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optical device, serskilt for anvendning in treffsimulatorer for weapons

机译:光学装置,塞斯基尔特(Serskilt),用于在武器仿真器中进行伪装

摘要

In order to provide a laser beam having a relatively constant width (i.e. transverse spacing between points receiving a theshold irradiance), a converging lens 15 having substantial negative spherical aberration is used. In the far field, the beam comprises paraxial rays 18 which have diverged to provide the desired beam-width. In the near-field, the smaller, higher-irradiance beam formed by these rays is augmented by a 'sheath' of marginal rays 19 which are not refracted towards the optical axis as strongly as the paraxial rays. The shape of the beam in the far field is determined primarily by the shape of the (laser) light source 10, while that of the near-field beam is controlled by a mask 14. In another arrangement, a lens 102 having substantial positive spherical aberration is used to create a 'light source' having an accurately-controlled brightness distribution and very small size. Paraxial rays 109 are brought to a focus at a plane 108 defining the 'position' of the 'light source', while the more strongly refracted marginal rays 110 cross the optical axis before reaching this plane, thus creating a halo round the bright central beam produced by the paraxial rays. The brightness distribution at the plane is controlled by adjusting the spherical aberration of the lens, and by masking.
机译:为了提供具有相对恒定的宽度(即,接收阈值辐照度的点之间的横向间隔)的激光束,使用具有基本负的球面像差的会聚透镜15。在远场中,光束包括近轴光线18,其已发散以提供所需的光束宽度。在近场中,由这些射线形成的较小的,较高辐射的光束被边缘射线19的“鞘”所增强,该边缘射线没有像近轴射线那样强烈地向光轴折射。远场光束的形状主要由(激光)光源10的形状确定,而近场光束的形状由掩模14控制。在另一种布置中,具有基本为正球面的透镜102像差用于创建具有精确控制的亮度分布且尺寸非常小的“光源”。近轴光线109在定义“光源”的“位置”的平面108上聚焦,而折射更强的边缘光线110在到达该平面之前穿过光轴,从而在明亮的中心光束周围产生光晕由近轴射线产生。通过调整透镜的球差和遮罩,可以控制平面上的亮度分布。

著录项

  • 公开/公告号SE7903164L

    专利类型

  • 公开/公告日1979-10-12

    原文格式PDF

  • 申请/专利权人 SOLARTRON ELECTRONIC GROUP;

    申请/专利号SE19790003164

  • 发明设计人 MARCH A A C;

    申请日1979-04-10

  • 分类号G02B27/00;

  • 国家 SE

  • 入库时间 2022-08-22 20:27:13

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