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arXiv 0705.3379physics.opticsphysics.ins-det
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radio telescope孔径效率的光线追迹和物理光学分析

Ray-tracing and physical-optics analysis of the aperture efficiency in a radio telescope

Luca Olmi, Pietro Bolli

摘要:

在微波或可见/IR波长下工作的望远镜系统的性能通常根据波长范围用不同的参数来描述。大多数商业射线跟踪软件包都是专门为可见光/红外系统设计的,因此,尽管非常灵活和复杂,但不能提供适当的参数来充分描述微波天线,从而无法与规格进行比较。在这项工作中,我们证明了斯特列尔比等于相位效率时,切趾因子被考虑在内。相位效率是影响天线口径效率的最关键因素,也是望远镜设计中最难优化的参数。斯特列尔比和相位效率之间的等效性使望远镜的设计者/用户有机会使用更快的商业射线跟踪软件来优化设计。我们还讨论了几个测试的结果,以检查这种关系的有效性,我们进行了使用射线跟踪软件,ZEMAX和一个完整的物理光学软件,GRASP9.3,适用于三个不同的望远镜设计,跨越一个因素的$\simeq 10 in terms of D/lambda. The maximum measured discrepancy between phase efficiency and Strehl ratio varies between $ \simeq 0.4和1.9高达一个偏移角>40束,这取决于光学配置,但在斯特列尔比>0.95的情况下,它总是小于0.5。

英文摘要:

The performance of telescope systems working at microwave or visible/IR wavelengths is typically described in terms of different parameters according to the wavelength range. Most commercial ray tracing packages have been specifically designed for use with visible/IR systems and thus, though very flexible and sophisticated, do not provide the appropriate parameters to fully describe microwave antennas, and thus to compare with specifications. In this work we demonstrate that the Strehl ratio is equal to the phase efficiency when the apodization factor is taken into account. The phase efficiency is the most critical contribution to the aperture efficiency of an antenna, and the most difficult parameter to optimize during the telescope design. The equivalence between the Strehl ratio and the phase efficiency gives the designer/user of the telescope the opportunity to use the faster commercial ray-tracing software to optimize the design. We also discuss the results of several tests performed to check the validity of this relationship that we carried out using a ray-tracing software, ZEMAX and a full Physical Optics software, GRASP9.3, applied to three different telescope designs that span a factor of $\simeq 10 in terms of D/lambda. The maximum measured discrepancy between phase efficiency and Strehl ratio varies between $\simeq 0.4 and 1.9 up to an offset angle of >40 beams, depending on the optical configuration, but it is always less than 0.5 where the Strehl ratio is >0.95.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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