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    • 1. 发明公开
    • Optical sampling waveform measuring apparatus and polarization beam splitter which can be assembled therein
    • Polarisationsstrahlteiler
    • EP1610108A2
    • 2005-12-28
    • EP05018845.7
    • 1998-09-17
    • ANRITSU CORPORATIONNIPPON TELEGRAPH AND TELEPHONE CORPORATION
    • Otani, AkihitoOtsubo, ToshinobuTakara, HidehikoKawanishi, Satoki
    • G01J11/00
    • G02B27/283G01J11/00
    • A sampling light source (10) generates a pulse sequence of sampling light having a pulse width smaller than that of target light (a) and a single plane of polarization. A polarization beam splitting unit (11) splits each of the sampling light output from the sampling light source, and the target light into two light components having planes of polarization shifted 90° from each other, multiplexes each pair of split sampling and target light components having planes of plane of polarization shifted 90° from each other, and outputs the respective multiplexed light components to different optical paths. A pair of nonlinear optical members (1a, 1b) each generate a cross-correlation signal based on the sampling and target light components output from the polarization beam splitting unit to each optical path and having planes of polarization shifted 90° from each other as sum frequency light. A pair of photodetectors (7a, 7b) each convert the sum frequency light output from each of the pair of nonlinear optical members into an electrical signal. A signal processing unit (12) adds the electrical signals output from the pair of photodetectors, processes the resultant electrical signal, and displays its pulse waveform. With this operation, the pulse waveform of the target light can be accurately measured regardless of variations in the polarized state of the target light.
    • 采样光源(10)产生具有比目标光(a)的脉冲宽度小的偏振光的脉冲宽度的采样光的脉冲序列。 偏振光束分离单元(11)将从采样光源输出的采样光中的每一个分离,并将目标光分离成具有彼此偏移90°的偏振平面的两个光分量,将每对分离采样和目标光分量 具有偏振平面的平面彼此偏移90°,并将各个复用的光分量输出到不同的光路。 一对非线性光学构件(1a,1b)基于从偏振光束分离单元输出到每个光路并且具有彼此偏移90°的平面的采样和目标光分量产生互相关信号作为总和 频率灯。 一对光电检测器(7a,7b)将从每对非线性光学部件的每一个输出的和频率光转换为电信号。 信号处理单元(12)将从一对光电检测器输出的电信号相加,处理所得的电信号,并显示其脉冲波形。 通过这种操作,无论目标光的偏振状态的变化如何,都可以精确地测量目标光的脉搏波形。
    • 2. 发明公开
    • Optical sampling waveform measuring apparatus
    • Optisch提出了Wellenform-Messgerät
    • EP0903567A2
    • 1999-03-24
    • EP98117669.6
    • 1998-09-17
    • ANRITSU CORPORATIONNippon Telegraph and Telephone Corporation
    • Otani, AkihitoOtsubo, ToshinobuTakara, Hidehiko, c/o Nippon T & T CorporationKawanishi, Satori, c/o Nippon T & T Corporation
    • G01J11/00
    • G02B27/283G01J11/00
    • A sampling light source (10) generates a pulse sequence of sampling light having a pulse width smaller than that of target light (a) and a single plane of polarization. A polarization beam splitting unit (11) splits each of the sampling light output from the sampling light source, and the target light into two light components having planes of polarization shifted 90° from each other, multiplexes each pair of split sampling and target light components having planes of plane of polarization shifted 90° from each other, and outputs the respective multiplexed light components to different optical paths. A pair of nonlinear optical members (1a, 1b) each generate a cross-correlation signal based on the sampling and target light components output from the polarization beam splitting unit to each optical path and having planes of polarization shifted 90° from each other as sum frequency light. A pair of photodetectors (7a, 7b) each convert the sum frequency light output from each of the pair of nonlinear optical members into an electrical signal. A signal processing unit (12) adds the electrical signals output from the pair of photodetectors, processes the resultant electrical signal, and displays its pulse waveform. With this operation, the pulse waveform of the target light can be accurately measured regardless of variations in the polarized state of the target light.
    • 采样光源(10)产生具有比目标光(a)的脉冲宽度小的偏振光的脉冲宽度的采样光的脉冲序列。 偏振光束分离单元(11)将从采样光源输出的采样光中的每一个分离,并将目标光分成具有彼此偏移90°的平面的两个光分量,将每对分离采样和目标光分量 具有偏振面的平面彼此偏移90°,并将各个复用的光分量输出到不同的光路。 一对非线性光学构件(1a,1b)基于从偏振光束分离单元输出到每个光路并且具有彼此偏移90°的平面的采样和目标光分量产生互相关信号作为总和 频率灯。 一对光电检测器(7a,7b)将从每对非线性光学部件的每一个输出的和频率光转换为电信号。 信号处理单元(12)将从一对光电检测器输出的电信号相加,处理所得的电信号,并显示其脉冲波形。 通过这种操作,无论目标光的偏振状态的变化如何,都可以精确地测量目标光的脉搏波形。
    • 4. 发明公开
    • Optical sampling waveform measuring apparatus
    • Optisch提出了Wellenform-Messgerät
    • EP0903567A3
    • 2004-09-08
    • EP98117669.6
    • 1998-09-17
    • ANRITSU CORPORATIONNippon Telegraph and Telephone Corporation
    • Otani, AkihitoOtsubo, ToshinobuTakara, Hidehiko, c/o Nippon T & T CorporationKawanishi, Satoki, c/o Nippon T & T Corporation
    • G01J11/00G02B27/28G02F1/35
    • G02B27/283G01J11/00
    • A sampling light source (10) generates a pulse sequence of sampling light having a pulse width smaller than that of target light (a) and a single plane of polarization. A polarization beam splitting unit (11) splits each of the sampling light output from the sampling light source, and the target light into two light components having planes of polarization shifted 90° from each other, multiplexes each pair of split sampling and target light components having planes of plane of polarization shifted 90° from each other, and outputs the respective multiplexed light components to different optical paths. A pair of nonlinear optical members (1a, 1b) each generate a cross-correlation signal based on the sampling and target light components output from the polarization beam splitting unit to each optical path and having planes of polarization shifted 90° from each other as sum frequency light. A pair of photodetectors (7a, 7b) each convert the sum frequency light output from each of the pair of nonlinear optical members into an electrical signal. A signal processing unit (12) adds the electrical signals output from the pair of photodetectors, processes the resultant electrical signal, and displays its pulse waveform. With this operation, the pulse waveform of the target light can be accurately measured regardless of variations in the polarized state of the target light.
    • 采样光源(10)产生具有比目标光(a)的脉冲宽度小的偏振光的脉冲宽度的采样光的脉冲序列。 偏振光束分离单元(11)将从采样光源输出的采样光中的每一个分离,并将目标光分离成具有彼此偏移90°的偏振平面的两个光分量,将每对分离采样和目标光分量 具有偏振平面的平面彼此偏移90°,并将各个复用的光分量输出到不同的光路。 一对非线性光学构件(1a,1b)基于从偏振光束分离单元输出到每个光路并且具有彼此偏移90°的平面的采样和目标光分量产生互相关信号作为总和 频率灯。 一对光电检测器(7a,7b)将从每对非线性光学部件的每一个输出的和频率光转换为电信号。 信号处理单元(12)将从一对光电检测器输出的电信号相加,处理所得的电信号,并显示其脉冲波形。 通过这种操作,无论目标光的偏振状态的变化如何,都可以精确地测量目标光的脉搏波形。
    • 6. 发明公开
    • Optical sampling waveform measuring apparatus with high bandwidth
    • Optisch提供了Wellenform-Messgerätmit hoher Bandbreite
    • EP1241458A1
    • 2002-09-18
    • EP02005918.4
    • 2002-03-14
    • ANRITSU CORPORATIONNippon Telegraph and Telephone Corporation
    • Otani, AkihitoOtsubo, ToshinobuTakara, HidehikoShake, IppeiKawanishi, Satoki
    • G01J11/00
    • G01J11/00G02F1/3534
    • A nonlinear optical crystal (10) is composed of 2-adamantyl-5-nitorpyridine (AANP) allowing the type 2 phase matching to the sampling light and a measuring object light, emitting a sum frequency light of the measuring object light and the sampling light, with the polarization directions thereof being perpendicular to each other, when the sampling light and measuring object light multiplexed by a multiplexer (3) are entered. When the sum frequency light is emitted through the nonlinear optical crystal (10), a control portion (2, 5) controls the polarization direction of the sampling light so as to be parallel to a predetermined reference axis located within a plane perpendicular to a phase matching direction of the nonlinear optical crystal. The predetermined reference axis is a single axis maintaining parallelism with the crystal axis of the nonlinear optical crystal even if the wavelength of the inputted light is changed.
    • 非线性光学晶体(10)由允许与采样光进行2相匹配的2-金刚烷基-5-硝基吡啶(AANP)和测量对象光组成,发射测量对象光和采样光的和频光 当由多路复用器(3)光复用的采样光和测量对象进入时,其偏振方向彼此垂直。 当通过非线性光学晶体(10)发射总和频率光时,控制部分(2,5)控制采样光的偏振方向,以平行于垂直于相位的平面内的预定基准轴 非线性光学晶体的匹配方向。 即使输入光的波长发生变化,预定的基准轴也是与非线性光学晶体的晶轴保持平行的单轴。
    • 7. 发明公开
    • Wavelength dispersion measuring apparatus and polarization dispersion measuring apparatus
    • 设备,用于测量的波长色散和偏振色散测量装置
    • EP0937973A3
    • 2002-07-17
    • EP99103133.7
    • 1999-02-17
    • ANRITSU CORPORATIONNippon Telegraph and Telephone Corporation
    • Otani, AkihitoOtsubo, ToshinobuTakara, Hidehiko c/o Nippon Telegr. & Tele. Corp.Kawanishi, Satoki c/o Nippon Telegr. & Tele. Corp.Yamabayashi, Yoshiaki c/o Nippon Telegr.& Tel.Cor.
    • G01J9/02G01M11/00
    • G01M11/336G01J4/00G01J7/00G01J2009/0261G01M11/332G01M11/335
    • A first tunable wavelength pulse light source (22) is driven by a reference signal to emit a first optical pulse. An optical demultiplexer (24) demultiplexes a first optical pulse emitted from the first pulse light source (22) into a reference optical pulse and an incident optical pulse to be sent into an object to be measured. An optical multiplexer (26) multiplexes the reference optical pulse and an outgoing optical pulse passing through the object to output multiplexed light. A second pulse light source (23) generates a second optical pulse which is synchronous with the first optical pulse and delays a predetermined time for each period of the first optical pulse. A sampling unit (27, 27a, 27b) receives the multiplexed light and the second optical pulse to obtain an optical pulse train signal proportional to the intensity of the multiplexed light obtained in synchronism with the second optical pulse. From the optical pulse train signal from the sampling unit (27, 27a, 27b), a signal processor (37) obtains an envelope formed by peaks of individual optical pulses forming the optical pulse train. The wavelength dispersion of the object is obtained by measuring the delay time of the outgoing optical pulse passing through the object on the basis of intervals between the peaks of the envelope.
    • 第一波长可调谐脉冲光源(22)由一个参考信号驱动以发射第一光脉冲。 光解复用器(24)解复用从第一脉冲光源(22)转换成参照光脉冲,并射入光脉冲发射的第一光脉冲在物体被发送到要被测量。 光复用器(26)复用该参照光脉冲和出射光脉冲通过对象传递到输出多路复用的光。 第二脉冲光源(23)基因速率的第2光脉冲的所有这是同步于所述第一光脉冲,并延迟一个预定时间的第1光脉冲的每个周期。 取样单元(27,27A,27B)接收多路复用的光以及第2光脉冲,以获得在光脉冲串信号正比于同步获得了与第2光脉冲的复用的光的强度。 从采样单元的光脉冲列信号(27,27A,27B),信号处理器(37)获取通过形成光脉冲列单独的光学脉冲的波峰形成的包络线。 对象的波长分散是通过测量穿过物体通过包络线的峰之间的间隔的基础上,输出光脉冲的延迟时间而获得。
    • 9. 发明公开
    • Optical sampling waveform measuring apparatus and polarization beam splitter which can be assembled therein
    • Optisch提出了Wellenform-Messgerätund darin verwendbarer Polarisationsstrahlteiler
    • EP1610108A3
    • 2007-03-14
    • EP05018845.7
    • 1998-09-17
    • ANRITSU CORPORATIONNIPPON TELEGRAPH AND TELEPHONE CORPORATION
    • Otani, AkihitoOtsubo, ToshinobuTakara, HidehikoKawanishi, Satoki
    • G01J11/00G02B27/28G02F1/35
    • G02B27/283G01J11/00
    • A sampling light source (10) generates a pulse sequence of sampling light having a pulse width smaller than that of target light (a) and a single plane of polarization. A polarization beam splitting unit (11) splits each of the sampling light output from the sampling light source, and the target light into two light components having planes of polarization shifted 90° from each other, multiplexes each pair of split sampling and target light components having planes of plane of polarization shifted 90° from each other, and outputs the respective multiplexed light components to different optical paths. A pair of nonlinear optical members (1a, 1b) each generate a cross-correlation signal based on the sampling and target light components output from the polarization beam splitting unit to each optical path and having planes of polarization shifted 90° from each other as sum frequency light. A pair of photodetectors (7a, 7b) each convert the sum frequency light output from each of the pair of nonlinear optical members into an electrical signal. A signal processing unit (12) adds the electrical signals output from the pair of photodetectors, processes the resultant electrical signal, and displays its pulse waveform. With this operation, the pulse waveform of the target light can be accurately measured regardless of variations in the polarized state of the target light.
    • 采样光源(10)产生具有比目标光(a)的脉冲宽度小的偏振光的脉冲宽度的采样光的脉冲序列。 偏振光束分离单元(11)将从采样光源输出的采样光中的每一个分离,并将目标光分离成具有彼此偏移90°的偏振平面的两个光分量,将每对分离采样和目标光分量 具有偏振平面的平面彼此偏移90°,并将各个复用的光分量输出到不同的光路。 一对非线性光学构件(1a,1b)基于从偏振光束分离单元输出到每个光路并且具有彼此偏移90°的平面的采样和目标光分量产生互相关信号作为总和 频率灯。 一对光电检测器(7a,7b)将从每对非线性光学部件的每一个输出的和频率光转换为电信号。 信号处理单元(12)将从一对光电检测器输出的电信号相加,处理所得的电信号,并显示其脉冲波形。 通过这种操作,无论目标光的偏振状态的变化如何,都可以精确地测量目标光的脉搏波形。