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Trapping light pulses at controlled perturbations in periodic optical structures

机译:在周期光学结构中以受控的扰动捕获光脉冲

摘要

A gap soliton can be controlled by introducing a perturbation into a waveguide structure that includes an otherwise essentially periodic variation of its refractive index. In one embodiment of our invention, by controlling the amplitude, phase and/or average value of the refractive index of a first perturbation, and by maintaining the speed of the soliton below a certain critical speed, we have found that the soliton will transfer its energy to the modes of the perturbation. When the soliton transfers essentially all of its energy in this way, we refer to the soliton as being trapped or captured by the perturbation. Surprisingly, the soliton can be trapped without loss of a significant amount of its energy. In an alternative embodiment, when the speed of the soliton exceeds the critical speed, a second perturbation is introduced into the waveguide structure to reduce the speed of the soliton, thereby enabling its capture by the first perturbation. In another embodiment, a gap soliton is captured between two perturbation regions neither of which is capable of capturing the soliton by itself. Trapped gap solitons enable a variety of unique system applications in, for example, memories, buffers, switches and WDM demultiplexers.
机译:可以通过将扰动引入波导结构来控制间隙孤子,该波导结构包括其折射率的否则基本上周期性的变化。在本发明的一个实施例中,通过控制第一扰动的折射率的幅度,相位和/或平均值,并且通过将孤子的速度保持在某个临界速度以下,我们发现了孤子将转移其能量的摄动模式。当孤子以这种方式基本转移其所有能量时,我们将孤子称为被扰动捕获或捕获。出人意料的是,孤子可以被捕获而不会损失大量能量。在替代实施例中,当孤子的速度超过临界速度时,第二扰动被引入到波导结构中以减小孤子的速度,从而使得能够通过第一扰动来捕获孤子。在另一个实施例中,间隙孤子被捕获在两个扰动区域之间,这两个扰动区域都不能够单独捕获孤子。陷波间隙孤子可以在例如存储器,缓冲器,开关和WDM多路分解器中实现各种独特的系统应用。

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