IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING, VOL. 56, NO. 1, JANUARY 2018 49
A Wavelet Decomposition and Polynomial
Fitting-Based Method for the Estimation
of Time-Varying Residual Motion Error
in Airborne Interferometric SAR
Hai Qiang Fu, Jian Jun Zhu, Chang Cheng Wang, Member, IEEE, Hui Qiang Wang, and Rong Zhao
Abstract— Compensating the residual motion error (RME)
is very important in airborne interferometric synthetic aper-
ture radar (InSAR). In this paper, the wavelet decomposition
and polynomial fitting-based (WDPF) method is proposed for
detecting and correcting the RME. Wavelet decomposition with
root-mean-square error (RMSE) change ratio-based decompo-
sition scale identification is used to detect the RME from the
differential interferogram. Polynomial fitting in combination
with robust estimation-based least squares is used to absorb
the incidence-angle-dependent and topography-dependent com-
ponents of the RME. A simulated experiment was conducted to
test the proposed WDPF method. High-precision RME (with an
RMSE of 0.0375 rad) was obtained, which can meet the require-
ments of InSAR. Real-data L- and P-band InSAR experiments
were also performed to test the WDPF method. The results
confirmed that the WDPF method can effectively correct the
RME for the interferogram. The RMSE of the estimated digital
elevation model (DEM) was reduced from 8.03 to 3.46 m and
8.18 to 3.10 m for the L- and P-band interferograms, respectively.
Finally, the effects of the external DEM error and polarization
on the RME calibration were investigated. The results indicated
that the global InSAR DEM products can fulfill the requirement
of differential interferogram generation for the WDPF method,
and the multipolarization interferograms can help to reduce the
effect of the topographic error phase on RME estimation.
Index Terms— Interferometric synthetic aperture radar
(InSAR), motion compensation (MoCo), repeat pass, residual
motion error (RME).
I. I NTRODUCTION
A
IRBORNE interferometric synthetic aperture radar
(InSAR) systems have been shown to be a powerful
tool for the monitoring of forests [1], [2], agriculture [3], [4],
and geological hazards [5], [6]. In order to build a rigorous
Manuscript received March 14, 2017; revised June 15, 2017; accepted
July 9, 2017. Date of publication November 8, 2017; date of current version
December 27, 2017. This work was supported in part by the National Natural
Science Foundation of China under Grant 41531068, Grant 41671356, and
Grant 41371335, in part by the Hunan Provincial Innovation Foundation for
Postgraduate under Grant 150140004, and in part by the PA-SB ESA EO
Project Campaign. (Corresponding author: Jian Jun Zhu.)
The authors are with the School of Geosciences and Info-Physics, Central
South University, Changsha 410083, China (e-mail: haiqiangfu@csu.edu.cn;
zjj@csu.edu.cn; wangchangcheng@csu.edu.cn; wanghuiqiang@csu.edu.cn;
zhaorong1018@126.com).
Color versions of one or more of the figures in this paper are available
online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TGRS.2017.2727076
geometrical relationship between the interferometric phase
and ground target position, it is important to exactly record
platform motion by the SAR sensor’s navigation system so
that motion compensation (MoCo) [7]–[9] can later be per-
formed during the SAR imaging process. However, any MoCo
approach is restricted by the positioning quality of the SAR
sensor’s navigation system. As a result, the residual motion
error (RME) induces misregistration and undesirable phase
artifacts in the interferogram. For a single-pass interferometry,
most of the RME can be canceled out since the two interfer-
ometric images will have similar RMEs.
However, the MoCo cannot meet the requirement of the
positioning quality in repeat-pass interferometry. The reason
for this is that it is difficult for the navigation system to exactly
capture atmospheric turbulence motion, and the RMEs of
each flight track are independent. Even when a high-precision
navigation system is employed, the RME can still cause
significant interferometric phase errors. As a result, the RME
prohibits the extraction of accurate interferometric information
from InSAR or differential InSAR (D-InSAR) data.
In order to reduce the effect of the RMEs on the interfer-
ograms, some efforts have been made to detect the RME and
remove them from SAR and InSAR data by postprocessing
steps, which differ from each other based on how the RMEs
are estimated and modeled. The first kind of method is based
on the multisquint processing technique [10]–[12], whose main
principle is that the RMEs differ in different subapertures.
This kind of method has widely been adopted in airborne
D-InSAR applications [13], but its capacity is limited by low
coherence, terrain displacement, and different phase centers
of the sublook interferograms [14], [15]. The second kind
of method, such as the weighted phase curvature autofo-
cus (WPCA) method [16], is free from the limitation of any
interferometric process or assumption on the interferometric
phase, but it needs targets with high signal-to-noise ratio. The
last kind of method based on detecting stable point-like targets
is suitable for multibaseline InSAR data stacks [17]–[20].
However, sufficient SAR or polarimetric SAR data are needed
to secure satisfactory results.
As an alternative, in this paper, we propose a simpler way
to correct the RMEs for the coregistered SAR images by the
wavelet decomposition and polynomial fitting-based (WDPF)
method. The main principle of this method is that along the
range direction, the errors of the baseline parameters are scaled
by incidence angles and ground elevations, which present
definite trend and allow to be parameterized. This approach
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