会员体验
专利管家(专利管理)
工作空间(专利管理)
风险监控(情报监控)
数据分析(专利分析)
侵权分析(诉讼无效)
联系我们
交流群
官方交流:
QQ群: 891211   
微信请扫码    >>>
现在联系顾问~
热词
    • 21. 发明公开
    • Method and system for optical heterodyne detection of an optical signal
    • Verfahren und System zur optischenÜberlagerungsdetektioneines optischen Signals
    • EP1193483A2
    • 2002-04-03
    • EP01117550.2
    • 2001-07-20
    • Agilent Technologies, Inc. (a Delaware corporation)
    • Sorin, Wayne V.Szfraniec, BogdanBaney, Douglas M.
    • G01J9/04
    • H04B10/60G01J9/04H04B10/64
    • An optical heterodyne detection system in accordance with an embodiment of the invention includes two optical receivers (232 and 242) for separately measuring the power of an input signal (202) and a local oscillator signal (206) before the signals are combined. The measurements of the input signal and the local oscillator signal are then utilized by a processor (216) to enhance the heterodyne signal to noise ratio by removing the intensity noise contributed by the input signal and the local oscillator signal. By measuring portions of the input signal power and the local oscillator signal power and then subtracting out the scaled quantities from the photocurrent measurement during signal processing, the signal to noise of the heterodyne signal is improved beyond that which is accomplished by known balanced receivers.
    • 根据本发明实施例的光外差检测系统包括两个用于在信号组合之前分别测量输入信号(202)和本地振荡器信号(206)的功率的光接收器(232和242)。 输入信号和本地振荡器信号的测量然后由处理器(216)利用,以通过去除由输入信号和本地振荡器信号贡献的强度噪声来增强外差信噪比。 通过测量输入信号功率和本地振荡器信号功率的部分,然后在信号处理期间从光电流测量中减去量化的量,外差信号的信噪比被改进超过了已知的平衡接收机完成的信噪比。
    • 26. 发明授权
    • ZWEI-WELLENLÄNGEN-INTERFEROMETRIE MIT OPTISCHEM HETERODYNVERFAHREN
    • 具有光学异质性过程的双波长干涉
    • EP0314709B1
    • 1992-03-11
    • EP88902383.4
    • 1988-03-30
    • Leica Heerbrugg AG
    • DÄNDLIKER, René
    • G01J9/04G01B9/02
    • G01B9/02007G01B9/02003G01B9/02027G01B9/02067G01B2290/70G01J9/04G01J2009/0207G01J2009/0253G01J2009/0261
    • The device comprises : a laser device (10, 20) for the frequency n1 (11) and the frequency n2 (21), each provided with a polarizing beam splitter (12, 22) for producing crossed polarized partial beams of frequency n1 (13, 14) and n2 (23, 24), respectively, with a modulator (18, 28) for shifting the frequency of each of the partial beams to the frequency f1 or f2, respectively, with a pair of deflecting mirrors (15, 17, 25, 27) and with a polarizing beam splitter (16, 26) for uniting (19, 29) the partial beams n1, n1+f1, n2, n2+f2; two photodetectors (35, 45) before each of which a polarizer (34, 44) is arranged; a Michelson interferometer; a non-polarizing beam splitter (30) for distributing each of the partial beams (19, 29) into a measurement light beam (32) or a reference light beam (33). The reference light beam is transmitted to the corresponding photodetector (35). The measurement light beam (32) is transmitted to the Michelson interferometer and then to the corresponding photodetector (45).The photodetector signals are modulated in function of the amplitude, and the phase difference between the two modulated signals is determined. This phase difference depends only on the position of the test object and the equivalent wavelenght of the difference, n1-n2. For stabilization or correction, the device can be executed in duplicate and one of the executions used as a reference. The corresponding process can be applied to determine positions or distances as the interval between two positions. Uncertainties can be eliminated by shifting the distance or changing the frequency with simultaneous integration of the phase difference over time.
    • 27. 发明公开
    • Frequency detector for discriminating multi-longitudinal mode laser operation
    • 激光Bet。。。。。。。。。。。。。。。。。。。。。
    • EP0428924A2
    • 1991-05-29
    • EP90121017.9
    • 1990-11-02
    • Hughes Aircraft Company
    • Ottusch, John J.
    • G01J9/04G02F2/00H01S3/00G01R23/14
    • G01J9/04G01J2009/004
    • A photodetector produces an output signal in response to irradiation by an optical beam from a pulled laser. A delay unit delays the output signal for a period corresponding to one-half of one cycle of a beat frequency generated by interaction of two frequency components in the optical beam corresponding to two predetermined longitudinal modes of operation of the laser. A differential mixer subtractively combines the output of the photodetector with the output of the delay unit, to produce an output signal having the main profile of the laser pulses suppressed, and the beat frequency component, if present, amplified. A resonant circuit and amplifier may be provided to further amplify the beat frequency component. The output of the amplifier is integrated to produce a DC signal having a magnitude which corresponds to the amplitude of the beat frequency component. The DC signal is compared with a threshold value to discriminate between single and multi-mode operation of the laser. An optical shutter may be closed in response to sensed multi-longitudinal mode operation to block the laser beam and protect equipment which would otherwise be damaged thereby.
    • 光电检测器响应于来自拉动激光器的光束的照射而产生输出信号。 延迟单元将对应于对应于激光器的两个预定纵向工作模式的光束中的两个频率分量的相互作用产生的拍频的一个周期的一半周期延迟输出信号。 差分混频器将光电检测器的输出与延迟单元的输出相减,以产生抑制激光脉冲的主要轮廓的输出信号,并且如果存在则将拍频分量放大。 可以提供谐振电路和放大器以进一步放大拍频分量。 放大器的输出被积分以产生具有对应于节拍频率分量的振幅的幅度的DC信号。 将DC信号与阈值进行比较,以区分激光器的单模式和多模式操作。 可以响应于感测的多纵模式操作来闭合光学快门来阻挡激光束并保护否则将由此损坏的设备。
    • 28. 发明公开
    • Emission spectral width measuring apparatus for light source
    • 用于光源的发射光谱宽度测量装置
    • EP0297556A3
    • 1991-03-06
    • EP88110398.0
    • 1988-06-29
    • ANRITSU CORPORATION
    • Sonobe, Yoji
    • G01J9/04
    • G01J9/04
    • A measurement beam emitted from a laser diode is split into two beams by a beam splitter (12), and one of the two beams is guided to a first port (201) of an acoustic optical element (20). When a high-frequency signal is applied from a diffraction controller (22) to a piezoelectric transducer (205), the split beam input into the acoustic optical element (20) from the first port (201) is diffracted and frequency-shifted and output from a second port (202). If the high-frequency signal is not applied, the input beam rectilinearly pro­pagates without diffracting and is output from a third port (203). This output beam is guided to a fourth port (204) through an optical fiber (24). The beam input from the fourth port (204) rectilinearly propaga­tes and is output from the second port (202). The beam output from the second port (202) is mixed with the other measurement beams split by the beam splitter (12) to be converted to an electrical signal. The electrical signal is analyzed by a spectrum analyzer (28). When the high-frequency signal is applied to the piezoelectric transducer (205), measurement using an optical heterodyne spectroscopy is performed, and when the high-frequency signal is not applied, measurement using an optical homodyne spectroscopy is performed.