会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 26. 发明授权
    • Methods for operating diode lasers
    • 二极管激光器的运行方法
    • US07978742B1
    • 2011-07-12
    • US12730482
    • 2010-03-24
    • Dmitri Vladislavovich KuksenkovShenping Li
    • Dmitri Vladislavovich KuksenkovShenping Li
    • H01S3/00
    • A61F11/002H01S5/0602H01S5/06251H01S5/06256
    • Methods for operating diode lasers are provided. According to one method, the diode laser comprises a wavelength selection section, a gain section and a saturable absorber. The method comprises applying a hybrid-control signal comprising a hybrid-control DC bias to the saturable absorber, and applying a hybrid-driving signal comprising a hybrid-driving DC bias and a hybrid-driving AC bias to the gain section. The hybrid signals are selected and the diode laser is configured such that a relatively high hybrid-control DC bias corresponds to a relatively low average of the output power of the diode laser, and a relatively low hybrid-control DC bias corresponds to a relatively high average of the output power of the diode laser. The hybrid-driving DC bias is between a switch-on threshold of the diode laser and a switch-off threshold of the diode laser, and the hybrid-driving AC bias is periodic. The hybrid-driving AC bias has a peak-to-peak amplitude greater than the difference between the switch-on threshold and the switch-off threshold.
    • 提供了操作二极管激光器的方法。 根据一种方法,二极管激光器包括波长选择部分,增益部分和饱和吸收体。 该方法包括将包括混合控制DC偏置的混合控制信号施加到可饱和吸收器,以及将包括混合驱动DC偏置和混合驱动AC偏置的混合驱动信号施加到增益部分。 选择混合信号,并且二极管激光器被配置为使得相对高的混合控制DC偏压对应于二极管激光器的输出功率的相对较低的平均值,并且相对低的混合控制DC偏压对应于相对较高的 平均二极管激光器的输出功率。 混合驱动DC偏压在二极管激光器的接通阈值和二极管激光器的关断阈值之间,并且混合驱动AC偏压是周期性的。 混合驱动AC偏压具有比接通阈值和关断阈值之间的差大的峰 - 峰幅度。
    • 28. 发明授权
    • All fiber chirped pulse amplification system and method
    • 所有光纤啁啾脉冲放大系统及方法
    • US07486436B1
    • 2009-02-03
    • US11729896
    • 2007-03-29
    • Dmitri Vladislavovich KuksenkovShenping Li
    • Dmitri Vladislavovich KuksenkovShenping Li
    • H01S4/00
    • 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 λc, 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 λ 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(λ) 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 λc 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匹配 以避免峰值功率限制脉冲失真。 CPA系统包括具有输入和输出的稀土离子掺杂光纤放大器,该输入和输出放大具有中心波长lambdac的光脉冲,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在与光纤放大器的输出光学连接的脉冲的波长λ上变化,并且具有由大于约50的函数D1(λ)的斜率上的D1的比率定义的k参数, 以及连接到具有色散值D2和色散斜率S2的光纤放大器的输入的色散补偿光纤的脉冲拉伸长度L2。 选择长度使得L1D1 = -L2D2,并且输入的光脉冲的中心波长lambdac优选地接近光子带隙光纤的带隙的中心波长。
    • 29. 发明授权
    • Phase-insensitive recovery of clock pulses of wavelength division multiplexed optical signals
    • US07027468B2
    • 2006-04-11
    • US10667932
    • 2003-09-22
    • Krassimir KrastevDmitri V. KuksenkovShenping Li
    • Krassimir KrastevDmitri V. KuksenkovShenping Li
    • H01S3/30H01S3/83
    • H04L7/0075H04J14/02
    • An optically-pumped mode-locked fiber ring laser for optical clock recovery of multiple wavelength division multiplexed optical signals actively mode-locks a plurality of outputs of the laser as a plurality of recovered clocks for a plurality of the multiple wavelength division multiplexed optical signals. The laser cavity has a cavity length corresponding to an integer multiple of bit periods of at least one of the multiplexed optical signals for receiving a pre-amplified version of the plurality of wavelength division multiplexed optical signals to provide gain modulation through a phase-insensitive parametric amplification and recirculating a proportion of the output from the laser cavity back through the laser cavity for spatially mode-locking the output of the laser cavity as a recovered clock whereby the recovered optical clock each having a periodic train of optical pulses with a repetition rate corresponding to the clock rate of the corresponding multiplexed optical signal is generated by mode-locking of the optically-pumped laser produced by a spatial modulation of the phase-insensitive parametric gain produced by the pulsed nature of the wavelength division multiplexed optical signals. A nonlinear gain medium disposed in the cavity has a sufficiently large dispersion at all of the wavelengths corresponding to the multiple wavelength multiplexed optical signals for minimizing four-wave mixing crosstalk among the multiple wavelength multiplexed optical signals, among the recovered clocks, and between the plurality of multiple wavelength multiplexed optical signals and the recovered clocks. The gain medium is pumped by the plurality of pre-amplified multiplexed optical signals to provide efficient gain modulation through the phase-insensitive parametric amplification at a plurality of narrow wavelength bands, each of the plurality of narrow wavelength bands immediately adjacent to a wavelength of a corresponding optical signal and each of the plurality of narrow wavelength bands including a corresponding recovered optical clock wavelength, and each of the corresponding optical signals copropagating in the laser cavity through the nonlinear gain medium with the recovered optical clocks. A parametric optical amplifier or a Raman amplifier having an inhomogenously broadened gain amplifies the plurality of recovered clocks for compensating a portion of the cavity loss at all wavelengths of the plurality of recovered clocks. A wavelength selector passes the light at the plurality of wavelengths of the recovered clocks for recirculation in the laser cavity and preventing the light from the multiple wavelength division multiplexed optical signals and a plurality of idler waves generated by four wave mixing between the multiple wavelength division multiplexed optical signals and recovered optical clocks from recirculating in the laser cavity.