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    • 33. 发明申请
    • Fabry-perot fiber optic sensing device and method
    • 法布里 - 珀罗光纤传感装置及方法
    • US20050151975A1
    • 2005-07-14
    • US10756329
    • 2004-01-14
    • Ivan Melnyk
    • Ivan Melnyk
    • G01B9/02G01B11/16G01D5/353
    • G01B9/02023G01B9/02044G01B9/02057G01B9/0209G01B11/18G01B2290/25G01D5/35303
    • The invention provides a device and a method for measuring a physical parameter. The device comprises a Fabry-Perot interferometer coupled to a polychromatic light source via fiber optic means. Light, modulated by the Fabry-Perot cavity, is recorded by a spectrometer. A phase function is calculated by a signal processing means from the modulated spectrum. Correlation coefficients are calculated between the determined phase function and a number of theoretical phase functions calculated for a variety of gap spacing of the Fabry-Perot cavity or a number of calibrated phase functions measured for variety of values of physical parameter. The gap spacing, which is associated with the physical parameter, is determined from the best-matched phase function. The processing time is shortened by the approximate estimation of the gap spacing through the position of the maximums and minimums of the modulated spectrum and by consequent precise determining of the gap spacing through correlation.
    • 本发明提供一种用于测量物理参数的装置和方法。 该装置包括通过光纤装置耦合到多色光源的法布里 - 珀罗干涉仪。 由法布里 - 珀罗腔调制的光被光谱仪记录下来。 通过来自调制频谱的信号处理装置计算相位函数。 在确定的相位函数和针对法布里 - 珀罗腔的各种间隙间隔计算的理论相位函数的数量或针对各种物理参数值测量的多个校准相位函数之间计算相关系数。 与物理参数相关联的间隙间距由最佳匹配的相位函数确定。 通过通过调制频谱的最大值和最小值的位置的间隙间距的近似估计以及随后通过相关性精确确定间隙间距来缩短处理时间。
    • 39. 发明授权
    • Interferometer
    • 干涉仪
    • US4830496A
    • 1989-05-16
    • US146851
    • 1988-01-22
    • Niels O. Young
    • Niels O. Young
    • G01B9/02
    • G01B11/26G01B9/02019G01B2290/25
    • A reference mirror (50) in an interferometer is fixed in position with respect to a laser (34). A refractive block (40) having parallel upper and lower surfaces is mounted for pivoting about a pivot axis (60) parallel to the reference mirror (40). The refractive block (40) is disposed in the path of the light beam (36) produced by the laser (34), and it includes a partially reflective surface (42) on its lower face that divides the incident beam (36) into two components (44 and 46), which travel along different paths, in which they are reflected from different portions (48 and 54) of the surface of the reference mirror (50) and from different portions (52 and 56) of a reflective surface on the upper face of the refractive block (40). A second partially reflective coating (58) rejoins portions of the two components to form an exit beam (32) in which the radiation from the two beams interferes in accordance with the angle of the refractive block (40). The angle that the exit beam (32) makes with the surface of the reference mirror (50) is independent of the angle of the refractive block (40).
    • 干涉仪中的参考反射镜(50)相对于激光器(34)固定就位。 具有平行的上表面和下表面的折射块(40)被安装用于围绕平行于参考镜(40)的枢转轴线(60)枢转。 折射块(40)设置在由激光器(34)产生的光束(36)的路径中,并且其折射块(40)在其下表面上包括将入射光束(36)分成两部分的部分反射表面(42) 组件(44和46)沿着不同的路径行进,其中它们从参考反射镜(50)的表面的不同部分(48和54)反射并且从反射表面的不同部分(52和56) 折射块(40)的上表面。 第二部分反射涂层(58)重新结合两个部件的部分以形成出射光束(32),其中来自两个光束的辐射根据折射块(40)的角度而干涉。 出射光束(32)与参考反射镜(50)的表面形成的角度与折射块(40)的角度无关。
    • 40. 发明授权
    • Method and apparatus for optically measuring three-dimensional
coordinates
    • 用于光学测量三维坐标的方法和装置
    • US4627722A
    • 1986-12-09
    • US646638
    • 1984-08-31
    • Robert A. FalkGary L. Phillis
    • Robert A. FalkGary L. Phillis
    • G01B9/02G01B11/00
    • G01B11/002G01B9/02032G01B9/02057G01B2290/25
    • The disclosed apparatus provides a point optical radiation source (i.e. point light source), at one or more distant points, the three-dimensional coordinates of which are to be measured relative to a known frame of reference. Each point light source emits light waves of a known wavelength which are received by the front plate of a multiple-beam interferometer means having a known angle of light acceptance. With respect to the light waves transmitted by each point light source and received by the interferometer means, a set of non-localized multiple-beam interference fringes are created within the interferometer means. A photo-electric detection means is provided a known distance from the back plate of the multiple-beam interferometer means and is positioned so that the interferometer means and photo-electric detection means have a common optical center axis. The intersection of such optical center axis and the plane defined by the back plate of the interferometer means establishes the origin of the known frame of reference. The photo-electric detection means both detects the two-dimensional position of at least the innermost fringe of each set of interference fringes, and transmits the detected positional information to a processor means by electric signals. The processor means employs the electric signals to determine the coordinate values for the center point of each set of interference fringes relative to the common optical center axis, and determines the radius of the innermost fringe of each set of interference fringes. Such determinations allow the processor means to calculate the three-dimensional coordinates of the distant points relative to the known frame of reference.
    • 所公开的装置在一个或多个远点处提供相对于已知的参考系来测量三维坐标的点光源(即点光源)。 每个点光源发射已知波长的光波,其由具有已知的光接收角的多光束干涉仪装置的前板接收。 对于由每个点光源发送并由干涉仪装置接收的光波,在干涉仪装置内产生一组非局部多光束干涉条纹。 光电检测装置设置在与多光束干涉仪装置的背板已知的距离处,并且被定位成使得干涉仪装置和光电检测装置具有共同的光中心轴。 这种光学中心轴与由干涉仪装置的背板限定的平面的交点确定了已知参考系的原点。 光电检测装置检测至少每组干涉条纹的最内边缘的二维位置,并通过电信号将检测到的位置信息发送到处理器装置。 处理器装置采用电信号来确定每组干涉条纹相对于公共光学中心轴的中心点的坐标值,并且确定每组干涉条纹的最内边缘的半径。 这种确定允许处理器装置计算相对于已知参考系的远点的三维坐标。