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    • 3. 发明授权
    • Optical synchronizer
    • 光同步器
    • US07715724B2
    • 2010-05-11
    • US11057365
    • 2005-02-15
    • Shigeki WatanabeMasataka Nakazawa
    • Shigeki WatanabeMasataka Nakazawa
    • H04B10/00
    • H04B10/25137
    • The phase modulation in which the frequency chirp becomes 0 at the timing which the user wants to synchronize, and the frequency chirp becomes larger as the time deviates in a positive or negative direction from this timing is applied to the signal light with each wavelength comprising pulse train of different timing. Thus, the optical pulses which deviate from the timing which the user wants to synchronize receive the frequency chirp in accordance with the amount of the timing deviation. The WDM signal light which has been chirped in this way is made to pass a linear dispersive medium, and the dispersion fit for the amount of frequency chirp is made to be given. By adjusting the amount of dispersion, it is possible to obtain the pulses which conform to the timing at which the user wants to synchronize the pulses of each wavelength.
    • 在用户想要同步的定时,频率啁啾变为0的相位调制,并且随着从该定时向正或负方向偏离的时间,频率啁啾变大,对每个波长包括脉冲的信号光 不同时间的火车 因此,偏离用户想要同步的定时的光脉冲根据定时偏差量接收频率啁啾声。 已经以这种方式啁啾的WDM信号光通过线性色散介质,并且给出了频率啁啾量的色散配合。 通过调整色散量,可以获得符合用户想要使每个波长的脉冲同步的定时的脉冲。
    • 4. 发明申请
    • LASER OSCILLATOR
    • 激光振荡器
    • US20100067100A1
    • 2010-03-18
    • US12422758
    • 2009-04-13
    • Kazunori ShiotaShin MasudaMasataka NakazawaMasato Yoshida
    • Kazunori ShiotaShin MasudaMasataka NakazawaMasato Yoshida
    • H04B10/17H01S3/00
    • H01S3/06791H01S3/0675H01S3/08H01S3/094042H01S3/1109H01S3/1118
    • A laser oscillator includes a ring resonator. The ring resonator includes an optical circulator having first, second, third, and fourth ports and a first optical amplification fiber connected to the optical circulator. Light incident on the first port is exited from the second port, and light incident on the second port is exited from the third port. The fourth port provides an exciting light and injects the exciting light into the ring resonator through the first port. The first optical amplification fiber amplifies light exited from the third port with the exciting light provided by the fourth port. The laser oscillator also includes an optical member connected to the optical circulator. The optical member reflects at least a part of the light exited from the second port and injects the same into the second port again.
    • 激光振荡器包括环形谐振器。 环形谐振器包括具有第一,第二,第三和第四端口的光循环器和连接到光循环器的第一光放大光纤。 第一个港口的光线从第二个港口出发,第二个港口的光线从第三个港口出来。 第四个端口提供激发光,并通过第一个端口将激发光注入环形谐振器。 第一光放大光纤利用由第四端口提供的激发光放大从第三端口退出的光。 激光振荡器还包括连接到光循环器的光学构件。 光学构件反射从第二端口退出的光的至少一部分,并再次将其注入第二端口。
    • 5. 发明申请
    • Optical fourier transform device and method
    • 光学傅立叶变换装置及方法
    • US20070273958A1
    • 2007-11-29
    • US10584932
    • 2004-12-27
    • Toshihiko HirookaMasataka Nakazawa
    • Toshihiko HirookaMasataka Nakazawa
    • G02F1/35
    • G02F1/3515G01J11/00
    • Optical Fourier transform is executed over a wide time range. A quadratic function type optical pulse generator (7) generates a control light pulse of a shape expressed by a quadratic function or a parabola according to a clock signal based on a signal light pulse from an optical coupler (1). The signal light pulse inputted is multiplexed by a multiplexer (9) with the control light pulse optically delayed by an optical delay element (8) so that the timing is matched with the signal light pulse, and introduced into an optical Kerr medium (10). In the optical Kerr medium (10), the signal light pulse inputted by the mutual phase modulation between the signal light pulse and the control light pulse is subjected to a linear phase modulation (frequency chirp) over the entire pulse or a wide time range. After that, the signal light pulse isolated by an optical filter (11) is introduced into the dispersion medium (12) having a group velocity dispersion (secondary dispersion), thereby converting the time waveform of the inputted signal light pulse into the shape of the frequency spectrum.
    • 光学傅里叶变换在较宽的时间范围内执行。 二次函数型光脉冲发生器(7)根据来自光耦合器(1)的信号光脉冲的时钟信号产生由二次函数或抛物线表示的形状的控制光脉冲。 输入的信号光脉冲由多路复用器(9)与由光延迟元件(8)光延迟的控制光脉冲进行复用,使得定时与信号光脉冲匹配,并被引入光学克尔介质(10) 。 在光学克尔介质(10)中,通过信号光脉冲和控制光脉冲之间的相位调制输入的信号光脉冲在整个脉冲或宽时间范围内经受线性相位调制(频率啁啾)。 之后,将由滤光器(11)隔离的信号光脉冲引入到具有组速度色散(二次色散)的分散介质(12)中,从而将输入的信号光脉冲的时间波形转换为 频谱。
    • 6. 发明授权
    • Optical pulse compressor, optical function generator, optical pulse compression method, and optical function generation method
    • 光脉冲压缩机,光学函数发生器,光脉冲压缩法,光学函数生成法等
    • US07428096B2
    • 2008-09-23
    • US10553649
    • 2004-03-23
    • Masataka NakazawaToshihiko Hirooka
    • Masataka NakazawaToshihiko Hirooka
    • G02F1/35G02F2/02
    • H01S3/0057G02F1/0553G02F2203/26H04B10/508
    • A small-sized, high-functionality optical pulse compressor capable of generating a low-power, high-repetition-frequency ultrashort pulse train used for ultrafast optical communication and photometry, and a simple-structure optical function generator for realizing an arbitrary time waveform. The optical pulse compressor comprises and optical Fourier transform device (F) having an optical phase modulator (9) driven by the repetition-frequency of an input optical pulse train and a dispersive medium (8), for converting the shape of an input optical pulse frequency spectrum into its time waveform, and an optical filter (3) inserted ahead of the optical Fourier transform device (F), for reducing the spectrum width of an input optical pulse, wherein the optical Fourier transform device (F) converts a small-spectrum-width optical pulse output from the optical function generator generates an optical pulse. The optical function generator generates an optical pulse having an arbitrary time waveform by reproducing, as it is, a spectrum waveform-shaped arbitrarily by an optical filter on a time-axis by the optical Fourier transform device (F).
    • 一种能够产生用于超快速光通信和光度测量的低功率,高重复频率超短脉冲串的小尺寸,高功能的光脉冲压缩器,以及用于实现任意时间波形的简单结构的光学函数发生器。 光脉冲压缩机包括具有由输入光脉冲串的重复频率驱动的光相位调制器(9)和色散介质(8)的光学傅里叶变换装置(F),用于转换输入光脉冲的形状 频谱到其时间波形,以及插入光傅立叶变换装置(F)前面的滤光器(3),用于降低输入光脉冲的光谱宽度,其中光傅里叶变换装置(F) 来自光学函数发生器的光谱宽度光脉冲输出产生光脉冲。 光学函数发生器通过由傅里叶逆变换装置(F)在时间轴上任意地再现由光学滤波器任意地形成的波形波形,产生具有任意时间波形的光脉冲。
    • 8. 发明申请
    • Optical synchronizer
    • 光同步器
    • US20050185965A1
    • 2005-08-25
    • US11057365
    • 2005-02-15
    • Shigeki WatanabeMasataka Nakazawa
    • Shigeki WatanabeMasataka Nakazawa
    • G02F1/05G02F1/35G02F3/00H04B10/25H04B10/29H04B10/508H04B10/516H04B10/548H04B10/58H04B10/61H04B10/00
    • H04B10/25137
    • The phase modulation in which the frequency chirp becomes 0 at the timing which the user wants to synchronize, and the frequency chirp becomes larger as the time deviates in a positive or negative direction from this timing is applied to the signal light with each wavelength comprising pulse train of different timing. Thus, the optical pulses which deviate from the timing which the user wants to synchronize receive the frequency chirp in accordance with the amount of the timing deviation. The WDM signal light which has been chirped in this way is made to pass a linear dispersive medium, and the dispersion fit for the amount of frequency chirp is made to be given. By adjusting the amount of dispersion, it is possible to obtain the pulses which conform to the timing at which the user wants to synchronize the pulses of each wavelength.
    • 在用户想要同步的定时,频率啁啾变为0的相位调制,并且随着从该定时向正或负方向偏离的时间,频率啁啾变大,对每个波长包括脉冲的信号光 不同时间的火车 因此,偏离用户想要同步的定时的光脉冲根据定时偏差量接收频率啁啾声。 已经以这种方式啁啾的WDM信号光通过线性色散介质,并且给出了频率啁啾量的色散配合。 通过调整色散量,可以获得符合用户想要使每个波长的脉冲同步的定时的脉冲。
    • 9. 发明授权
    • Optical pulse generator
    • US6101021A
    • 2000-08-08
    • US349225
    • 1999-07-08
    • Yoshihiro KumagaiAkio IchikawaRikihiro IidaMasataka NakazawaEiji Yoshida
    • Yoshihiro KumagaiAkio IchikawaRikihiro IidaMasataka NakazawaEiji Yoshida
    • G02F1/01H01S3/06H01S3/067H01S3/07H01S3/083H01S3/098H01S3/10G02F1/00
    • H01S3/06791H01S3/1109H04B10/503H04B10/508H04B10/564G02F2203/26H01S3/06754H01S3/10038H01S3/1121H01S3/136
    • According to the present invention, damage to a photo-detector disposed in clock signal extractor by means of an optical pulse having an optical power exceeding a rated value is prevented. A ring resonator generates a repetitive, high-frequency optical pulse. Optical branching circuit branches a portion of the optical pulse circulating through ring resonator, while optical branching circuit further branches a portion thereof to protective device. Pumping source generates an excitation light for exciting a rare-earth doped optical fiber. Optical multiplexer couples the optical pulse branched by optical branching circuit, and the excitation light. Upon excitation by means of the excitation light, rare-earth doped optical fiber amplifies and emits the incoming optical pulse. The optical power of the excitation light is adjusted such that the output of rare-earth doped optical fiber reaches a saturation power. Optical switch blocks the incoming optical pulse during the time period when pumping source is not emitting an excitation light, and during a fixed time period following the emission of the excitation light. In this manner, the entry of an excessively large optical pulse exceeding the saturation power into photo-detector at the time of starting up the power source is prevented. Optical attenuator attenuates the optical power of the optical pulse emitted from optical switch to an optical power which the photo-detector is capable of photo-detecting. Photo-detector converts the optical pulse emitted from protective device into an electronic signal; narrow band filter extracts a clock signal from the output of photo-detector; and electric amplifier amplifies the output of narrow band filter, and outputs a clock signal. Phase shifter adjusts the phase of this clock signal; electric amplifier amplifies the output of phase shifter, and outputs a clock signal to optical modulator. Optical modulator modulates the intensity of the light circulating through the ring resonator based on the clock signal, and generates an optical pulse.