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    • 2. 发明申请
    • OPTICAL PROXIMITY FUZE
    • 光临近度燃料
    • WO2010015860A1
    • 2010-02-11
    • PCT/GB2009/050985
    • 2009-08-06
    • MBDA UK LIMITEDJENNINGS, Martyn, RobertMILLER, Lee, Douglas
    • JENNINGS, Martyn, RobertMILLER, Lee, Douglas
    • F42C13/02G01S7/481G01S17/02
    • G01S7/4818F42C13/02G01S17/026G01S17/87G01S17/89
    • Described herein is an optical fuze for a guided missile that comprisesan array of a large number of optical apertures distributed about the outer surface of the missile. An optical waveguide network selectively couplesthe array of apertures to a laser source and to a photodetectorsuch that light from the laser source is emitted by selected ones of said apertures, and light returned from a target is received by selected ones of said apertures and directed by said optical waveguide network to said photodetector. These apertures might be arranged to form a compositetarget images in a particular direction, and/or may be arranged to perform a sensing operation along selected directions. The optical proximity fuze described herein provides inherent flexibility in the way the fuze can be configured in the missilefor optimisationfor different applications.
    • 这里描述的是用于导弹的光引信,其包括围绕导弹的外表面分布的大量光学孔的阵列。 光波导网络选择性地将孔阵列耦合到激光源和光电检测器,来自激光源的光由选定的所述孔发射,并且从目标返回的光由选定的所述孔接收并由所述 光波导网络连接到所述光电检测器。 这些孔可以被布置成在特定方向上形成复合目标图像,和/或可被布置成沿着选定的方向执行感测操作。 这里描述的光学邻近引信提供了在导弹中可以配置引信的方式的固有的灵活性,以针对不同的应用进行优化。
    • 3. 发明申请
    • TARGET SCENE GENERATOR
    • 目标场景发生器
    • WO2010058194A1
    • 2010-05-27
    • PCT/GB2009/051501
    • 2009-11-10
    • MBDA UK LIMITEDJENNINGS, Martyn, RobertMILLER, Lee, Douglas
    • JENNINGS, Martyn, RobertMILLER, Lee, Douglas
    • G01S7/497F41G7/00
    • F41G7/002G01S7/497G01S17/74
    • A target scene generator for testing an imaging ladar in a Hard Ware in the Loop arrangement, such as might be employed for testing an optical seeker on a guided missile, the generator comprising an array of pixel elements (10), a photodetector (20) for detecting incident light from a ladar a laser source (18) for generating pulses of light representing returned ladar pulses, and a reconfigurable fibre network (14) including an optical switch selectively coupling the laser (18) to the pixel elements, and a controller (22) which selectively reconfigures the fibre network, to present to selected pixel elements the pulses of light with selected time delay characteristics such that light emitted from the pixels represent light returned from a target illuminated by the ladar.
    • 一种目标场景发生器,用于测试环路装置中Hard Ware中的成像装置,例如可用于在导弹上测试光学探测器,所述发生器包括像素元件阵列(10),光电检测器(20) 用于检测来自激光源(18)的入射光,用于产生表示返回的脉冲的脉冲的光;以及可重构光纤网络(14),包括选择性地将激光器(18)耦合到像素元件的光开关,以及控制器 (22),其选择性地重新配置光纤网络,向所选择的像素元件呈现具有所选择的时间延迟特性的光脉冲,使得从像素发射的光表示从由灯塔照射的目标返回的光。
    • 5. 发明申请
    • LASER
    • 激光
    • WO2007012902A1
    • 2007-02-01
    • PCT/GB2006/050225
    • 2006-07-27
    • MBDA UK LimitedJENNINGS, Martyn, RobertMILLER, Lee, Douglas
    • JENNINGS, Martyn, RobertMILLER, Lee, Douglas
    • H01S3/094H01S3/06H01S3/11H01S3/16H01S3/07
    • H01S3/094H01S3/0606H01S3/07H01S3/094026H01S3/094053H01S3/094061H01S3/094084H01S3/1103
    • A laser device and a method of pumping a laser gain medium (R) comprise directing pulses of laser light from a pump laser (10) to a series of separate locations (11 , 12, 13, 14, 15, 16 and 17) arranged longitudinally along the gain medium (R) in the direction of laser propagation. Each pulse of laser light generates a population inversion in an associated portion of the gain medium (R) just ahead of the laser photons. The pulses from the pump laser (10) are transmitted by a splitter (18) to the series of separate locations by optical delay lines (11 , 12, 13, 14, 15, 16 and 17) and each delay line is arranged to pump a different portion of the gain medium to cause a localised population inversion. The pulse transmission delays deliver a sequence of pulses to the portions of the gain medium (R) such that each portion will in turn contribute to amplification of a laser propagating within the gain medium (R).
    • 一种激光装置和一种泵浦激光增益介质(R)的方法包括将来自泵激光器(10)的激光脉冲引导到一系列分开的位置(11,12,13,14,15,16和17) 沿着增益介质(R)在激光传播方向上纵向延伸。 激光的每个脉冲在激光光子之前的增益介质(R)的相关部分中产生总体反转。 来自泵激光器(10)的脉冲通过光学延迟线(11,12,13,14,15,16和17)由分离器(18)传输到一系列分离的位置,并且每个延迟线被布置成泵送 增益介质的不同部分导致局部群体反转。 脉冲传输延迟将一系列脉冲提供给增益介质(R)的部分,使得每个部分又将有助于在增益介质(R)内传播的激光器的放大。