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    • 3. 发明授权
    • Reflective optical apparatus for interconverting between a point of light and a line of light
    • 用于在光点和光线之间相互转换的反射光学装置
    • US06705737B1
    • 2004-03-16
    • US10224834
    • 2002-08-20
    • Paul K. Manhart
    • Paul K. Manhart
    • G02B510
    • G02B17/0621G02B17/0856
    • An optical apparatus includes a nonplanar light-reflecting surface having a shape referenced relative to an orthogonal axial system having an x-axis, a y-axis, and a z-axis. The light-reflecting surface has a non-circular conic profile with a conic axis and a distance f from a conic vertex to a finite focal point of the conic, wherein the non-circular conic profile is determined in a yz-plane containing the y-axis and the z-axis. The light-reflecting surface has a circular profile with a circular center and a radius of curvature r numerically equal to the distance f from the conic vertex to the finite focal point of the conic, wherein the circular profile is determined in an xz-plane containing the x-axis and the z-axis. A point light transceiver is at a transceiver location, wherein the transceiver location lies on the conic axis in the yz plane, and also at the circular center in the xz plane.
    • 光学装置包括具有相对于具有x轴,y轴和z轴的正交轴向系统参考的形状的非平面光反射表面。 光反射表面具有非圆圆锥曲线,其具有圆锥轴线和从圆锥顶点到圆锥的有限焦点的距离f,其中非圆形圆锥曲线在包含y的yz平面中确定 轴和z轴。 光反射表面具有圆形轮廓,圆形轮廓具有圆形中心和曲率半径r,其数值等于从圆锥顶点到圆锥的有限焦点的距离f,其中圆形轮廓在包含 x轴和z轴。 点光收发器位于收发器位置,其中收发器位置位于yz平面中的圆锥轴上,并且还位于xz平面中的圆形中心处。
    • 6. 发明授权
    • Liquid filled conformal windows and domes
    • 液体填充的保形窗和圆顶
    • US07019320B2
    • 2006-03-28
    • US10682578
    • 2003-10-09
    • David J. KnappPaul K. Manhart
    • David J. KnappPaul K. Manhart
    • G02B27/22
    • G01N21/0303
    • A system for sensing light transmitted with reduced optical aberrations into the interior of an enclosure utilizing a liquid filled cavity. A window is disposed on the exterior surface of the enclosure for allowing light to pass into the enclosure. A lens is disposed on the interior side of the window, defining a cavity between the window and the lens. A fluid is disposed within that cavity. An optical sensor is disposed in the interior of the enclosure, and positioned to receive light through the window and the lens. The exterior surface of the window is shaped to conform to the exterior surface of the enclosure. The fluid is selected for having an index of refraction that minimizes the mismatch with the index of refraction of the window.
    • 一种利用减少的光学像差传播的光,利用充满液体的腔体将光传感到外壳内部的系统。 在外壳的外表面上设置一个窗口,以允许光线进入外壳。 透镜设置在窗口的内侧上,在窗口和透镜之间限定空腔。 流体设置在该腔内。 光学传感器设置在外壳的内部,并被定位成通过窗口和透镜接收光。 窗口的外表面成形为符合外壳的外表面。 选择流体以具有使与窗口的折射率的失配最小化的折射率。
    • 7. 发明授权
    • Gradient refractive index lens elements
    • 渐变折射率透镜元件
    • US5617252A
    • 1997-04-01
    • US513250
    • 1995-08-10
    • Paul K. ManhartTilman W. StuhlingerKenneth R. CastleMitchell C. Ruda
    • Paul K. ManhartTilman W. StuhlingerKenneth R. CastleMitchell C. Ruda
    • G02B3/00
    • G02B3/0087
    • A lens element (40) is formed from a monolithic unit (46) having two sections (46A and 46B) aligned on an optical axis. A selected one of the sections has an axial gradient refractive index, and the other has a homogeneous refractive index. A first surface 42 is generated one section and a second surface is generated on the other. The axial gradient index material may be selected such that third order spherical aberration of the element is zero. The axial gradient index material may be selected such that similarly constructed elements having shape factors between about 0 and 2.0 also have zero third order spherical aberration. Another element (20) may be formed entirely from an axially graded refractive index material. The refractive index preferably varies as a non-linear function of at least distance along the optical axis. The refractive index function and index change may be selected such that a selected third order aberration is zero or some constant value over a wide range of shape factor. An element (98) is formed from a material having an axial gradient dispersion. Shape factor and dispersion gradient may be selected such that the element is achromatic.
    • 透镜元件(40)由具有在光轴上对准的两个部分(46A和46B)的单片单元(46)形成。 所选择的一个部分具有轴向梯度折射率,另一个具有均匀的折射率。 第一表面42产生一个部分,另一个表面另一个产生。 可以选择轴向梯度折射率材料,使得元件的三阶球面像差为零。 可以选择轴向梯度折射率材料,使得具有约0和2.0之间的形状系数的类似构造的元件也具有零三阶球面像差。 另一个元件(20)可以完全由轴向梯度折射率材料形成。 优选地,折射率作为沿着光轴的至少距离的非线性函数而变化。 可以选择折射率函数和折射率变化,使得所选择的三阶像差在宽的形状因子范围内为零或一些恒定值。 元件(98)由具有轴向梯度分散的材料形成。 可以选择形状因子和色散梯度,使得该元素是消色差的。
    • 8. 发明授权
    • Method and apparatus for phasing segmented mirror arrays
    • 分段镜阵列相位的方法和装置
    • US5113064A
    • 1992-05-12
    • US665509
    • 1991-03-06
    • Paul K. Manhart
    • Paul K. Manhart
    • G01J9/00G02B5/08
    • G02B5/08G01J9/00
    • A method and apparatus are disclosed for edge phasing an array of segments in a segmented primary telescope mirror using white light from a far field source and starting with the inner edge of each segment in the first ring of segments. The segments are individually phased for zero piston and tilt error with respect to the edge of a reference surface in the open center position of the telescope mirror, and proceeding from ring to ring by edge phasing one edge of each segment in each subsequent ring with an edge of a segment in a preceding ring that has been edge phased. After edge phasing of all segments in the telesope mirror array has been completed, full surface phasing can be achieved using a conventional Shack-Hartmann technique followed by finding the RMS best fit for each segment of the mirror array.
    • 公开了一种方法和装置,用于使用来自远场源的白光并且从第一环段中的每个段的内边缘开始,在分段的主望远镜中的边缘阵列的边缘定相。 这些段相对于望远镜的开放中心位置处的参考表面的边缘处于零活塞和倾斜误差,并且从环到环通过在每个后续环中的每个段的一个边缘相位定位 在前一个环中已经被边缘化的段的边缘。 在电视镜镜阵列中的所有片段的边缘定相已经完成之后,可以使用常规的Shack-Hartmann技术实现全表面定相,然后找到镜阵列的每个片段的RMS最佳拟合。
    • 9. 发明授权
    • Equal path, phase shifting, sample point interferometer for monitoring
the configuration of surfaces
    • 等路径,相移,采样点干涉仪,用于监测表面的配置
    • US5080490A
    • 1992-01-14
    • US527509
    • 1990-05-23
    • Paul K. Manhart
    • Paul K. Manhart
    • G01B9/02G01B11/255
    • G01B9/0201G01B11/255G01B9/02011G01B9/02019G01B9/02027G01M11/005G01B2290/15G01B2290/70
    • A system for monitoring the configuration of a surface (e.g., a segmented parabolic surface) using orthogonally placed retroreflectors at sets of points A, B and C dispersed throughout the surface with a stationary halfwave plate HWP in the front of the one retroreflector at a corner point C and a rotating halfwave plate RHWP over a source of linearly polarized coherent light, thereby causing the direction of linear polarization to continuously rotate through 360.degree. and causing light returned by the retroreflector at point C to be continuously phase shifted through 360.degree. relative to light returned by retroreflectors at points A and B. The returned light from each set of points A. B and C is focused onto a bed-of-nails (BON) phase grating diagonally oriented with respect to the orthogonal orientation of the incident beams from retroreflectors A, B and C, thereby causing overlap in the light from points A and C and from points B and C to produce interferometric signals AC and BC. Any change in phase of the interferometric signals AC and BC indicates both the magnitude and direction of any change in the position of the retroreflector at point C relative to retroreflectors at points A and B.
    • 一个系统,用于使用正交放置的回射器在一组分布在整个表面上的点A,B和C中的一个表面(例如,分段的抛物线表面)的配置,该固定半波片HWP位于一个后向反射器的前部的角部 点C和旋转半波片RHWP在线偏振相干光源上,从而使线偏振方向连续旋转360度,并使由点反射器返回的光在C点连续相移360度相对于 点A和B由后向反射器返回的光。来自每组点A.B和C的返回光聚焦到相对于入射光束的正交取向对角定向的指甲(BON)相位光栅上 后向反射器A,B和C,从而在来自点A和C以及从点B和C的光中引起重叠以产生干涉信号AC和BC。 干涉测量信号AC和BC的任何相位变化都指示回归反射器在点C相对于后点反射器在点A和B处的位置的任何变化的大小和方向。