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    • 1. 发明授权
    • Raman amplifier, pump source for use in a raman amplifier and method for amplifying an optical signal
    • 拉曼放大器,用于拉曼放大器的泵浦源和用于放大光信号的方法
    • US07206123B2
    • 2007-04-17
    • US10935286
    • 2004-09-08
    • Yoshihiro EmoriJake BromageLynn E. NelsonShu Namiki
    • Yoshihiro EmoriJake BromageLynn E. NelsonShu Namiki
    • H01S4/00H04B10/12
    • H01S3/06754H01S3/0078H01S3/06758H01S3/094011H01S3/0941H01S3/10069H01S3/1305H01S3/302H04B10/2916
    • A method, pump and Raman amplifier control an amount of stimulated Brillouin scattering (SBS) produced by the Raman amplifier pump so as to regulate a power penalty experienced by a receiver due to the SBS. A multi-mode semiconductor laser produces a multi-mode pump light having a dominate mode at a predetermined wavelength. At least a portion of the multi-mode pump light is coupled to a Raman gain medium in a forward pumping direction. A reflection sensor monitors reflected light that is at least partially reflected from said Raman gain medium. The reflection sensor has a passband characteristic that passes optical power of a dominate SBS peak of said reflected light, but suppresses other SBS peaks that are offset in wavelength from said dominate SBS peak. The optical power of the dominate SBS peak is compared to an optical power of the multi-mode pump light, and it is determined whether a result of the comparing step is above a predetermined threshold.
    • 一种方法,泵浦和拉曼放大器控制由拉曼放大器泵产生的受激布里渊散射(SBS)的量,以便调节由于SBS而导致的接收器所经受的功率损失。 多模半导体激光器产生具有预定波长的主导模式的多模式泵浦光。 至少一部分多模式泵浦光在正向泵送方向上耦合到拉曼增益介质。 反射传感器监测至少部分地从所述拉曼增益介质反射的反射光。 反射传感器具有通过所述反射光的主要SBS峰值的光焦度的通带特性,但抑制了波长偏离所述主导SBS峰值的其他SBS峰值。 将主要SBS峰值的光功率与多模式泵浦光的光功率进行比较,并且确定比较步骤的结果是否高于预定阈值。
    • 3. 发明申请
    • LIGHT SOURCE IN OPTICAL TRANSMISSION SYSTEM, WAVEFORM SHAPER, OPTICAL PULSE TRAIN GENERATOR AND OPTICAL REPRODUCTION SYSTEM
    • 光传输系统中的光源,波形形状,光脉冲发生器和光学再现系统
    • US20090092400A1
    • 2009-04-09
    • US12238065
    • 2008-09-25
    • Koji IGARASHIYoshihiro EmoriAtsushi OguriShu NamikiOsamu AsoMasateru Tadakuma
    • Koji IGARASHIYoshihiro EmoriAtsushi OguriShu NamikiOsamu AsoMasateru Tadakuma
    • H04B10/12
    • G02F1/365G02F1/3513G02F2203/17G02F2203/26H01S5/0623H04B10/25077H04B10/291
    • The present invention provides a pulse train generator comprising: a dual-frequency signal light source for generating a dual-frequency signal; a soliton shaper for soliton-shaping output light from the dual-frequency signal light source; and an adiabatic soliton compressor for performing adiabatic soliton compression on output light from the soliton shaper, and also provides a waveform shaper used in this pulse train generator, including a plurality of highly nonlinear optical transmission lines and a plurality of low-nonlinearity optical transmission lines which has a nonlinearity coefficient lower than that of the plurality of highly nonlinear optical transmission lines and which has a second-order dispersion value of which an absolute value is different from that of the plurality of highly nonlinear optical transmission lines. Further, the present invention provides a light source comprising a plurality of continuous light sources of which at least one oscillates in a multimode; a multiplexer for multiplexing output light from the continuous light sources; and a nonlinear phenomenon producer for producing a nonlinear phenomenon on output light from the multiplexer so as to suppress SBS (Stimulated Brillouin Scattering).
    • 本发明提供一种脉冲串发生器,包括:用于产生双频信号的双频信号光源; 用于孤子整形的孤子整形器来自双频信号光源的输出光; 以及用于对来自孤子整形器的输出光进行绝热孤子压缩的绝热孤子压缩器,并且还提供在该脉冲串发生器中使用的波形整形器,包括多个高度非线性的光传输线和多个低非线性光传输线 其具有比多个高度非线性光传输线的非线性系数低的非线性系数,并且具有绝对值与多个高度非线性光传输线的绝对值不同的二阶色散值。 此外,本发明提供了一种光源,其包括至少一个以多模振荡的多个连续光源; 多路复用器,用于复用来自连续光源的输出光; 以及用于在来自多路复用器的输出光上产生非线性现象以抑制SBS(受激布里渊散射)的非线性现象产生器。
    • 4. 发明授权
    • Optical signal amplifier
    • 光信号放大器
    • US07400442B2
    • 2008-07-15
    • US10645528
    • 2003-08-22
    • Shunichi MatsushitaShu NamikiYoshihiro Emori
    • Shunichi MatsushitaShu NamikiYoshihiro Emori
    • H01S3/00
    • H01S3/302H01S3/094003H01S3/094073H01S3/094096H01S3/2375H01S5/146
    • An optical signal amplifier includes a light source, a depolarizer, and a gain medium that transfers energy from a pump beam output from the depolarizer to the optical signal. The depolarizer may include one or more birefringent optical fibers which support two polarization modes, a fast mode and a slow mode. The light propagates in the fast mode at a higher velocity than the light propagates in the slow mode so as to impart phase delay as the light propagates in the birefringent optical fibers, thereby at least partially depolarizing the beam. A method for using the amplifier with different types of transmission fibers enables the matching of depolarizers with relatively high percentage of degree of polarization, depending on fiber type, while staying below polarization dependent gain requirements.
    • 光信号放大器包括光源,去偏振器和将从去偏振器输出的泵浦光束的能量传递到光信号的增益介质。 去极化器可以包括一种或多种支持两种偏振模式的双折射光纤,即快速模式和慢速模式。 光在快速模式下以比在慢速模式中传播的光速更高的速度传播,以便当光在双折射光纤中传播时给予相位延迟,从而至少部分地使光束去极化。 使用具有不同类型的传输光纤的放大器的方法使得取决于光纤类型的去偏振器的匹配度具有相对高百分比的偏振度,同时保持在偏振相关增益要求之下。
    • 6. 发明申请
    • Raman amplifier
    • 拉曼放大器
    • US20050157379A1
    • 2005-07-21
    • US11079301
    • 2005-03-15
    • Yoshihiro EmoriShu Namiki
    • Yoshihiro EmoriShu Namiki
    • H01S3/094H01S3/23H01S3/30H04B10/291H01S3/00
    • H04B10/2916H01S3/06766H01S3/0677H01S3/09408H01S3/094096H01S3/10007H01S3/302H01S2301/04
    • In a Raman amplifier using three or more pumping wavelengths, when the pumping wavelengths are divided into a short wavelength side group and a long wavelength side group at the boundary of the pumping wavelength having the longest interval between the adjacent wavelengths, the short wavelength side group includes two or more pumping wavelengths having intervals therebetween which are substantially equidistant, and the long wavelength side group is constituted by two or less pumping wavelengths. When a certain pumping wavelength is defined as a first channel and pumping wavelengths which are spaced apart from each other by about 1 THz from the certain pumping wavelength toward a long wavelength side are defined as second to n-th channels, respectively, pump lights having wavelengths corresponding to the first to n-th channels are multiplexed, and pump light having a wavelength spaced apart from the n-th channel by 2 THz or more toward the long wavelength side is further multiplexed with the said multiplexed pump light, and resultant pump light is used as pump source. Pump lights of all of the wavelengths corresponding to the channels other than (n−1)th and (n−2)th channels are multiplexed with each other, and resultant pump light is used as pump source. Pump lights of all of the wavelengths corresponding to the channels other than (n−2)th and (n−3)th channels are multiplexed with each other, and resultant pump light is used as pump source.
    • 在使用三个或更多个泵浦波长的拉曼放大器中,当在相邻波长之间具有最长间隔的激励波长的边界处将泵浦波长分成短波长侧组和长波长侧组时,短波长侧组 包括两个或更多个泵浦波长,其间具有基本等距的间隔,并且长波长侧组由两个或更少的泵浦波长构成。 当将一定的泵浦波长定义为第一通道时,分别从一定的泵浦波长朝向长波长侧彼此隔开约1THz的泵浦波长分别定义为第二至第n通道,泵浦光具有 对应于第一至第n通道的波长被多路复用,并且与所述多路复用泵浦光进一步多路复用具有与第n通道相隔离长波长侧2THz以上的波长的泵浦光, 光用作泵浦源。 对应于第(n-1)和(n-2)个通道以外的通道的所有波长的泵浦光彼此多路复用,并且所得到的泵浦光用作泵浦源。 与第(n-2)和(n-3)通道以外的通道相对应的所有波长的泵浦光彼此多路复用,并且所得到的泵浦光用作泵浦源。
    • 7. 发明授权
    • Raman amplification method and optical signal transmission method using the same
    • 拉曼放大法和光信号传输法使用相同
    • US06882467B1
    • 2005-04-19
    • US10615187
    • 2003-07-09
    • Yoshihiro EmoriShu Namiki
    • Yoshihiro EmoriShu Namiki
    • H01S3/094H01S3/30H04B10/291H01S3/00
    • H04B10/2916H01S3/094011H01S3/302
    • First pump light for Raman-amplifying optical signal is inputted to the output end of the optical signal, and second pump light used for Raman-amplifying the first pump light and having a wavelength shorter than that of the first pump light is inputted to the input end of the optical signal. The second pump light is also inputted to the output end of the optical signal. The first pump light is also inputted to the input end of the optical signal. The Raman amplification band of the second pump light is made not to be overlapped with that of the optical signal. The wavelength of the second pump light is shorter than that of the first pump light by the Raman shift of the amplifier fiber. The light source of either the first or second pump light or both the light sources of them are multiplex optical sources. The first pump light is emitted from a semiconductor laser. Third pump light for Raman-amplifying the second pump light is directed to an optical transmission line. The optical signal is transmitted through a transmission line using the Raman amplification method.
    • 用于拉曼放大光信号的第一泵浦光被输入到光信号的输出端,并且用于拉曼放大第一泵浦光并且具有比第一泵浦光的波长短的波长的第二泵浦光被输入到输入 结束光信号。 第二泵浦光也被输入到光信号的输出端。 第一泵浦光也被输入到光信号的输入端。 第二泵浦光的拉曼放大频带不与光信号的拉曼放大频带重叠。 第二泵浦光的波长通过放大器光纤的拉曼偏移比第一泵浦光的波长短。 第一或第二泵浦光或其两个光源的光源是多路光源。 第一泵浦光从半导体激光器发射。 用于拉曼放大第二泵浦光的第三泵浦光被引导到光传输线。 光信号通过使用拉曼放大法的传输线传输。
    • 8. 发明申请
    • RAMAN AMPLIFIER, OPTICAL REPEATER, AND RAMAN AMPLIFICATION METHOD
    • 拉曼放大器,光学重放器和拉曼放大方法
    • US20100067099A1
    • 2010-03-18
    • US12619455
    • 2009-11-16
    • Youichi AKASAKAYoshihiro EmoriShu Namiki
    • Youichi AKASAKAYoshihiro EmoriShu Namiki
    • H01S3/30H01S3/00
    • A Raman amplifier according to the present invention comprises a plurality of pumping means using semiconductor lasers of Fabry-Perot, DFB, or DBR type or MOPAs, and pumping lights outputted from the pumping means have different central wavelengths, and interval between the adjacent central wavelength is greater than 6 nm and smaller than 35 nm. An optical repeater according to the present invention comprises the above-mentioned Raman amplifier and adapted to compensate loss in an optical fiber transmission line by the Raman amplifier. In a Raman amplification method according to the present invention, the shorter the central wavelength of the pumping light the higher light power of said pumping light. In the Raman amplifier according to the present invention, when a certain pumping wavelength is defined as a first channel, and second to n-th channels are defined to be arranged with an interval of about 1 THz toward a longer wavelength side, the pumping lights having wavelengths corresponding to the first to n-th channels are multiplexed, and an pumping light having a wavelength spaced apart from the n-th channel by 2 THz or more toward the longer wavelength side is combined with the multiplexed light, thereby forming the pumping light source. The pumping lights having wavelengths corresponding to the channels other than (n-1)-th and (n-2)-th channels may be multiplexed, thereby forming the pumping light source. The pumping lights having wavelengths corresponding to the channels other than (n-2)-th and (n-3)-th channels may be multiplexed, thereby forming the pumping light source.
    • 根据本发明的拉曼放大器包括使用Fabry-Perot,DFB或DBR型或MOPA的半导体激光器的多个泵浦装置,并且从泵送装置输出的泵浦光具有不同的中心波长,并且相邻中心波长 大于6nm且小于35nm。 根据本发明的光中继器包括上述拉曼放大器,并且用于补偿拉曼放大器在光纤传输线路中的损耗。 在根据本发明的拉曼放大方法中,泵浦光的中心波长越短,所述泵浦光的光功率越高。 在根据本发明的拉曼放大器中,当将一定的泵浦波长定义为第一通道时,并且将第二至第n通道限定为朝向较长波长侧以大约1THz的间隔布置,泵浦灯 具有对应于第一至第n通道的波长的多路复用,并且将具有与第n个信道间隔开2波长或更长的波长朝向较长波长侧的波长的泵浦光与多路复用光组合,从而形成泵浦 光源。 具有与第(n-1)和(n-2)通道以外的通道对应的波长的泵浦光可以被多路复用,从而形成泵浦光源。 具有与第(n-2)和(n-3)通道以外的通道对应的波长的泵浦光可以被多路复用,从而形成泵浦光源。
    • 9. 发明授权
    • Depolarized laser diode module and depolarized laser diode light source
    • 去极化激光二极管模块和去极化激光二极管光源
    • US07072369B2
    • 2006-07-04
    • US10820771
    • 2004-04-09
    • Shunichi MatsushitaShu NamikiYoshihiro Emori
    • Shunichi MatsushitaShu NamikiYoshihiro Emori
    • H01S3/13H01S3/30
    • H01S5/146H01S3/094003H01S3/094073H01S3/302H01S5/06236
    • The present invention provides the following designing method: in a laser diode module or a depolarized laser diode module which has one laser diode and one polarization maintaining fiber connected to the output side thereof, the length of the polarization maintaining fiber is a value obtained by calculation of equation 37 with use of a longitudinal mode spacing Δλoutput light from the Fabry Perot (FP) laser diode, an oscillating center wavelength λ0 of the laser light, a beat length LBeat 1 of the polarization maintaining fiber and an optical wavelength λBeat used in the measurement of the LBeat 1. (Equation 37) L Pig
    • 本发明提供以下设计方法:在激光二极管模块或去极化激光二极管模块中,其具有连接到其输出侧的一个激光二极管和一个偏振保持光纤,所述偏振保持光纤的长度是通过计算获得的值 使用来自法布里珀罗(FP)激光二极管的纵向模式间隔Deltalλ输出光,激光的振荡中心波长λ<0>,拍子长度L < / SUB>和用于测量L“Beat 1”的光波长λ。 (公式37) L > << / MO> > / MO> 1 lambda Beat 1