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    • 91. 发明申请
    • Wider dynamic range to a FBG stabilized pump
    • 更宽的动态范围到FBG稳定泵
    • US20040036956A1
    • 2004-02-26
    • US10610510
    • 2003-06-30
    • JDS Uniphase Corporation
    • Erji MaoStuart MacCormackGreg RothSteven Sanders
    • H01S003/00H04B010/12
    • H04B10/296H01S3/1305H01S3/1312H01S3/302H04B10/2916
    • The present application relates to a Raman amplifier having an increased dynamic range, and particularly for laser pump sources and a method of pumping Raman fiber amplifiers over a greater dynamic range. In a multi-channel optical system, optical amplifiers must be able to provide gains over a large dynamic range, which is determined by the distribution of node-to-node distances in the network, as well as the number of channels. The present invention has found that the dynamic range of a Raman amplifier can be significantly increased by using pulse width modulation to pulse pump current at or near the minimum current stability threshold, in order to produce lower power output. The duty cycle of the pulsed current is selected to achieve a time-averaged operating condition, thus the time averaged pump power can be reduced in a linear fashion well below the capability of a continuous wave system.
    • 本申请涉及具有增加的动态范围的拉曼放大器,特别是用于激光泵浦源的拉曼放大器以及在更大动态范围内泵浦拉曼光纤放大器的方法。 在多通道光学系统中,光放大器必须能够在大的动态范围内提供增益,这取决于网络中节点到节点间距离的分布以及信道数量。 本发明已经发现,为了产生较低的功率输出,通过使脉冲宽度调制到等于或接近最小电流稳定阈值的脉冲泵电流,可以显着提高拉曼放大器的动态范围。 选择脉冲电流的占空比以实现时间平均的操作条件,因此可以以远低于连续波系统的能力的线性方式减小时间平均的泵浦功率。
    • 92. 发明申请
    • Apparatus and method for measuring the dispersion of a fiber span
    • 用于测量纤维跨度分散的装置和方法
    • US20040028415A1
    • 2004-02-12
    • US10427897
    • 2003-04-30
    • Michael H. Eiselt
    • H04B010/12
    • H04B10/2513
    • The invention pertains to optical fiber transmission systems, and is particularly relevant to transmission of large volumes of data over long distances at high rates. An improved apparatus and method for measuring dispersion in a fiber span is disclosed. In particular, the invention teaches a highly accurate technique for measuring the fiber dispersion at a single wavelength. Transmitter and receiver structure and data processing algorithms are disclosed. An improved apparatus and method for measuring dispersion in a fiber span. In particular, the invention teaches a highly accurate technique for measuring the fiber dispersion at a single wavelength. Transmitter and receiver structure and data processing algorithms are disclosed.
    • 本发明涉及光纤传输系统,并且特别涉及以高速率长距离传输大量数据。 公开了一种用于测量光纤跨度中的色散的改进的装置和方法。 特别地,本发明教导了用于在单个波长下测量纤维分散体的高精度技术。 公开了发射机和接收机结构和数据处理算法。 一种用于测量纤维跨度中的色散的改进的装置和方法。 特别地,本发明教导了用于在单个波长下测量纤维分散体的高精度技术。 公开了发射机和接收机结构和数据处理算法。
    • 96. 发明申请
    • Dynamic measurement of and compensation for impairments to optical data communication pulses
    • 对光学数据通信脉冲的损伤的动态测量和补偿
    • US20030202795A1
    • 2003-10-30
    • US10128939
    • 2002-04-24
    • Hernando GarciaDaniel Charles KilperJeffrey Matthew RothChunhui Xu
    • H04B010/12
    • H04B10/2569G01J11/00H04B10/077H04B10/07955
    • A photomultiplier module (PMT), preferably a PMT with a gallium arsenide (GaAs) photocathode, is used as a N-photon detector (N is an integer null2). The PMT detects the N-photon absorption rate of an optical signal having a wavelength range extending from 1.0 nullm to an upper wavelength region that increases as the number of photons simultaneously absorbed by the PMT increases beyond two. The N-photon absorption rate is used by a signal compensation apparatus to reduce impairments which affect the rate, such as group velocity dispersion and/or polarization mode dispersion, in a received optical pulse communication signal. The N-photon absorption rate can also be used to determine the optical signal-to-noise ratio of a received optical pulse communication signal, and/or to synchronize a second optical pulse signal with the first optical signal.
    • 使用优选具有砷化镓(GaAs)光电阴极的PMT的光电倍增管模块(PMT)作为N-光子检测器(N为整数> = 2)。 PMT检测到具有从1.0μm的波长范围延伸到上升波长区域的光信号的N光子吸收率,随着PMT同时吸收的光子数增加超过两个,该波长区域增加。 信号补偿装置使用N光子吸收率来减少在接收的光脉冲通信信号中影响速率的损伤,例如组速度色散和/或偏振模色散。 N光子吸收率也可用于确定接收到的光脉冲通信信号的光信噪比和/或使第二光脉冲信号与第一光信号同步。
    • 100. 发明申请
    • All optical clock recovery
    • 所有光时钟恢复
    • US20030043433A1
    • 2003-03-06
    • US10191512
    • 2002-07-10
    • Nortel Networks Limited
    • John Kenton White
    • H04B010/00H04B010/12
    • H04L7/0075H01S5/0656H01S5/0657
    • All optical clock recovery includes a transmitter for generating an optical timing signal. The transmitter includes a semiconductor laser for the production of a dynamically synchronizable timing signal, the laser having an external resonator for feedback of the timing signal to the laser, the feedback having a delay time greater than a relaxation oscillation time for the laser, and the laser outputting an optical timing signal having a characteristic dynamic. The transmitter supplies the optical timing signal to a receiver configured to receive the timing signal and to synchronize to the laser on receipt of the timing signal, such that the receiver outputs a recovered timing signal having the characteristic dynamic. A number of receivers may be provided in sequence along an optical path, each receiver configured to receive the timing signal originally outputted with the characteristic dynamic from the transmitter, and synchronized to the transmitter on receiving the signal and thereby outputting a recovered timing signal having the characteristic dynamic. All optical clock recovery is provided without increased electronic complexity and avoids thermal drift.
    • 所有光时钟恢复包括用于产生光学定时信号的发射机。 发射机包括用于产生动态可同步的定时信号的半导体激光器,该激光器具有外部谐振器,用于向激光器反馈定时信号,反馈具有大于激光器的弛豫振荡时间的延迟时间, 激光输出具有特征动态的光学定时信号。 发射机将光学定时信号提供给被配置为接收定时信号并且在接收到定时信号时与激光器同步的接收机,使得接收机输出具有特征动态的恢复的定时信号。 可以沿着光路顺序地提供多个接收机,每个接收机被配置为从发射机接收原始以特征动态输出的定时信号,并且在接收到信号时同步到发射机,从而输出恢复的定时信号, 特征动态。 提供所有光时钟恢复,而不会增加电子复杂性并避免热漂移。