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    • 32. 发明授权
    • Article comprising an optical pulse compressor
    • 一种光脉冲压缩机
    • US06163638A
    • 2000-12-19
    • US181728
    • 1998-10-29
    • Benjamin John EggletonGadi Lenz
    • Benjamin John EggletonGadi Lenz
    • G02F1/35G02B6/34H04B10/18
    • G02B6/02085G02B6/29322H04B10/25077
    • Optical pulse compression is of importance in very high bit rate optical fiber communication systems. We are disclosing an adiabatic optical pulse compressor that can achieve substantial compression by means of a relatively short (e.g., about 100 cm) chirped periodic structure, exemplarily an apodized and chirped fiber Bragg grating. The input pulse to the periodic structure typically are not soliton pulses, but the passage through the periodic structure results in transformation of the pulses into substantially transform-limited soliton pulses that are available (typically after appropriate modification) for transmission through conventional optical fiber towards utilization means. The input pulses can be generated by any applicable method, e.g., by combining the cw outputs of two lasers that differ with regard to the frequency of their output.
    • 光脉冲压缩在非常高的比特率光纤通信系统中是重要的。 我们公开了一种绝热的光脉冲压缩机,其可以通过相对较短的(例如约100cm)的啁啾周期结构实现实质压缩,示例性地是变迹和啁啾的光纤布拉格光栅。 到周期性结构的输入脉冲通常不是孤子脉冲,但是通过周期性结构的通过导致脉冲变换为可用的(通常在适当的修改之后)的基本上变换限制的孤子脉冲,用于通过常规光纤传输到利用 手段。 可以通过任何适用的方法产生输入脉冲,例如通过组合两个激光器的输出相对于其输出频率而不同的cw输出。
    • 33. 发明授权
    • Optical pulse compressor for optical communications systems
    • 光通信系统光脉冲压缩机
    • US6108474A
    • 2000-08-22
    • US989093
    • 1997-12-11
    • Benjamin John EggletonGadi Lenz
    • Benjamin John EggletonGadi Lenz
    • G02B6/02G02F1/35G02F1/365H01S3/00H04J14/08
    • G02F1/365H01S3/0057
    • In accordance with the invention, an optical pulse compressor comprises a pulse source, a section of nonlinear optical waveguide including a periodic structure, such as a Bragg grating, for providing positive dispersion and a section of linear optical waveguide including a negative dispersion component. The nonlinear waveguide should have a second order index N.sub.2 at least ten times the second order index N.sub.2 ' of the linear waveguide. The nonlinear waveguide is preferably chalcogenide fiber, with a Bragg grating photoinduced into the core. Because the grating is 4-5 orders of magnitude more dispersive than standard optical fiber, the length of the nonlinear waveguide section can be scaled down to a few centimeters with accompanying reduction of deleterious processes. Modeling suggests that compression factors of 5 with an initial 60 ps pulse are achievable with grating lengths of about 20 cm.
    • 根据本发明,光脉冲压缩机包括脉冲源,包括诸如布拉格光栅的周期性结构的非线性光波导的一部分,用于提供正色散和包括负色散分量的一段线性光波导。 非线性波导应该具有至少十倍于线性波导的二阶索引N2'的二阶索引N2。 非线性波导优选是硫族化物纤维,其中布拉格光栅光致激发成核心。 由于光栅与标准光纤相比分散性高4-5个数量级,因此随着减少有害过程,非线性波导部分的长度可以缩小到几厘米。 建模表明,采用初始60 ps脉冲的压缩因子为5,光栅长度约为20 cm。