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An efficient method for measuring the internal parameters of optical cameras based on optical fibres

机译:基于光纤的光学相机内部参数的有效测量方法

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摘要

In this work, we report an expedient auto-collimating method for self-measuring the internal parameters (IPs) of optical cameras. Several key optical components, including the thin optical fibre (TOF), reflecting prism, and receiver, are introduced into optical cameras. The TOF outgoing end and area-array image receiver are integrated onto the focal-plane assembly of optical cameras. Different wavelengths of light, which are emitted by external sources, are transmitted to the focal plane through optical fibres. Because one optical fibre can transmit different wavelengths of light, the same position on the focal plane can obtain point light sources (PLSs) with different wavelengths. Then, the optical system of the cameras spontaneously transforms the PLSs into auto-collimating lights. The auto-collimating lights are reflected by a two-plane prism, return to the camera optical system, reach the focal plane and are received by the area-array sensor. Finally, the IPs are calculated based on a mathematical model of the imaging relation between fibre light sources and images. The experiment confirms that this method is efficient and has a level of precision of dozens of micrometres for an optical camera with a short focal length and small field of view. Our method is suitable for on-orbit IP measurements for cameras without spatial or temporal limitations.
机译:在这项工作中,我们报告了一种用于自我测量光学相机内部参数(IP)的便捷自动准直方法。光学相机中引入了几个关键的光学组件,包括细光纤(TOF),反射棱镜和接收器。 TOF输出端和区域阵列图像接收器集成到光学相机的焦平面组件上。外部光源发出的不同波长的光通过光纤传输到焦平面。由于一根光纤可以传输不同波长的光,因此焦平面上的相同位置可以获得具有不同波长的点光源(PLS)。然后,摄像机的光学系统自发地将PLS转换为自动准直光。自动准直光被两平面棱镜反射,返回到相机光学系统,到达焦平面,并由区域阵列传感器接收。最后,基于光纤光源和图像之间的成像关系的数学模型来计算IP。实验证实,对于焦距短,视野小的光学相机,该方法有效且具有数十微米的精度。我们的方法适用于无空间或时间限制的摄像机在轨IP测量。

著录项

  • 期刊名称 Scientific Reports
  • 作者

    Jin Li; Shou-Fu Tian;

  • 作者单位
  • 年(卷),期 -1(7),-1
  • 年度 -1
  • 页码 12479
  • 总页数 9
  • 原文格式 PDF
  • 正文语种
  • 中图分类
  • 关键词

  • 入库时间 2022-08-21 10:56:11

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