(1H)。 OH孤立模式可以称为准1D(一维)时间孤子。它们的特性仅取决于能量流。 1H孤立模式可以称为准2D(二维)子弹,其宽度比波导的角域窄得多。与OH模式相反,1H单独模式的特性取决于它们的能量流和波导的旋转速度。我们用数值方法证明,当1H孤立模式的能量流小于Townes孤子的阈值范数时,它们是稳定的。通过两种模式的近似分析,可以预测这两种类型的孤立模式的双稳态区域的边界。该预测与数值结果一致。我们还分析地证明,该系统的1H孤模可以应用于通过光学将一维Rashba自旋轨道(SO)耦合模拟孤模的非线性动力学。通过SO耦合的机理从该设置中发现了1H孤模式的两个简并状态,即半偶极子模式和混合模式。本文还讨论了这两种类型的孤立模式中的一对之间的冲突。一对OH孤模式仅具有弹性碰撞,而当一对1H孤模式的总能量流小于或接近Townes孤子的阈值范数时,一对1H孤模式可以同时具有弹性和非弹性碰撞。 (C)2018 Elsevier B.V.保留所有权利。

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