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    • 25. 发明授权
    • Broadband optical fiber laser
    • 宽带光纤激光器
    • US4964131A
    • 1990-10-16
    • US319241
    • 1989-03-09
    • Karen LiuByoung Y. KimMichel J. F. DigonnetKenneth A. FeslerHerbert J. Shaw
    • Karen LiuByoung Y. KimMichel J. F. DigonnetKenneth A. FeslerHerbert J. Shaw
    • G01C19/72H01S3/067H01S3/094H01S3/0941
    • G01C19/721H01S3/06795H01S3/0941H01S3/094003
    • An optical fiber laser includes a single-mode optical fiber doped with a lasing material such as Neodymium. The optical fiber is pumped with a pump optical signal having a pump wavelength selected to cause spontaneous emission of an optical signal at a second wavelength different from the pump wavelength. The optical fiber is formed into a laser cavity such as by including a suitable reflector at each of the two ends of a suitable length of the optical fiber so that the emitted optical signal oscillates therein. One of the reflectors has a reflectivity at the wavelength of the emitted light so that most (e.g., approximately 95%) of the emitted light is reflected back into the laser cavity and a smaller portion (e.g, approximately 5%) is transmitted through the mirror as a laser output signal. Alternatively, the optical fiber can be formed into a ring laser structure using an optical coupler that couples a substantial portion (e.g., approximately 95%) of the emitted light back into the ring for recirculation therein and provides a smaller portion of the emitted light (e.g., approximately 5%) as a laser output signal. The wavelength of the pump optical signal is selected to be outside the pump variable tuning range of the Neodymium-doped optical fiber (i.e., the range of pump wavelengths which stimulate emitted wavelengths having a average wavelengths with a generally one-to-one correspondence to the pump wavelength). Pumping with a pump signal outside the pump variable tuning ranges causes the emitted light to have a broad spectral envelope of longitudinal modes having emission wavelengths corresponding to substantially all the pump variable tuning range. Thus, by pumping the optical fiber with a single pump wavelength, a broadband laser output signal is generated.
    • 光纤激光器包括掺杂有诸如钕的激光材料的单模光纤。 用选择了泵浦波长的泵浦光信号来泵浦光纤,以引起与泵浦波长不同的第二波长的光信号的自发发射。 光纤被形成为激光腔,例如通过在光纤的适当长度的两端中的每一端包括合适的反射器,使得所发射的光信号在其中振荡。 反射器中的一个在发射光的波长处具有反射率,使得大部分(例如,大约95%)的发射光被反射回到激光腔中,并且较小的部分(例如,大约5%)通过 镜像为激光输出信号。 或者,可以使用光耦合器将光纤形成为环形激光器结构,所述光耦合器将发射的光的大部分(例如,大约95%)重新连接到环中以在其中再循环,并且提供较小部分的发射光 例如约5%)作为激光输出信号。 泵浦光信号的波长被选择在掺杂钕光纤的泵可变调谐范围之外(即,泵浦波长的范围,其激发平均波长与一般一一对应的发射波长 泵浦波长)。 在泵可变调谐范围之外用泵浦信号泵送使得发射的光具有宽泛的光谱包络,其具有与基本上所有泵可变调谐范围对应的发射波长的纵向模式。 因此,通过用单个泵浦波长泵浦光纤,产生宽带激光输出信号。
    • 27. 发明授权
    • Phase reading fiber optic interferometer
    • 相位读取光纤干涉仪
    • US4836676A
    • 1989-06-06
    • US946628
    • 1986-12-29
    • Byoung Y. KimHerbert J. Shaw
    • Byoung Y. KimHerbert J. Shaw
    • G01C19/72
    • G01C19/72
    • A system and method for detecting the influence of selected forces on an interferometer over an extended dynamic range. One presently preferred embodiment is disclosed for detecting rotation of an interferometer. In this embodiment, an open-loop, all-fiber-optic gyroscope provides an output signal comprising the phase difference of two light waves which are counterpropagating within the gyroscope, and which are phase modulated at a selected frequency. The phase difference of the light waves is influenced by the rotation rate of the interferometer. The output signal is amplitude modulated at the phase modulation frequency to transpose the optical phase shift into a low frequency electronic phase shift, which is measured using a digital time interval counter. A linear scale factor is achieved through use of this system and method.
    • 一种用于在扩展动态范围内检测所选力对干涉仪的影响的系统和方法。 公开了一种目前优选的实施例,用于检测干涉仪的旋转。 在该实施例中,开环全光纤陀螺仪提供包括在陀螺仪内相反传播的两个光波的相位差并且以所选频率进行相位调制的输出信号。 光波的相位差受到干涉仪的旋转速度的影响。 输出信号以相位调制频率进行幅度调制,以将光相位转换成低频电子相移,其使用数字时间间隔计数器测量。 通过使用该系统和方法实现线性比例因子。
    • 29. 发明授权
    • Synchronously pumped ring fiber Raman laser
    • 同步泵浦环形光纤拉曼激光器
    • US4794598A
    • 1988-12-27
    • US888170
    • 1986-07-18
    • Emmanuel DesurvireHerbert J. Shaw
    • Emmanuel DesurvireHerbert J. Shaw
    • H01S3/00H01S3/06H01S3/094H01S3/16H01S3/30
    • H01S3/094026H01S3/302
    • An all-fiber ring laser has a single, uninterrupted length of single-mode optical fiber that is formed into a loop by using an optical coupler. Pump signal pulses at a first optical wavelength are introduced into one end of the optical fiber. Each pump pulse propagates through the loop formed in the fiber and then exits the fiber. The pump signal pulses excite the molecules of the optical fiber to cause them to go to a higher, unstable energy level. When the molecules return to a lower energy level, photons are emitted at a second optical frequency that has a wavelength that is shifted from the wavelength of the pump signal to form laser signal pulses. The coupler is a multiplexing coupler that has a first coupling ratio at the wavelength of the pump signal and has a second coupling ratio at the wavelength of the emitted optical signal. The first coupling ratio is preferably close to zero and the second coupling coefficient is greater than 0.5. The laser optical signal recirculates in the loop to stimulate further emission of optical energy at the shifted wavelength in phase with the recirculating optical signal. Each pump pulse is timed to enter the optical fiber loop in synchronism with the recirculating laser signal pulse so as to excite the fiber molecules so as to amplify the recirculating signal pulses. The laser signal has a loop transit time related to the time interval between pump pulses such that a multiple of the loop transit time is substantially equal to a multiple of the time interval.
    • 全光纤环形激光器具有单个不间断长度的单模光纤,其通过使用光耦合器形成环路。 在第一光波长的泵浦信号脉冲被引入光纤的一端。 每个泵浦脉冲通过形成在光纤中的环路传播,然后离开光纤。 泵浦信号脉冲激发光纤的分子,使它们进入更高,不稳定的能级。 当分子返回到较低的能量水平时,光子以具有从泵浦信号的波长偏移的波长的第二光学频率发射以形成激光信号脉冲。 耦合器是在泵浦信号的波长处具有第一耦合比并且在所发射的光信号的波长处具有第二耦合比的多路耦合器。 第一耦合比优选接近零,第二耦合系数大于0.5。 激光光信号在环路中再循环以刺激与再循环光信号同相的移动波长的光能的进一步发射。 每个泵浦脉冲被定时以与循环激光信号脉冲同步地进入光纤回路,以激发光纤分子,以放大再循环信号脉冲。 激光信号具有与泵脉冲之间的时间间隔相关的回路通过时间,使得循环通过时间的倍数基本上等于时间间隔的倍数。