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    • 1. 发明授权
    • Fiber fourier spectrometer
    • 光纤光谱仪
    • US4558951A
    • 1985-12-17
    • US465229
    • 1983-02-09
    • Jacques E. LudmanJohn L. SampsonHenry J. Caulfield
    • Jacques E. LudmanJohn L. SampsonHenry J. Caulfield
    • G01J3/453G01J3/45
    • G01J3/453G01J3/0218
    • A fiber Fourier spectrometer having a focusing element, a beamsplitter, a pair of monomode optical fibers, a block of electro-optic material defining a pair of optical paths and means for controlling the effective length of one of the optical paths. A source of electromagnetic radiation is focused through and reflected by the beamsplitter into the pair of monomode fibers, respectively, and from there to the respective optical paths within the electro-optic block of material. The outputs of the two optical paths are combined and received by an intensity detector. Varying the effective path length of one of the optical paths alters the phase of the beam passing therethrough. Because the source of electromagnetic radiation has different wavelengths, the spectral components of the source are phase retarded by different amounts as they pass through the electro-optic material and can therefore be analyzed by a conventional Fourier spectroscopy technique.
    • 具有聚焦元件,分束器,一对单模光纤,限定一对光路的电光材料块的光纤傅立叶光谱仪和用于控制一个光路的有效长度的装置。 电磁辐射源分别聚焦到分束器中并通过分光器反射到一对单模光纤中,并从那里到电光学材料块内的各个光路。 两个光路的输出由强度检测器组合和接收。 改变光路中的一个的有效路径长度改变通过其中的光束的相位。 因为电磁辐射源具有不同的波长,所以源的光谱分量在它们通过电光材料时被相位延迟不同的量,因此可以通过常规的傅立叶光谱技术进行分析。
    • 2. 发明授权
    • Fiber stellar interferometer
    • 纤维恒星干涉仪
    • US4505588A
    • 1985-03-19
    • US465215
    • 1983-02-09
    • Jacques E. LudmanJohn L. SampsonHenry J. Caulfield
    • Jacques E. LudmanJohn L. SampsonHenry J. Caulfield
    • G01B9/02G01J9/02
    • G01J9/02G01B9/02063G01B2290/10G01B2290/40G01J2009/0226
    • A fiber stellar interferometer having a pair of adjustably movable focusing lenses, a pair of monomode optical fibers, a block of electro-optic material defining a pair of optical paths, means for controlling the effective path length of one of the optical paths and an intensity detector. Electromagnetic radiation emanating from a source, such as a star, is received at two separate locations by the focusing lenses which direct this electromagnetic radiation into two separate beams which are focused into each of the pair of monomode fibers, respectively. The monomode fibers direct these two beams into respective optical paths within the electro-optic block of material. The outputs from the two optical paths are combined and received by the intensity detector. Varying the effective path length of one of the optical paths alters the phase of the beam passing therethrough. As a consequence thereof the intensity of the output received by the detector varies accordingly. These varying intensities can be utilized to determine the size and shape of the source by conventional stellar intensity interferometer techniques.
    • 一种具有一对可调节移动聚焦透镜的光纤恒星干涉仪,一对单模光纤,限定一对光路的电光材料块,用于控制一条光路的有效路径长度和强度 探测器。 从诸如恒星的源发出的电磁辐射通过聚焦透镜在两个分开的位置处被接收,该聚焦透镜将该电磁辐射分别引导到分别聚焦到该对单模光纤中的每一个中的两个单独的光束。 单模光纤将这两个光束引导到电光学材料块内的相应的光路中。 来自两个光路的输出被强度检测器组合和接收。 改变光路中的一个的有效路径长度改变通过其中的光束的相位。 因此,由检测器接收的输出的强度相应地变化。 这些变化的强度可以用于通过传统的恒星强度干涉仪技术来确定源的尺寸和形状。
    • 4. 发明授权
    • Holographic coupler for fiber optic systems
    • 光纤系统的全息耦合器
    • US4398792A
    • 1983-08-16
    • US231088
    • 1981-02-03
    • Joseph L. HornerJacques E. Ludman
    • Joseph L. HornerJacques E. Ludman
    • G02B5/32G02B6/42G02B7/26
    • G02B6/4204G02B5/32G02B6/4206G02B6/4226
    • A holographic coupler for fiber optic systems having a holographic element utilized in conjunction with an optical source and an optical fiber in order to direct and couple the beam emanating from the optical source into the fiber. The holographic element, source and optical fiber have the same relative position with respect to each other as (1), a photosensitive medium, (2) a means for sizing and shaping a beam of temporally and spatially coherent radiation to the same geometry as the optical source before the beam impinges upon the photosensitive medium, and (3) the focal point of a converging beam of temporally and spatially coherent radiation impinging upon the photosensitive medium during the making of the holographic element used with the coupler.
    • 一种用于光纤系统的全息耦合器,其具有与光源和光纤结合使用的全息元件,以将从光源发出的光束引导和耦合到光纤中。 全息元件,光源和光纤相对于彼此具有相同的相对位置(1),光敏介质,(2)用于将时间和空间相干辐射束定尺寸和成形为与 在光束照射到感光介质之前的光源,以及(3)在与耦合器一起使用的全息元件的制造期间,入射到感光介质上的会聚光束的时间和空间相干辐射的焦点。
    • 5. 发明授权
    • Interferometer optical system
    • 干涉仪光学系统
    • US4056323A
    • 1977-11-01
    • US564498
    • 1975-04-02
    • Jacques E. Ludman
    • Jacques E. Ludman
    • G01B9/02G01B11/26
    • G01B11/26G01B9/02021G01B9/02024
    • An interferometer optical system for general use to measure optical parallelism or relative rotational or joint translational positions of the two spaced subject mirrors uses coherent light split into two beams which are directed, one normal to one of the two mirrors and the other normal to the other of the two mirrors. The reflections of these two beams are then superimposed on a target which reveals a light interference pattern indicative of the parallelism or relative rotation or joint translation of the two mirrors. In preferred embodiments, in order to compensate for the mutual tilt of the subject mirrors with respect to the plane of the beams incident thereon, the path of one of the beams to and from the subject mirror includes a corner mirror, or retrodirective mirror, and the path of the other beam includes at least one adjustable mirror.
    • 通常用于测量两个间隔的对象镜的光学平行度或相对旋转或联合平移位置的干涉仪光学系统使用相干光分为两个光束,一个垂直于两个反射镜之一,另一个垂直于另一个 的两个镜子。 然后将这两个光束的反射叠加在目标上,该目标显示指示两个反射镜的平行度或相对旋转或联合平移的光干涉图案。 在优选实施例中,为了补偿目标反射镜相对于入射在其上的光束的平面的相互倾斜,光束中的一个光束与被摄体反射镜之间的路径包括角镜或反射镜,以及 另一个光束的路径包括至少一个可调镜。
    • 6. 发明授权
    • Interferometric angular measurement system
    • 干涉角度测量系统
    • US4516854A
    • 1985-05-14
    • US326857
    • 1981-12-03
    • Jacques E. Ludman
    • Jacques E. Ludman
    • G01B11/26
    • G01B11/26
    • An interferometric system for general use to measure the angular relationship of two surfaces of the same object, or of different objects, or the relative angular change of one surface with respect to another. This device uses coherent light, a set of mirrors aligned as a Ludman Interferometer, and a reference pair of mirrors with a well known fixed angle similar to that of the angle of the sample pair to be measured. In preferred embodiments, the fixed angle mirror pair has a fine tilt adjustment to facilitate the interpretation of the output fringe pattern.
    • 用于一般用于测量相同物体或不同物体的两个表面的角度关系或一个表面相对于另一个的相对角度变化的干涉测量系统。 该装置使用相干光,一组与Ludman干涉仪对准的反射镜,以及具有与待测量样品对的角度相似的公知固定角度的参考对镜。 在优选实施例中,固定角度镜对具有精细的倾斜调整以便于解释输出条纹图案。
    • 9. 发明授权
    • Optical electromagnetic radiation detector
    • 光电磁辐射探测器
    • US4533829A
    • 1985-08-06
    • US511592
    • 1983-07-07
    • William J. MiceliJacques E. Ludman
    • William J. MiceliJacques E. Ludman
    • G01J5/10G01R29/08G02F1/03G02F1/21G02B5/14
    • G01J5/10G01R29/0885G02F1/03G02F2001/213
    • An optical electromagnetic radiation detector having a probe for receiving nearby electromagnetic radiation. The probe includes a loop antenna connected to a pair of transparent electrodes deposited on the end surfaces of an electro-optic Fabry-Perot interferometer. When the loop antenna picks up the presence of electromagnetic radiation, a voltage will be developed across the crystal of the electro-optic Fabry-Perot interferometer thereby changing the optical length of the interferometer. A beam of light from a remote location is transmitted through an optical fiber onto the Fabry-Perot interferometer. The change in optical length of the Fabry-Perot interferometer alters the intensity of the beam of light as it is reflected from the Fabry-Perot interferometer back through the optical fiber to the remote location. A beamsplitter directs this reflected beam of light onto an intensity detector in order to provide an output indicative of the variations in intensity. The variations in intensity are directly related to the strength of the electromagnetic radiation received by the loop antenna.
    • 一种具有用于接收附近电磁辐射的探针的光学电磁辐射检测器。 探头包括连接到沉积在电光法布里 - 珀罗干涉仪的端表面上的一对透明电极的环形天线。 当环形天线拾取电磁辐射的存在时,将跨越电光法布里 - 珀罗干涉仪的晶体产生电压,从而改变干涉仪的光学长度。 来自远程位置的光束通过光纤传输到法布里 - 珀罗干涉仪上。 法布里 - 珀罗干涉仪的光学长度变化会改变光束的强度,因为它从法布里 - 珀罗干涉仪反射回光纤到远程位置。 分束器将该反射光束引导到强度检测器上,以提供表示强度变化的输出。 强度的变化与环形天线接收的电磁辐射的强度直接相关。