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左手材料中的非线性表面波。

Nonlinear surface waves in left-handed materials.

作者信息

Shadrivov Ilya V, Sukhorukov Andrey A, Kivshar Yuri S, Zharov Alexander A, Boardman Allan D, Egan Peter

机构信息

Nonlinear Physics Group, Research School of Physical Sciences and Engineering, Australian National University, Canberra ACT 0200, Australia.

出版信息

Phys Rev E Stat Nonlin Soft Matter Phys. 2004 Jan;69(1 Pt 2):016617. doi: 10.1103/PhysRevE.69.016617. Epub 2004 Jan 30.

Abstract

We study both linear and nonlinear surface waves localized at the interface separating a left-handed (LH) medium (i.e., a medium with both negative dielectric permittivity and negative magnetic permeability) and a conventional [or right-handed (RH)] dielectric medium. We demonstrate that the interface can support both TE- and TM-polarized surface waves-surface polaritons, and we study their properties. We describe the intensity-dependent properties of nonlinear surface waves in three different cases, i.e., when both the LH and RH media are nonlinear and when either of the media is nonlinear. In the case when both media are nonlinear, we find two types of nonlinear surface waves, one with the maximum amplitude at the interface, and the other one with two humps. In the case when one medium is nonlinear, only one type of surface wave exists, which has the maximum electric field at the interface, unlike waves in right-handed materials where the surface-wave maximum is usually shifted into a self-focusing nonlinear medium. We discuss the possibility of tuning the wave group velocity in both the linear and nonlinear cases, and show that group-velocity dispersion, which leads to pulse broadening, can be balanced by the nonlinearity of the media, so resulting in soliton propagation.

摘要

我们研究了局域于左手(LH)介质(即介电常数和磁导率均为负的介质)与常规[或右手(RH)]电介质界面处的线性和非线性表面波。我们证明该界面能够支持TE极化和TM极化的表面波——表面极化激元,并研究了它们的特性。我们描述了三种不同情况下非线性表面波的强度依赖特性,即当LH介质和RH介质均为非线性时,以及当其中任意一种介质为非线性时的情况。在两种介质均为非线性的情况下,我们发现了两种类型的非线性表面波,一种在界面处具有最大振幅,另一种有两个波峰。在其中一种介质为非线性的情况下,仅存在一种类型的表面波,其在界面处具有最大电场,这与右手材料中的波不同,在右手材料中表面波的最大值通常会向自聚焦非线性介质中移动。我们讨论了在线性和非线性情况下调节波群速度的可能性,并表明导致脉冲展宽的群速度色散可通过介质的非线性来平衡,从而实现孤子传播。

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