Decoherence recovery method of coseismic deformation field:Taking the 2009 L′Aquila MW6.3 earthquake as an example
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摘要: 在合成孔径雷达干涉测量中,干涉相干是局部干涉条纹质量的重要评价标准,但是由于各种失相干源的影响,会出现失相干现象,而这可能会丢失重要的形变数据。本文首先利用ENVISAT ASAR的两景影像获得了2009年意大利拉奎拉MW6.3地震的带有失相干现象的同震形变场,对数据预处理后再使用移动窗口克里金法对拉奎拉地震的同震形变场进行插值处理,恢复了形变图的失相干区域,之后进一步通过正反演获得同震形变场,并与上一步的插值结果进行对比分析。结果显示,插值结果与反演结果在极震区吻合得很好,验证了移动窗口克里金插值法恢复失相干的可靠性,说明插值法可以成为实现地震同震形变场失相干恢复的一种途径。
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关键词:
- InSAR技术 /
- 2009年拉奎拉MW6.3地震 /
- 移动窗口克里金法 /
- 正反演 /
- 失相干恢复
Abstract: In SAR interferometry, interference coherence is an important evaluation criterion for the quality of local interference fringes. However, due to the influence of various sources of decoherence, decoherent phenomena appear, which may lose important deformation data. In this paper, we first obtain the coseismic deformation field of the 2009 L′Aquila MW6.3 earthquake with the two scenes of ENVISAT ASAR. After preprocessing the data, we interpolate the coseismic deformation field of the L′Aquila earthquake using the moving window Kriging method, with a result that the decoherence area of the deformation map is restored, and then the co-seismic deformation field obtained by the forward and inversion is used to compare and analyze the interpolation results with the previous step. The results show that the interpolation results are in good agreement with the inversion results in the meizoseismal area, which verifies the reliability of the moving window Kriging interpolation method to restore the decoherence, and shows that the interpolation method can be used to realize the decoherence recovery of the coseismic deformation field. Therefore, it has important reference significance for the research on the recovery of remote sensing image data with decoherence phenomenon. -
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表 1 ENVI ASAR雷达数据参数列表
Table 1 Data parameters of ENVI ASAR radar
轨道 升降轨模式 接收日期 时间基线/d 空间垂基线/m T079 降轨 2008-04-27
2009-04-12350 40.401 表 2 拉奎拉地震断层模型几何参数列表
Table 2 List of geometric parameters of L′Aquila seismic fault model
采样点个数 断层参数 MW 误差/cm 东经/(°) 北纬/(°) 走向/° 倾角/° 断层长度/km 顶深/km 底深/km 滑动角/° 2 919 13.470 42.367 141.8° 55° 13.2 2.9 12.6 −118.7 6.3 1.2 -
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