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Applicability of theoretical approaches for dispersion managed solitons

机译:理论方法在色散管理孤子中的适用性

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We present here recent results on dispersion management for non-linear return-to-zero pulse propagation in optical fibers. The main purpose of dispersion management is to reduce several effects such as radiation from the pulse due to lumped amplifiers compensating dispersion loss, modulational instability, jitters caused by the collisions between signals in different channels of wavelength-division-multiplexed (WDM) systems, the Gordon-Haus effect resulting from the interaction with noise, and to set a desired average value of dispersion. Additionally, DM solitons present a possibility of upgrading installed systems (see for example the UPGRADE project). The so-called dispersion managed soliton can be studied by different methods, which are compared and extended in the present paper. Those methods can generally be applied to general dispersion maps, but we particularize here to the case of a two-step dispersion map, of average dispersion D_(av), dispersion difference ΔD and of period Z_d. The Z = 0 point is at the center of the positive (or higher) dispersion fiber. Our model equation is iu_Z + D(Z)u_(TT/2 + S(Z)|u|~2u = 0, the nonlinear Schroedinger equation (NLSE). It can incorporate loss and amplification through S(Z) (see for example). This equation can be rescaled by three parameters acting on T,Z,u,D or S, but we do not impose conditions on them yet as they will be useful later. This NLSE admits some conservation laws: three trivial ones being the energy ∫ |u|~2dT, the moment i ∫ uu~*_TdT and the "Hamiltonian" H = 1/2 ∫ [S|u|~4 - D|u_T|~2]dT, this last one being only valid when both the dispersion and the non-linearities are constants (in which case there are an infinite number of conserved quantities). A test of validity of the different methods exposed here is to see how they conserve, or don't, those quantities.
机译:我们在此介绍有关光纤中非线性归零脉冲传播的色散管理的最新结果。色散管理的主要目的是减少多种影响,例如,由于集总放大器补偿了色散损耗,调制不稳定性,由波分多​​路复用(WDM)系统的不同通道中的信号之间的冲突引起的抖动引起的脉冲辐射。 Gordon-Haus效应是由与噪声的相互作用引起的,并设置了期望的色散平均值。此外,DM孤子还可以升级已安装的系统(例如,参见UPGRADE项目)。所谓的色散管理孤子可以通过不同的方法来研究,在本文中进行了比较和扩展。这些方法通常可以应用于一般色散图,但是在此我们将具体说明两步色散图的情况,即平均色散D_(av),色散差ΔD和周期Z_d。 Z = 0点位于正(或更高)色散光纤的中心。我们的模型方程为iu_Z + D(Z)u_(TT / 2 + S(Z)| u |〜2u = 0,这是非线性Schroedinger方程(NLSE)。它可以包含通过S(Z)引起的损耗和放大(请参见参考资料可以用作用在T,Z,u,D或S上的三个参数来重新定标该方程式,但我们尚未对其施加条件,因为它们稍后将有用。该NLSE接受了一些守恒定律:三个平凡的定律能量∫| u |〜2dT,时刻i∫uu〜* _TdT和“哈密顿” H = 1/2∫[S | u |〜4-D | u_T |〜2] dT当色散和非线性均是常数时有效(在这种情况下,存在无限数量的守恒量)。这里公开的不同方法的有效性检验是看它们如何保留或不保留那些量。

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