RECEPTACLE FERRULE ASSEMBLIES WITH GRADIENT INDEX LENSES AND FIBER OPTIC CONNECTORS USING SAME
    41.
    发明申请
    RECEPTACLE FERRULE ASSEMBLIES WITH GRADIENT INDEX LENSES AND FIBER OPTIC CONNECTORS USING SAME 审中-公开
    带梯级索引镜片和光纤连接器的接收器芯片组合

    公开(公告)号:WO2012099769A3

    公开(公告)日:2012-11-22

    申请号:PCT/US2012021036

    申请日:2012-01-12

    Abstract: A receptacle ferrule assembly for a fiber optic receptacle connector. The receptacle ferrule assembly comprises a first lens (155) with first second optical surfaces and a receptacle ferrule body having first and second ends. At least one monolithic optical system is formed in a monolithic receptacle ferrule body and includes a lens (420) formed at the second end of monolithic receptacle ferrule body and an optical surface formed at the first end of monolithic receptacle ferrule body. The optical surface is situated adjacent to, and mated to the second optical surface (155S2) of the first lens The monolithic optical system is configured, in conjunction with the first lens, to define a receptacle optical pathway from the second end of the monolithic optical system to the first surface of the first lens. According to some embodiments the first lens is a gradient index lens.

    Abstract translation: 一种用于光纤插座连接器的插座套圈组件。 插座套圈组件包括具有第一第二光学表面的第一透镜(155)和具有第一和第二端的插座套圈本体。 至少一个整体式光学系统形成在单片插座套圈本体中,并且包括形成在单片插座套圈本体的第二端处的透镜(420)和形成在单片插座套圈本体的第一端处的光学表面。 光学表面位于与第一透镜的第二光学表面(155S2)相邻并配合的位置。单片光学系统与第一透镜一起被配置为从单片光学器件的第二端限定一个插座光路 系统到第一透镜的第一表面。 根据一些实施例,第一透镜是梯度折射率透镜。

    ENERGY TRANSFER IN SCANNING LASER PROJECTORS
    42.
    发明申请
    ENERGY TRANSFER IN SCANNING LASER PROJECTORS 审中-公开
    扫描激光投影仪中的能量传输

    公开(公告)号:WO2012030749A2

    公开(公告)日:2012-03-08

    申请号:PCT/US2011049623

    申请日:2011-08-30

    Inventor: GOLLIER JACQUES

    CPC classification number: H04N9/3188 H04N9/3129

    Abstract: The present disclosure introduces a number of image compression schemes designed to optimize operational efficiency in laser scanning projectors. Contemplated compression modes include, but are not limited to, intra-frame energy transfer, inter-frame energy transfer, and combinations thereof. The image compression modes disclosed herein are equally applicable to native laser sources and synthetic sources, such as green lasers based on a non-linear wavelength conversion. In cases where multiple lasers are used together in a multi-color projection system, it will often be preferable to favor particular image compression modes for particular colors, particularly where image brightness is more readily attributable to one color, e.g., green, because of the spectral responsivity of the human eye.

    Abstract translation: 本公开引入了许多设计用于优化激光扫描投影仪中的操作效率的图像压缩方案。 考虑的压缩模式包括但不限于帧内能量传输,帧间能量传输及其组合。 这里公开的图像压缩模式同样适用于本地激光源和合成源,例如基于非线性波长转换的绿色激光。 在多色投影系统中一起使用多个激光器的情况下,对于特定颜色,特别是在图像亮度更容易归因于一种颜色(例如绿色)的情况下,通常会优选特定图像压缩模式,因为 人眼的光谱响应度。

    CORRECTION OF POWER VARIATIONS IN LASER SOURCES
    43.
    发明申请
    CORRECTION OF POWER VARIATIONS IN LASER SOURCES 审中-公开
    激光源功率变化的修正

    公开(公告)号:WO2010048353A3

    公开(公告)日:2010-07-29

    申请号:PCT/US2009061571

    申请日:2009-10-22

    CPC classification number: H01S5/06832 H01S5/0092 H01S5/06256 H04N9/3129

    Abstract: The present invention relates generally to semiconductor lasers and laser projection systems. According to one embodiment of the present invention, a method of correcting output power variations in a semiconductor laser is provided. According to the method, an output power feedback loop is utilized to generate optical intensity feedback signals representing actual output power of the laser source for discrete portions V1, Vi, Vj of the image signal. Error signals E1, Ei, Ej are generated representing the degree to which actual projected output power varies from a target projected output power for the discrete portions V1, Vi, Vj of the image signal. These error signals E1, Ei, Ej are utilized to apply corrected control signals G1', Gi', Gj' to the gain section of the semiconductor laser for projection of compatible discrete portions V1', Vi', Vj' of the image signal. According to another embodiment of the present invention, a system is provided for generating a projected laser image.

    Abstract translation: 本发明一般涉及半导体激光器和激光投影系统。 根据本发明的一个实施例,提供了一种校正半导体激光器中的输出功率变化的方法。 根据该方法,利用输出功率反馈回路产生代表图像信号的离散部分V1,Vi,Vj的激光源的实际输出功率的光强度反馈信号。 产生表示实际投影输出功率相对于图像信号的离散部分V1,Vi,Vj的目标投影输出功率变化程度的误差信号E1,Ei,Ej。 利用这些误差信号E1,Ei,Ej将校正的控制信号G1',Gi',Gj'施加到半导体激光器的增益部分,用于投影图像信号的兼容离散部分V1',Vi',Vj'。 根据本发明的另一个实施例,提供了一种用于产生投影激光图像的系统。

    WAVELENGTH CONVERSION DEVICE AND LASER PROJECTION SYSTEM INCORPORATING THE SAME
    44.
    发明申请
    WAVELENGTH CONVERSION DEVICE AND LASER PROJECTION SYSTEM INCORPORATING THE SAME 审中-公开
    波长转换装置和激光投射系统

    公开(公告)号:WO2010024912A3

    公开(公告)日:2010-04-15

    申请号:PCT/US2009004886

    申请日:2009-08-27

    CPC classification number: G02F1/377 G02F1/3775 H01S3/0092 H04N9/3129

    Abstract: The present invention relates generally to a wavelength conversion device (10) and a laser projection system (100) incorporating the same. According to one embodiment of the present invention, the wavelength conversion device is provided to a laser projection system (100). The wavelength conversion device (10) comprises an axial waveguide portion (12A) and a pair of lateral planar waveguide portions (12B) confined between a pair of relatively low index cladding layers (14). The effective index of refraction in the axial waveguide portion (12A) of the waveguide region and the effective index of refraction in the lateral planar waveguide portions (12B) of the waveguide region (12) are established such that the relatively low intensity laterally distributed parasitic light (17) is associated with a scattering angle ? that is at least as large as the beam divergence angle of the relatively high intensity light (15) propagating in the axial waveguide portion (12A).

    Abstract translation: 本发明一般涉及一种波长转换装置(10)和包含该波长转换装置的激光投射系统(100)。 根据本发明的一个实施例,波长转换装置被提供给激光投射系统(100)。 波长转换装置(10)包括轴向波导部分(12A)和限定在一对相对较低折射率的包层(14)之间的一对横向平面波导部分(12B)。 波导区域的轴向波导部分(12A)中的有效折射率和波导区域(12)的横向平面波导部分(12B)中的有效折射率建立为使得相对低强度的横向分布的寄生 光(17)与散射角α 其至少与在轴向波导部分(12A)中传播的相对高强度的光(15)的光束发散角一样大。

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