Radar interferometric imaging using the maximum entropy method for the case of point targets

Qian Zhu, J. Mathews
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Abstract

Summary form only given. The radar interferometry technique was first used at the Jicamarca Radio Observatory by Woodman (1971) for measuring the inclination of geomagnetic field. Since then, this technique has been successfully developed for imaging ionospheric plasma irregularities phenomena (Farley 1981; Kudeki 1987; Hysell 1996; etc.). With this technique, we can obtain the spatial and temporal (image) information of objects at the same time. We explore practical methods to achieve both fine spatial and temporary resolutions for radar imaging of meteor (point target) events. The basic mathematical description of radar interferometric imaging is the linear Fourier transform relationship (Woodman 1997). The complex visibility measurement from one interferometer baseline is a Fourier component of the objects brightness distribution. However, since the observed visibility data (the Fourier coefficients) from radar interfereometry is necessarily incomplete and noisy, in most cases the directly linear inversion is not sufficient to obtain the desired resolution of objects. We need non-linear inversion techniques to remove “ringing” effects and obtain details that are not revealed using linear inversion techniques. Among the non-linear inversion techniques, the maximum entropy method has been widely used in many fields (e.g., radio astronomy, etc.) to reconstruct images of objects. According to the comparisons between maximum entropy method and other conventional inversion methods (CLEAN, etc.) from many papers, we believe maximum entropy method is an optimal choice to achieve satisfactory reconstructions from incomplete and noisy data. Therefore, for meteor head-echoes modeling purposes, a discrete linear radar interferometric signal model is derived, and a maximum entropy image reconstruction method based on Newton-Raphson technique is applied to point targets. Its advantages and limitations are discussed.
点目标情况下的最大熵法雷达干涉成像
只提供摘要形式。雷达干涉测量技术是伍德曼(1971)在Jicamarca射电天文台首次用于测量地磁场倾角。从那时起,这项技术已经成功地用于成像电离层等离子体不规则现象(Farley 1981;Kudeki 1987;Hysell 1996;等等)。利用该技术,我们可以同时获得物体的时空(图像)信息。我们探索实现流星(点目标)事件雷达成像的精细空间和临时分辨率的实用方法。雷达干涉成像的基本数学描述是线性傅立叶变换关系(Woodman 1997)。一个干涉仪基线的复杂能见度测量是物体亮度分布的傅里叶分量。然而,由于雷达干涉测量观测到的能见度数据(傅里叶系数)必然是不完整和有噪声的,在大多数情况下,直接线性反演不足以获得期望的目标分辨率。我们需要非线性反演技术来消除“振铃”效应,并获得使用线性反演技术无法揭示的细节。在非线性反演技术中,最大熵法已被广泛应用于许多领域(如射电天文学等)来重建物体图像。根据许多文献对最大熵法与其他常规反演方法(CLEAN等)的比较,我们认为最大熵法是在不完整和有噪声数据中获得满意重建结果的最佳选择。为此,针对流星头回波建模的目的,推导了离散线性雷达干涉信号模型,并将基于牛顿-拉夫森技术的最大熵图像重构方法应用于点目标。讨论了它的优点和局限性。
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