Residual motion estimation for UAVSAR: Implications of an electronically scanned array

S. Hensley, T. Michel, M. Simard, Cathleen E. Jones, R. Muellerschoen, C. Le, H. Zebker, B. Chapman
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引用次数: 24

Abstract

The UAVSAR instrument, employing an L-band actively electronically scanned antenna, had its genesis in the ESTO Instrument Incubator Program and after 3 years of development has begun collecting engineering and science data. System design was motivated by solid Earth applications where repeat pass radar interferometry can be used to measure subtle deformation of the surface, however flexibility and extensibility to support other applications were also major design drivers. In order to make geophysically useful repeat pass interferometric measurements it is necessary to reconstruct the repeat pass baseline with millimeter accuracy, however onboard motion metrology systems only achieve 5–15 cm accuracy. Thus it is necessary to recover the residual motion from the data itself. Algorithms for recovering the motion based on along-track offsets between the repeat pass interferometric pair of images were described in [3], [1] and [4]. Later these techniques were extended to use azimuth subbanded differential interferograms in [5]. This paper provides a derivation for the formula for the along-track offsets (or corresponding the subbanded differential phase), i.e. the relative displacement between two SAR images in a interferometric pair in the along track direction, as a function of baseline for systems employing an electronically scanned antenna. The standard formula for systems not employing electronically scanned antenna for the along-track offsets, Δs, has the form in given equation where bc is the cross-track baseline, bh is the vertical baseline, θℓ is the look angle, θaz is the azimuth or squint angle, ρ is the range and d = 1 for left looking systems and d = −1 for right looking systems. A key feature of this formula is the along-track offsets only range dependency is from the derivatives of the baseline with respect to along-track position. In the electronically scanned case this in no longer true and an additional range dependency arises that is a function of the electronic steering angle.
UAVSAR的剩余运动估计:电子扫描阵列的含义
UAVSAR仪器采用l波段主动电子扫描天线,起源于ESTO仪器孵化器计划,经过3年的发展,已经开始收集工程和科学数据。系统设计的动机是固体地球应用,其中重复通过雷达干涉测量可用于测量表面的细微变形,但支持其他应用的灵活性和可扩展性也是主要的设计驱动因素。为了使重复通道干涉测量在地球物理上有用,有必要以毫米精度重建重复通道基线,然而机载运动测量系统只能达到5-15厘米的精度。因此,有必要从数据本身恢复残余运动。基于重复通道干涉图像对之间的沿轨迹偏移量恢复运动的算法在[3]、[1]和[4]中有描述。后来,这些技术在[5]中扩展到使用方位角子带差分干涉图。本文提供了沿航迹偏移(或对应的子带差分相位)公式的推导,即沿航迹方向干涉对中两个SAR图像之间的相对位移,作为采用电子扫描天线的系统的基线函数。不使用电子扫描天线的系统的标准公式,Δs,具有给定方程的形式,其中bc是交叉轨迹基线,bh是垂直基线,θ r是观察角度,θ z是方位角或斜视角,ρ是距离,d = 1左望系统,d = - 1右望系统。该公式的一个关键特征是沿航迹偏移量,距离依赖于基线相对于沿航迹位置的导数。在电子扫描的情况下,这不再是真的,并且出现了额外的范围依赖,这是电子转向角的函数。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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