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调制的PT对称波导阵列中的边缘和体耗散孤子

Edge and bulk dissipative solitons in modulated PT-symmetric waveguide arrays.

作者信息

Kartashov Yaroslav V, Vysloukh Victor A

出版信息

Opt Lett. 2019 Feb 15;44(4):791-794. doi: 10.1364/OL.44.000791.

DOI:10.1364/OL.44.000791
PMID:30767988
Abstract

We address dissipative soliton formation in modulated parity-time (PT)-symmetric continuous waveguide arrays composed from waveguides with amplifying and absorbing sections, whose density gradually increases (due to decreasing waveguide separation) either towards the center of the array or towards its edges. In such a structure, the level of gain/loss at which PT-symmetry gets broken depends on the direction of increase of waveguide density. Breakup of PT-symmetry occurs when eigenvalues of modes localized in the region where waveguide density is largest collide and move into a complex plane. In this regime of broken symmetry, the inclusion of focusing Kerr-type nonlinearity of the material and weak two-photon absorption allows to arrest the growth of amplitude of amplified modes and may lead to the appearance of stable attractors either in the center or at the edge of the waveguide array, depending on the type of array modulation. Such solitons can be stable; they acquire specific triangular shapes and notably broaden with increase of gain/loss level. Our results illustrate how spatial array modulation that breaks PT-symmetry "locally" can be used to control the specific location of dissipative solitons forming in the array.

摘要

我们研究了由具有放大和吸收段的波导组成的调制奇偶时间(PT)对称连续波导阵列中的耗散孤子形成,这些波导的密度朝着阵列中心或边缘逐渐增加(由于波导间距减小)。在这种结构中,PT对称性被打破时的增益/损耗水平取决于波导密度增加的方向。当局域在波导密度最大区域的模式的本征值发生碰撞并进入复平面时,PT对称性就会破裂。在这种对称性破缺的情况下,考虑材料的聚焦克尔型非线性和弱双光子吸收,可以抑制放大模式振幅的增长,并可能导致在波导阵列的中心或边缘出现稳定吸引子,这取决于阵列调制的类型。这种孤子可以是稳定的;它们呈现出特定的三角形形状,并随着增益/损耗水平的增加而显著展宽。我们的结果说明了如何利用“局部”打破PT对称性的空间阵列调制来控制阵列中形成的耗散孤子的特定位置。

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