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    • 61. 发明授权
    • Dual coupler fiber optic recirculating memory
    • 双耦合光纤再循环存储器
    • US4479701A
    • 1984-10-30
    • US326215
    • 1981-12-01
    • Steven A. NewtonJohn E. BowersHerbert J. Shaw
    • Steven A. NewtonJohn E. BowersHerbert J. Shaw
    • G11C21/00G01S7/285G02B6/00G02B6/28G02B5/172
    • G02B6/29338G02B6/2821G02B6/2861G02B6/29332
    • A fiber optic recirculating memory is disclosed which utilizes dual couplers to form a splice-free recirculating memory device from a length of single mode optical fiber forming a loop which acts as a delay line and a second length of single mode optical fiber which provides an input end and an output end for the device. A single signal supplied as an input to the device will result in a series of output signals identical to the input signal, although at smaller, decreasing amplitudes; the invention prevents the first output signal from being substantially larger than the rest of the output signals, thus eliminating the need for protective circuitry on the output end or the rejection of the first output signal. In addition to being useful as a recirculating memory device for use in a system where data is generated at a rate faster than it can be accepted by a data processor, the invention may be used as a tap filter to pass a selected fundamental frequency and its harmonics, and to attenuate all other frequencies.
    • 公开了一种光纤再循环存储器,其利用双耦合器从一单一模式光纤的长度形成无拼接的循环存储器件,该单模光纤形成用作延迟线的环路和第二长度的单模光纤,其提供输入 端和输出端。 作为输入到设备的单个信号将产生与输入信号相同的一系列输出信号,尽管幅度较小,幅度较小。 本发明防止第一输出信号显着地大于其余的输出信号,从而消除了在输出端上对保护电路的需要或第一输出信号的抑制。 除了用作在数据以比数据处理器可以接受的速度更快的速度生成数据的系统中有用的本发明之外,本发明可以用作抽头滤波器以通过选定的基频,并且其 谐波,并衰减所有其他频率。
    • 64. 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。
    • 66. 发明授权
    • Continuously variable fiber optic delay line
    • 连续可变光纤延迟线
    • US4676585A
    • 1987-06-30
    • US637042
    • 1984-07-09
    • Herbert J. ShawJohn E. BowersSteven A. Newton
    • Herbert J. ShawJohn E. BowersSteven A. Newton
    • G02B6/00G02B6/28H04B10/02G02B6/26
    • G02B6/2861G02B6/2821G02B6/2826G02B6/283Y10S359/90
    • A continuously variable optical delay line having a first substrate (66, 70) and a second substrate (95). The first substrate is composed of a quartz block (70) with a large radius of curvature along its length, supporting a silicon substrate (66) having a plurality of longitudinal, parallel v-grooves (68). A single length (121) of single mode optical fiber is wrapped around the first substrate (66, 70) in helical fashion with each loop being secured in one of the v-grooves (68). The portions of the fiber (121) in the v-grooves (68) are lapped and polished to create a flat coupling surface extending laterally and longitudinally across the first substrate (66, 70). The second substrate (91) is composed of a quartz block with a single v-groove holding a segment of single mode fiber (95). The radius of curvature of this v-groove is substantially smaller than that of the first substrate, such that the flat coupling surface of the second substrate (91) is shorter than that of the first substrate (66). The first and second substrates are placed together such that the fiber in the second substrate is coupled to the fiber in the first substrate. By moving (142) the second substrate longitudinally with respect to the first substrate, a continuously variable delay can be obtained. The continuously variable delay line can be combined with a separate discretely variable delay line to create a longer continuous variable delay. The continuous variable delay line can be formed with only one v-groove (68) in the first substrate (66).
    • PCT No.PCT / US82 / 01609 Sec。 371日期1984年7月9日 102(e)日期1984年7月9日PCT申请日1982年11月12日PCT公布。 出版物WO84 / 02006 日期:1984年5月24日。一种具有第一基板(66,70)和第二基板(95)的连续可变光延迟线。 第一衬底由沿其长度具有大曲率半径的石英块(70)组成,支撑具有多个纵向平行V形槽(68)的硅衬底(66)。 单模光纤的单个长度(121)以螺旋方式缠绕在第一基板(66,70)周围,每个环固定在一个V形槽(68)中。 所述v形槽(68)中的所述纤维(121)的所述部分被研磨和抛光以产生横向和纵向延伸穿过所述第一衬底(66,70)的平坦的联接表面。 第二基板(91)由具有保持单模光纤(95)的单个v形槽的石英块组成。 该v形槽的曲率半径比第一衬底的曲率半径小,使得第二衬底(91)的平坦耦合表面比第一衬底(66)的平坦的耦合表面短。 将第一和第二基板放置在一起,使得第二基板中的光纤耦合到第一基板中的光纤。 通过相对于第一基板纵向移动(142)第二基板,可以获得连续可变的延迟。 连续可变延迟线可以与单独的离散可变延迟线组合以产生更长的连续可变延迟。 连续可变延迟线可以在第一基板(66)中仅形成一个V形槽(68)。