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    • 1. 发明申请
    • ALL-OPTICAL SIGNAL REGENERATION
    • 全光信号再生
    • WO2005109714A1
    • 2005-11-17
    • PCT/US2005/015921
    • 2005-05-03
    • CORNING INCORPORATEDEVANS, Alan FKUKSENKOV, Dmitri V
    • EVANS, Alan FKUKSENKOV, Dmitri V
    • H04J14/02
    • H04B10/299H04J14/0227H04J14/0241
    • An all-optical method of regenerating an optical return-to-zero format pulse signal of a first wavelength starts by introducing the input signal into a first end of a non-linear optical fiber to obtain a modified signal comprising pulses broadened in the wavelength domain. When this modified signal emerges from the second end of said non-linear optical fiber, a bandwidth slice is selected that is centered on a second wavelength so spaced from the first wavelength that its intensity is substantially unresponsive to weak pulses in the signal and relatively insensitive to intensity for other pulses. This slice is returned to the same non-linear optical fiber at its second end so that a further modified signal comprising pulses broadened in the wavelength domain will emerge from its first end. From this further modified signal a bandwidth slice centered on the first wavelength is selected as regenerated output. Regenerators operating in this way are also disclosed.
    • 通过将输入信号引入非线性光纤的第一端来重新生成第一波长的光返回到零格式的脉冲信号的全光学方法,以获得包括波长范围扩大的脉冲的修改信号 。 当该修改的信号从所述非线性光纤的第二端出现时,选择以与第一波长间隔的第二波长为中心的带宽片,其强度对信号中的弱脉冲基本上不响应,并且相对不敏感 到其他脉冲的强度。 该片在其第二端返回到相同的非线性光纤,使得包括在波长域中扩展的脉冲的另外修改的信号将从其第一端出现。 从该进一步修改的信号中选择以第一波长为中心的带宽切片作为再生输出。 还公开了以这种方式操作的再生器。
    • 2. 发明申请
    • ALL FIBER CHIRPED PULSE AMPLIFICATION SYSTEM AND METHOD
    • 所有光纤激光放大系统和方法
    • WO2008121273A2
    • 2008-10-09
    • PCT/US2008/003892
    • 2008-03-25
    • CORNING INCORPORATEDKUKSENKOV, Dmitri VLI, Shenping
    • KUKSENKOV, Dmitri VLI, Shenping
    • H01S3/0057G02B6/02304H01S3/06712H01S3/06725H01S3/06754H01S3/2308
    • An all-fiber chirped pulse amplification (CPA) system and method is provided that utilizes a hollow core photonic bandgap fiber as a pulse compressor and a dispersion compensating optical fiber as a pulse stretcher that are matched with respect to both the amount and slope of dispersion to avoid peak power-limiting pulse distortion. The CPA system includes a rare earth ion-doped optical fiber amplifier having an input and an output that amplifies optical pulses having a center wavelength of ?c, a pulse compressing length L1 of hollow core photonic bandgap fiber having a dispersion value D1 and a dispersion slope S1 that varies over a wavelength ? of the pulses that is optically connected to the output of the fiber amplifier and having a k-parameter defined by a ratio of D1 over the slope of the function D1(?) that is larger than about 50, and a pulse stretching length L2 of dispersion compensating optical fiber connected to the input of the fiber amplifier having a dispersion value D2 and dispersion slope S2. The lengths are selected such that L1D1 = -L2D2, and the center wavelength ?c of the inputted optical pulses is preferably close to the center wavelength of the bandgap of the photonic bandgap fiber.
    • 提供了全光纤啁啾脉冲放大(CPA)系统和方法,其利用空心光子带隙光纤作为脉冲压缩器和色散补偿光纤作为脉冲展宽器,其相对于色散的量和斜率都相匹配 以避免峰值功率限制脉冲失真。 CPA系统包括具有放大具有中心波长λc的光脉冲的输入和输出的稀土离子掺杂光纤放大器,具有色散值D1的空心光子带隙光纤的脉冲压缩长度L1和色散 斜率S1在波长上变化? 光学连接到光纤放大器的输出的脉冲,并且具有由大于约50的函数D1(θ)的斜率上的D1的比率定义的k参数以及大于约50的脉冲拉伸长度L2 色散补偿光纤连接到具有色散值D2和色散斜率S2的光纤放大器的输入。 选择长度使得L1D1 = -L2D2,并且输入的光脉冲的中心波长λc优选接近于光子带隙光纤的带隙的中心波长。