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    • 4. 发明申请
    • POLARIZATION RECOVERY SYSTEM FOR PROJECTION DISPLAYS
    • 用于投影显示的偏振恢复系统
    • WO0217000A2
    • 2002-02-28
    • PCT/US0123758
    • 2001-07-30
    • COGENT LIGHT TECHLI KENNETH K
    • LI KENNETH K
    • G02B5/30G02B27/28G02F1/13G02F1/1335G02F1/13357G03B21/00H04N5/74H04N9/31G02B27/00
    • H04N9/3167G02B6/4298G02B27/1033G02B27/145G02B27/149G02B27/283G02B27/285G02B27/286H04N5/7441H04N9/3102H04N9/3152
    • A waveguide polarization recovery system both polarizes the input light energy for use with an LCD imager and converts the polarity of unusable light energy to add to the illumination of the LCD imager. The compact polarization recovery waveguide system generally includes: (1) an input waveguide that provides non-polarized light energy into the system; (2) an output waveguide that receives polarized light energy from the system; (3) a polarized beam splitter that received the light energy from the input waveguide and transmits lights energy of a first polarization type and reflects light energy of a second polarization type, and (4) a wave plate that modifies the polarization of either the transmitted or reflected light energy. The polarization recovery system also generally includes one or more mirrors that are positioned as need to direct the transmitted and the reflected light energy to the output waveguide. The input and output waveguides may be shaped as needed by the projection system. For example, either one or both of the input and output waveguides may be tapered as needed to produce a desired image. In the waveguide polarization recovery system, the input and output waveguides are configured to have either an either a substantially parallel or a substantially perpendicular orientation. In another embodiment, the waveguide polarization recovery system further includes has one or more "gaps" of optically clear material positioned between the optical components to encourage the occurrence of total internal reflection that minimizes the loss of the optical energy by the system.
    • 波导偏振恢复系统使输入光能量偏振,以与LCD成像器一起使用,并且将不可用的光能的极性转换成LCD成像器的照明。 紧凑型偏振恢复波导系统通常包括:(1)向系统中提供非偏振光能的输入波导; (2)从系统接收偏振光能的输出波导; (3)偏振光束分离器,其从输入波导接收光能并透射第一偏振光类型的光能并反射第二偏振光类型的光能,以及(4)波片,其修改透射的 或反射光能。 偏振恢复系统还通常包括一个或多个反射镜,其被定位成需要将透射的和反射的光能引导到输出波导。 输入和输出波导可以根据投影系统的需要进行成形。 例如,输入和输出波导中的一个或两个可以根据需要被锥形以产生期望的图像。 在波导偏振恢复系统中,输入和输出波导被配置为具有基本上平行的或基本垂直的取向。 在另一个实施例中,波导偏振恢复系统还包括具有位于光学部件之间的光学透明材料的一个或多个“间隙”,以促进发生全内反射,从而最小化系统的光能损失。
    • 5. 发明申请
    • CONCENTRATING AND COLLECTING OPTICAL SYSTEM USING CONCAVE TOROIDAL REFLECTORS
    • 使用凹凸反射器集中和收集光学系统
    • WO0022344A9
    • 2002-08-22
    • PCT/US9922272
    • 1999-09-27
    • COGENT LIGHT TECH
    • BAKER GLENNBRENNER DOUGLAS M
    • G02B6/26F21V8/00F21V13/04G02B5/08G02B17/08G02B19/00
    • G02B6/0006
    • An electromagnetic radiation source (SO), such as an arc lamp, is located at a point displaced from the optical axis of a concave toroidal reflecting surface (M1). The concave primary reflector (M1) focuses the radiation from the source (SO) at an off-axis image point that is displaced from the optical axis. The use of a toroidal reflecting surface enhances the collection efficiency into a small target (T), such as an optical fiber, relative to a spherical reflecting surface by substantially reducing aberrations caused by the off-axis geometry. A second concave reflector (M2) is placed opposite to the first reflector (M1) to enhance further the total flux collected by a small target (T). In accordance with one embodiment, the present invention is directed to devices in which the square of the off-axis distance divided by the radius of curvature is equal to or less than the extent of the source of electromagnetic radiation (yo /r
    • 诸如弧光灯的电磁辐射源(SO)位于从凹面环形反射面(M1)的光轴偏离的点上。 凹形初级反射器(M1)将来自源极(SO)的辐射聚焦在离开光轴的偏轴图像点上。 环形反射表面的使用通过基本上减少由离轴几何形状引起的像差而将相对于球面反射表面的收集​​效率提高到诸如光纤的小目标(T)中。 第二凹面反射器(M2)与第一反射器(M1)相对设置,以进一步增强由小目标(T)收集的总通量。 根据一个实施例,本发明涉及离轴距离除以曲率半径的平方等于或小于电磁辐射源的程度的装置(yo 2 / r <左右)。
    • 9. 发明申请
    • LIGHT CONDENSING AND COLLECTING SYSTEMS USING LENSED LIGHT PIPES
    • 使用透光灯管的光凝和收集系统
    • WO0225329A3
    • 2003-04-10
    • PCT/US0129314
    • 2001-09-20
    • COGENT LIGHT TECHLI KENNETH K
    • LI KENNETH K
    • G02B27/00F21V8/00G02B6/42G02B19/00F21V7/04G02B5/10G02B17/00
    • G02B6/0006G02B6/4206G02B6/4298G02B19/0028G02B19/0047
    • An optical coupling element for use in large numerical aperture collecting and condensing systems. The optical coupling element includes a lens (503) having a curved surface and a tapered light pipe (504). The curved surface reduces the angle of incidence of the light striking the input end of the optical coupling element such that the Fresnel reflection is greatly reduced. Electromagnetic radiation emitted by a source (506) is collected and focused onto a target by positioning the source of electromagnetic radiation at a first focal point of a first reflector (508a) so that the source produces rays of radiation reflected from the first reflector that converge at a second focal point (511) of the second reflector (508b). The optical coupling element is positioned so that a center (507) of the lens is substantially proximate with the second focal point of the second reflector and the curved surface (505) is between the second reflector and the center. The converging rays of radiation reflected from the second reflector pass through the curved surface of the lens and reach the center.
    • 用于大数值孔径收集和冷凝系统的光耦合元件。 光耦合元件包括具有弯曲表面的透镜(503)和锥形光管(504)。 弯曲表面减小了光入射到光耦合元件的输入端的入射角,使得菲涅尔反射大大减小。 通过将电磁辐射源定位在第一反射器(508a)的第一焦点处,使源(506)发射的电磁辐射被聚集并聚焦到目标上,使得光源产生会聚的第一反射器反射的辐射光线 在第二反射器(508b)的第二焦点(511)处。 光学耦合元件被定位成使得透镜的中心(507)基本上与第二反射器的第二焦点接近,并且弯曲表面(505)在第二反射器和中心之间。 从第二反射镜反射的辐射的会聚射线穿过透镜的曲面并到达中心。