[go: up one dir, main page]

CN111239736A - Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline - Google Patents

Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline Download PDF

Info

Publication number
CN111239736A
CN111239736A CN202010195430.9A CN202010195430A CN111239736A CN 111239736 A CN111239736 A CN 111239736A CN 202010195430 A CN202010195430 A CN 202010195430A CN 111239736 A CN111239736 A CN 111239736A
Authority
CN
China
Prior art keywords
sub
phase
aperture
full
view
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN202010195430.9A
Other languages
Chinese (zh)
Other versions
CN111239736B (en
Inventor
付海强
刘志卫
朱建军
赵蓉
王会强
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Central South University
Original Assignee
Central South University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Central South University filed Critical Central South University
Priority to CN202010195430.9A priority Critical patent/CN111239736B/en
Publication of CN111239736A publication Critical patent/CN111239736A/en
Application granted granted Critical
Publication of CN111239736B publication Critical patent/CN111239736B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/89Radar or analogous systems specially adapted for specific applications for mapping or imaging
    • G01S13/90Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
    • G01S13/9021SAR image post-processing techniques
    • G01S13/9023SAR image post-processing techniques combined with interferometric techniques
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/882Radar or analogous systems specially adapted for specific applications for altimeters
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/885Radar or analogous systems specially adapted for specific applications for ground probing
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/89Radar or analogous systems specially adapted for specific applications for mapping or imaging
    • G01S13/90Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
    • G01S13/9004SAR image acquisition techniques
    • G01S13/9011SAR image acquisition techniques with frequency domain processing of the SAR signals in azimuth
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/40Means for monitoring or calibrating

Landscapes

  • Engineering & Computer Science (AREA)
  • Remote Sensing (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • General Physics & Mathematics (AREA)
  • Signal Processing (AREA)
  • Radar Systems Or Details Thereof (AREA)

Abstract

The invention discloses a single-baseline-based surface elevation correction method, a single-baseline-based surface elevation correction device, single-baseline-based surface elevation correction equipment and a single-baseline-based storage medium, wherein the method comprises the following steps: acquiring two full-aperture images of a research area, and acquiring each full-aperture image by adopting a sub-aperture decomposition technology to decompose the full-aperture image into two sub-view images; preprocessing the full-aperture image and the sub-view image to obtain a corresponding interference pattern; performing terrain removing processing on the two sub-view interferograms by using DEM data, and removing flat ground and orbit error phases to obtain two sub-view differential interferograms comprising the same troposphere delay error; performing correlation analysis on high-frequency wavelet coefficients of the two sub-view differential interferograms by adopting a wavelet decomposition technology, and extracting troposphere delay error phases; and removing the obtained troposphere delay error phase from the full-aperture interferogram, and calculating according to the satellite orbit parameters to obtain earth surface elevation data. The invention can extract the troposphere delay error phase only by using two full-aperture images and obtain high-precision earth surface elevation data.

Description

基于单基线的地表高程校正方法、装置、设备及存储介质Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline

技术领域technical field

本发明涉及合成孔径雷达干涉测量(InSAR)技术在大范围地形测量中的应用,属于星载合成孔径雷达提取地表高程技术领域,具体是指一种基于单基线的地表高程校正方法、装置、设备及存储介质。The invention relates to the application of synthetic aperture radar interferometry (InSAR) technology in large-scale terrain measurement, belongs to the technical field of surface elevation extraction by spaceborne synthetic aperture radar, and particularly relates to a single baseline-based surface elevation correction method, device and equipment and storage media.

背景技术Background technique

数字高程模型(digital elevation model,DEM)是国家经济建设、社会发展和国家安全必不可少的基础图件,是基础设施规划、设计和施工及资源调查、开发所必须的基础资料。合成孔径雷达(InSAR)技术,具备全天候、全天时、观测周期短、大范围的优势,成为了一种获取全球DEM的强有力工具。然而,在进行InSAR对地观测时,雷达信号会受到多种因素的影响,这也误差严重影响了采用InSAR技术进行地形测量的精度。对于目前常用的重轨星载SAR系统而言,对流层延迟误差是影响其测高精度最主要的误差源之一。因此,为了获取大范围、高精度的InSAR数字高程模型,必须对干涉相位中包含的对流层延迟误差进行有效的估计和去除。Digital elevation model (DEM) is an indispensable basic drawing for national economic construction, social development and national security. Synthetic Aperture Radar (InSAR) technology has the advantages of all-weather, all-day, short observation period and wide range, and has become a powerful tool for obtaining global DEM. However, during the InSAR earth observation, the radar signal will be affected by many factors, which also seriously affects the accuracy of the terrain measurement using InSAR technology. For the currently commonly used heavy-orbit spaceborne SAR systems, the tropospheric delay error is one of the most important error sources affecting the measurement accuracy. Therefore, in order to obtain a large-scale and high-precision InSAR digital elevation model, it is necessary to effectively estimate and remove the tropospheric delay error contained in the interferometric phase.

目前,InSAR测量中常用的对流层延迟误差改正方法主要包括以下三类:1)相位-高程的相关性分析分析法;2)外部水汽数据辅助法;3)时序InSAR分析法。其中,第一类方法通常需要依赖于一定的先验信息,即对流层延迟误差相位与地面高度呈现一定的相关性,且该方法只能去除与地形相关的对流层延迟误差相位,当干涉图中与地形不相关的湍流误差占优时,该方法不能得到较好的改正结果;相较于第一类方法,第二类方法要求SAR数据与外部水汽数据之间具有较好的时空一致性,这就限制了该方法的推广使用;与前两类方法不同的是,为了使用第三类方法得到较好的改正结果,需要覆盖同一地区的大量SAR数据量。然而,在实际应用中,由于外部数据的缺乏或SAR数据量较少,上述方法很难取得较好的对流层延迟误差改正效果。At present, the tropospheric delay error correction methods commonly used in InSAR measurements mainly include the following three categories: 1) phase-elevation correlation analysis method; 2) external water vapor data-assisted method; 3) time-series InSAR analysis method. Among them, the first type of method usually needs to rely on certain prior information, that is, the tropospheric delay error phase has a certain correlation with the ground height, and this method can only remove the tropospheric delay error phase related to the terrain. When terrain-independent turbulence errors dominate, this method cannot obtain better correction results; compared with the first type of method, the second type of method requires better spatiotemporal consistency between SAR data and external water vapor data, which This limits the popularization of this method. Different from the first two types of methods, in order to use the third type of method to obtain better correction results, a large amount of SAR data covering the same area needs to be covered. However, in practical applications, due to the lack of external data or the small amount of SAR data, it is difficult for the above methods to achieve good tropospheric delay error correction.

因此,有必要设计一种无需依赖外部水汽辅助数据或过量SAR数据的对流层延迟误差校正方法。Therefore, it is necessary to design a tropospheric delay error correction method without relying on external water vapor assistance data or excess SAR data.

发明内容SUMMARY OF THE INVENTION

本发明所要解决的技术问题在于,提供一种基于单基线的地表高程校正方法、装置、设备及存储介质,通过提取对流层延迟误差相位以对地表相位进行校准,从而得到更高精度的地表高程数据。The technical problem to be solved by the present invention is to provide a single-baseline-based surface elevation correction method, device, equipment and storage medium, which can calibrate the surface phase by extracting the tropospheric delay error phase, thereby obtaining higher-precision surface elevation data .

为实现上述技术目的,本发明采用如下技术方案:For realizing the above-mentioned technical purpose, the present invention adopts following technical scheme:

一种基于单基线的地表高程校正方法,包括以下步骤:A method for surface elevation correction based on a single baseline, comprising the following steps:

步骤1,获取研究区域的两个全孔径SAR影像,采用子孔径分解技术将每个全孔径SAR影像分解为两个与方位向入射角对应的子视影像;Step 1: Acquire two full-aperture SAR images of the study area, and use sub-aperture decomposition technology to decompose each full-aperture SAR image into two sub-view images corresponding to azimuth incident angles;

步骤2,对两个全孔径SAR影像进行预处理得到全孔径干涉图;对同一方位向入射角的两个子视影像进行预处理,得到与方位向入射角对应的子视干涉图;Step 2, preprocessing two full-aperture SAR images to obtain a full-aperture interferogram; preprocessing two sub-view images with the same azimuth incident angle to obtain a sub-view interferogram corresponding to the azimuth incident angle;

步骤3,对两个子视干涉图,均使用DEM数据并采用差分干涉技术进行去地形处理,然后再去除平地相位和轨道误差相位处理,得到两个如以下公式所示的子视差分干涉图:Step 3: For the two sub-parallax interferograms, both use DEM data and use differential interferometry to perform topographic processing, and then remove the flat-ground phase and orbit error phase processing to obtain two sub-parallax differential interferograms as shown in the following formulas:

Figure BDA0002417446130000021
Figure BDA0002417446130000021

式中,α1和α2代表两个不同的方位向入射角,φdiff为子视差分干涉图中的差分干涉相位,△φtopo为地形误差相位,φatmo为对流层延迟误差相位,φnoise为随机噪声误差相位;where α 1 and α 2 represent two different azimuthal incident angles, φ diff is the differential interference phase in the subparallax interferogram, Δφ topo is the topographic error phase, φ atmo is the tropospheric delay error phase, and φ noise is the random noise error phase;

步骤4,对两个子视差分干涉图进行小波分解,对两个子视差分干涉图在每个分解尺度下的高频小波系数进行相关性分析,得到对应分解尺度下两个高频小波系数之间的相关值,根据相关值和任一高频小波系数计算得到对流层延迟误差相位相关的小波系数;然后对所述与对流层延迟误差相位相关的小波系数进行小波逆变换,即可得到对流层延迟误差相位;Step 4: Perform wavelet decomposition on the two sub-parallax differential interferograms, perform correlation analysis on the high-frequency wavelet coefficients of the two sub-parallax differential interferograms at each decomposition scale, and obtain the difference between the two high-frequency wavelet coefficients at the corresponding decomposition scale. The correlation value of , and the wavelet coefficient related to the tropospheric delay error phase is calculated according to the correlation value and any high-frequency wavelet coefficient; then the wavelet coefficient related to the tropospheric delay error phase is subjected to wavelet inverse transformation to obtain the tropospheric delay error phase. ;

步骤5,对全孔径干涉图进行解缠处理,将步骤4得到的对流层延迟误差相位从全孔径干涉图的解缠相位中去除;最后,根据卫星轨道参数以及去除对流层延迟误差相位的全孔径干涉图解缠相位,计算得到地表高程数据。In step 5, the full aperture interferogram is unwrapped, and the tropospheric delay error phase obtained in step 4 is removed from the unwrapped phase of the full aperture interferogram; finally, according to the satellite orbit parameters and the full aperture interferogram that removes the tropospheric delay error phase Unwrapped phase, calculated to obtain surface elevation data.

在更优的技术方案中,对两个子视干涉图,使用两种由不同技术获得的DEM数据进行去地形处理。In a better technical solution, the two sub-view interferograms are de-topographically processed using two DEM data obtained by different techniques.

在更优的技术方案中,对子视差分干涉图进行小波分解表示为:In a better technical solution, the wavelet decomposition of the sub-parallax interferogram is expressed as:

Figure BDA0002417446130000022
Figure BDA0002417446130000022

式中,m和n分别表示干涉图的行数和列数,x,y是像素点在雷达坐标系的坐标,ix和iy分别表示干涉图的第ix行和第iy列,Φ和Ψ分别表示小波分解的平移函数和母小波函数,J表示最优分解尺度,j代表不同的分解尺度,v,w分别表示低频小波系数和高频小波系数,ε=1,2,3分别对应水平、垂直和对角方向;In the formula, m and n represent the number of rows and columns of the interferogram, respectively, x, y are the coordinates of the pixel in the radar coordinate system, i x and i y represent the ith row and the ith column of the interferogram, respectively, Φ and Ψ represent the translation function and mother wavelet function of wavelet decomposition, respectively, J represents the optimal decomposition scale, j represents different decomposition scales, v, w represent low-frequency wavelet coefficients and high-frequency wavelet coefficients, ε=1, 2, 3 Corresponding to the horizontal, vertical and diagonal directions respectively;

步骤4中的相关性分析方法为,取两个子视差分干涉图在每个分解尺度下的高频小波系数

Figure BDA0002417446130000031
Figure BDA0002417446130000032
按以下公式进行相关值计算:The correlation analysis method in step 4 is to take the high-frequency wavelet coefficients of the two sub-parallax differential interferograms at each decomposition scale.
Figure BDA0002417446130000031
and
Figure BDA0002417446130000032
The correlation value is calculated according to the following formula:

Figure BDA0002417446130000033
Figure BDA0002417446130000033

在小波分解得到ε=1,2,3时的高频小波系数

Figure BDA0002417446130000034
Figure BDA0002417446130000035
时,代入上述相关性计算公式中,即可通过方程组计算得到两个子视差分干涉图在分解尺度j时的相关值fj和整体偏移系数cj;High-frequency wavelet coefficients obtained when ε = 1, 2, 3 are obtained from wavelet decomposition
Figure BDA0002417446130000034
and
Figure BDA0002417446130000035
When , substituting into the above correlation calculation formula, the correlation value f j and the overall offset coefficient c j of the two sub-parallax differential interferograms at the decomposition scale j can be obtained through the equation system calculation;

再使用两个子视差分干涉图在分解尺度j时的相关性fj和整体偏移系数cj,按以下公式计算对流层延迟误差相位对应的高频小波系数:Then use the correlation f j of the two sub-parallax differential interferograms when decomposing scale j and the overall offset coefficient c j to calculate the high-frequency wavelet coefficient corresponding to the tropospheric delay error phase according to the following formula:

Figure BDA0002417446130000036
Figure BDA0002417446130000036

式中,

Figure BDA0002417446130000037
代表对流层延迟误差相位所对应的高频小波系数;
Figure BDA0002417446130000038
表示方位向入射角为αi子视差分干涉图在分解尺度j时高频小波系数。In the formula,
Figure BDA0002417446130000037
represents the high-frequency wavelet coefficient corresponding to the tropospheric delay error phase;
Figure BDA0002417446130000038
Represents the high-frequency wavelet coefficients when the azimuthal incident angle is α i sub-parallax interferogram at decomposition scale j.

在更优的技术方案中,去除平地相位时,平地相位的计算公式为:In a better technical solution, when the flat-earth phase is removed, the calculation formula of the flat-earth phase is:

Figure BDA0002417446130000039
Figure BDA0002417446130000039

式中,φflat为平地相位,λ为雷达信号波长,B//是平行基线长度。In the formula, φ flat is the phase of the flat ground, λ is the wavelength of the radar signal, and B // is the length of the parallel baseline.

在更优的技术方案中,轨道误差相位的去除方法为:使用融入地表高程h的多项式模型拟合轨道误差相位,通过最小二乘法解算多项式模型中的未知参数,然后将轨道误差相位从子视差分干涉图中对应像素点的解缠相位中去除,得到新的子视差分干涉图。In a better technical solution, the method of removing the orbital error phase is as follows: use a polynomial model integrated with the surface elevation h to fit the orbital error phase, solve the unknown parameters in the polynomial model by the least square method, and then convert the orbital error phase from the sub- The unwrapped phase of the corresponding pixel in the parallax interferogram is removed to obtain a new sub-parallax interferogram.

最后,将轨道误差相位φorbit从子视差分干涉图中对应像素点的解缠相位中去除。Finally, the orbit error phase φ orbit is removed from the unwrapped phase of the corresponding pixel in the subparallax interferogram.

在更优的技术方案中,步骤1采用子孔径分解技术将全孔径SAR影像分解的过程为:In a better technical solution, in step 1, the sub-aperture decomposition technology is used to decompose the full-aperture SAR image as follows:

首先,对全孔径SAR影像进行一维傅利叶变换,得到SAR影像在方位向上的频谱;First, perform one-dimensional Fourier transform on the full-aperture SAR image to obtain the spectrum of the SAR image in the azimuth direction;

然后,对SAR影像在方位向上的频谱按不同的方位向入射角进行分割,得到与方位向入射角对应的频谱;Then, the spectrum of the SAR image in the azimuth direction is divided according to different azimuth incident angles, and the spectrum corresponding to the azimuth incident angle is obtained;

最后,对所有与方位向入射角对应的频谱均进行傅里叶逆变换,得到与方位向入射角对应的影像,即为与方位向入射角对应的子视影像。Finally, inverse Fourier transform is performed on all the spectrums corresponding to the azimuthal incident angle to obtain an image corresponding to the azimuthal incident angle, that is, the subview image corresponding to the azimuthal incident angle.

在更优的技术方案中,对全孔径SAR影像进行预处理包括:对2个全孔径SAR影像进行共配准,然后逐像素共轭相乘生成全孔径干涉图;In a better technical solution, the preprocessing of the full-aperture SAR image includes: co-registering two full-aperture SAR images, and then pixel-by-pixel conjugate multiplication to generate a full-aperture interferogram;

对主、辅影像每个方位向入射角对应的2个子视影像进行预处理包括:将当前方位向入射角对应的2个子视影像逐像素共轭相乘得到当前方位向入射角对应的子视干涉图。Preprocessing the two sub-view images corresponding to each azimuth incident angle of the main and auxiliary images includes: multiplying the two sub-view images corresponding to the current azimuth incident angle pixel by pixel to obtain the sub-view corresponding to the current azimuth incident angle. Interferogram.

本发明还提供一种基于单基线的地表高程校正装置,包括:The present invention also provides a surface elevation correction device based on a single baseline, comprising:

子孔径分解模块,用于:获取两个全孔径SAR影像,采用子孔径分解技术将每个全孔径SAR影像分解为两个与方位向入射角对应的子视影像;The sub-aperture decomposition module is used to: acquire two full-aperture SAR images, and use the sub-aperture decomposition technology to decompose each full-aperture SAR image into two sub-view images corresponding to the azimuth incident angle;

数据预处理模块,用于:对两个全孔径SAR影像进行预处理得到全孔径干涉图;对同一方位向入射角的两个子视影像进行预处理,得到与方位向入射角对应的子视干涉图;The data preprocessing module is used to: preprocess the two full-aperture SAR images to obtain the full-aperture interferogram; preprocess the two sub-view images with the same azimuth incident angle to obtain the sub-view interference corresponding to the azimuth incident angle picture;

差分干涉相位建模模块,用于:对两个子视干涉图,均使用DEM数据并采用差分干涉技术进行去地形处理,然后再去除平地相位和轨道误差相位处理,得到两个如以下公式所示的子视差分干涉图:The differential interferometric phase modeling module is used to: use DEM data for two sub-view interferograms and use differential interferometric technology to perform topographic processing, and then remove the flat phase and orbit error phase processing, and obtain two as shown in the following formulas The subparallax interferogram of :

Figure BDA0002417446130000041
Figure BDA0002417446130000041

式中,α1和α2分别代表两个不同的方位向入射角,φdiff为子视差分干涉图中的差分干涉相位,△φtopo为地形误差相位,φatmo为对流层延迟误差相位,φnoise为随机噪声误差相位;where α 1 and α 2 represent two different azimuthal incident angles, respectively, φ diff is the differential interference phase in the subparallax interferogram, Δφ topo is the topographic error phase, φ atmo is the tropospheric delay error phase, φ noise is the random noise error phase;

对流层延迟误差相位提取模块,用于:对两个子视差分干涉图进行小波分解,对两个子视差分干涉图在每个分解尺度下的高频小波系数进行相关性分析,得到对应分解尺度下两个高频小波系数之间的相关值,根据相关值和任一高频小波系数计算得到对流层延迟误差相位相关的小波系数;然后对所述与对流层延迟误差相位相关的小波系数进行小波逆变换,即可得到对流层延迟误差相位;The tropospheric delay error phase extraction module is used to: perform wavelet decomposition on two sub-parallax differential interferograms, perform correlation analysis on the high-frequency wavelet coefficients of the two sub-parallax differential interferograms at each decomposition scale, and obtain two sub-parallax differential interferograms at the corresponding decomposition scale. The correlation value between the high-frequency wavelet coefficients is calculated according to the correlation value and any high-frequency wavelet coefficient to obtain the wavelet coefficient related to the phase of the tropospheric delay error; The tropospheric delay error phase can be obtained;

地表高程数据校正模块,用于:对全孔径干涉图进行解缠处理,将得到的对流层延迟误差相位从全孔径干涉图的解缠相位中去除;最后,根据卫星轨道参数以及去除对流层延迟误差相位的全孔径干涉图解缠相位,计算得到地表高程数据。The surface elevation data correction module is used for: unwrapping the full-aperture interferogram, and removing the obtained tropospheric delay error phase from the unwrapping phase of the full-aperture interferogram; finally, according to the satellite orbit parameters and removing the tropospheric delay error phase The full-aperture interferogram wraps the phase and calculates the surface elevation data.

本发明还提供一种设备,包括处理器和存储器;其中:所述存储器用于存储计算机指令;所述处理器用于执行所述存储器存储的计算机指令,具体执行上述任一所述的方法。The present invention also provides a device, comprising a processor and a memory; wherein: the memory is used for storing computer instructions; the processor is used for executing the computer instructions stored in the memory, specifically performing any of the above methods.

本发明还提供一种计算机存储介质,用于存储程序,所述程序被执行时,用于实现上述任一所述的方法。The present invention also provides a computer storage medium for storing a program, and when the program is executed, it is used to implement any one of the above-mentioned methods.

有益效果beneficial effect

本发明一种基于子孔径相关性分析的对流层延迟误差改正方法,其优点是:A tropospheric delay error correction method based on sub-aperture correlation analysis of the present invention has the following advantages:

(1)本发明基于子孔径分解技术获取不同方位向入射角下的子视干涉图,通过相关性分析提取相同的对流层延迟误差相位并予以剔除,削弱对流层延迟误差对InSAR测高的影响,从而提高了InSAR技术的测高精度;(1) The present invention obtains sub-view interferograms under different azimuth incident angles based on the sub-aperture decomposition technology, extracts the same tropospheric delay error phase through correlation analysis and eliminates it, and weakens the influence of the tropospheric delay error on InSAR height measurement, thereby Improve the measurement accuracy of InSAR technology;

(2)本发明无需过多SAR数据量,只需两景全孔径SAR影像形成单基线即可,且无需外部水汽辅助数据的情况下,通过对流层延迟误差相位在与方位向入射角的独立性,即可获取对流层延迟相位的分布特征;(2) The present invention does not need too much SAR data, only needs two full-aperture SAR images to form a single baseline, and without external water vapor auxiliary data, the tropospheric delay error phase is independent of the azimuth incident angle , the distribution characteristics of the tropospheric delay phase can be obtained;

(3)本发明利用相关性分析,从两个子视差分干涉图中提取相同的对流层延迟误差相位成分,即可提取消除干涉图中混叠的对流层延迟误差相位,相较于传统方法,本发明可以同时去除与地形相关的垂直分层大气以及与地面高度不相关的湍流大气延迟成分,从而极大地拓宽了InSAR测高的应用范围。(3) The present invention uses correlation analysis to extract the same tropospheric delay error phase components from two sub-parallax interferograms, so as to extract the tropospheric delay error phase that eliminates aliasing in the interferograms. Compared with the traditional method, the present invention has The vertical stratified atmosphere related to the terrain and the turbulent atmospheric delay component not related to the ground height can be removed at the same time, thus greatly broadening the application range of InSAR altimetry.

附图说明Description of drawings

图1为本发明实施例所述方法的流程图。FIG. 1 is a flowchart of a method according to an embodiment of the present invention.

图2为本发明实施例所述子孔径相关性分析对流层延迟误差改正算法详细流程;FIG. 2 is a detailed flowchart of the sub-aperture correlation analysis tropospheric delay error correction algorithm according to the embodiment of the present invention;

图3为本发明实施例所述SAR影像子孔径分解的示意图。FIG. 3 is a schematic diagram of sub-aperture decomposition of a SAR image according to an embodiment of the present invention.

图4为本发明实施例所述方法得到的DEM结果。FIG. 4 is a DEM result obtained by the method described in the embodiment of the present invention.

具体实施方式Detailed ways

为了更好的说明本发明的方法与步骤,利用位于洛杉矶地区两景间隔92天的ALOS1PALSAR雷达数据,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施仅用以解释本发明,并不用于限定本发明。In order to better illustrate the method and steps of the present invention, the present invention is further described in detail by using the ALOS1PALSAR radar data of two scenes located in the Los Angeles area with an interval of 92 days. It should be understood that the specific implementations described herein are only used to explain the present invention, but not to limit the present invention.

本发明实施例提供一种基于单基线的地表高程校正方法,如图1、2所示,包括以下步骤:An embodiment of the present invention provides a single-baseline-based surface elevation correction method, as shown in Figures 1 and 2, including the following steps:

步骤1,获取研究区域的两个全孔径SAR影像,采用子孔径分解技术将每个全孔径SAR影像分解为两个与方位向入射角对应的子视影像,基本原理如图3所示;每个全孔径SAR影像对应得到两个子视影像,称为前视影像和后视影像。Step 1: Acquire two full-aperture SAR images in the study area, and use sub-aperture decomposition technology to decompose each full-aperture SAR image into two sub-view images corresponding to the azimuth incident angle. The basic principle is shown in Figure 3; Two full-aperture SAR images correspond to two sub-view images, which are called forward-view images and rear-view images.

其中的两个全孔径SAR影像:1个全孔径SAR影像为2010年7月11日获取的ALOS1PALSAR雷达数据,本实施例中以该影像为主影像;另1个全孔径SAR影像为2010年10月11日获取的ALOS1 PALSAR雷达数据,本实施例以该影像为辅影像。Among them, two full-aperture SAR images: one full-aperture SAR image is the ALOS1PALSAR radar data acquired on July 11, 2010, and this image is the main image in this embodiment; the other full-aperture SAR image is from October 2010 The ALOS1 PALSAR radar data acquired on January 11, this example uses this image as the auxiliary image.

采用子孔径分解技术将全孔径SAR影像分解的过程具体为:The process of decomposing full-aperture SAR images using sub-aperture decomposition technology is as follows:

首先,对全孔径SAR影像进行一维傅利叶变换,得到SAR影像在方位向上的频谱;First, perform one-dimensional Fourier transform on the full-aperture SAR image to obtain the spectrum of the SAR image in the azimuth direction;

然后,对SAR影像在方位向上的频谱按不同的方位向入射角进行分割,得到与方位向入射角对应的频谱;Then, the spectrum of the SAR image in the azimuth direction is divided according to different azimuth incident angles, and the spectrum corresponding to the azimuth incident angle is obtained;

最后,对所有与方位向入射角对应的频谱均进行傅里叶逆变换,得到与方位向入射角对应的影像,即为与方位向入射角对应的子视影像。Finally, inverse Fourier transform is performed on all the spectrums corresponding to the azimuthal incident angle to obtain an image corresponding to the azimuthal incident angle, that is, the subview image corresponding to the azimuthal incident angle.

在具体实施中,采用子孔径分解技术对每个全孔径SAR影像均分解为两个不同方位向入射角的子视影像,具体通过采用两个不同方位向入射角的带通滤波器,生成不同方位向观测角度的子视影像。In the specific implementation, the sub-aperture decomposition technology is used to decompose each full-aperture SAR image into two sub-view images with different azimuth incident angles. Specifically, by using two band-pass filters with different azimuth incident angles, different A subview image of the azimuthal viewing angle.

步骤2,对两个全孔径SAR影像进行预处理得到全孔径干涉图;对同一方位向入射角的两个子视影像进行预处理,得到与方位向入射角对应的子视干涉图;Step 2, preprocessing two full-aperture SAR images to obtain a full-aperture interferogram; preprocessing two sub-view images with the same azimuth incident angle to obtain a sub-view interferogram corresponding to the azimuth incident angle;

对全孔径SAR影像进行预处理包括:对2个全孔径SAR影像进行共配准,然后逐像素共轭相乘生成全孔径干涉图;The preprocessing of full-aperture SAR images includes: co-registration of two full-aperture SAR images, and then pixel-by-pixel conjugate multiplication to generate a full-aperture interferogram;

对每个方位向入射角的两个子视影像进行预处理包括:将当前方位向入射角对应的2个子视影像进行干涉处理,得到当前方位向入射角对应的子视干涉图。Preprocessing the two sub-view images of each azimuth incident angle includes: performing interference processing on the two sub-view images corresponding to the current azimuth incident angle to obtain a sub-view interferogram corresponding to the current azimuth incident angle.

步骤3,对两个子视干涉图,均使用DEM数据并采用差分干涉技术进行去地形处理,然后再去除平地相位和轨道误差相位处理,得到两个如以下公式所示的子视差分干涉图:Step 3: For the two sub-parallax interferograms, both use DEM data and use differential interferometry to perform topographic processing, and then remove the flat-ground phase and orbit error phase processing to obtain two sub-parallax differential interferograms as shown in the following formulas:

Figure BDA0002417446130000063
Figure BDA0002417446130000063

式中,α1和α2代表两个不同的方位向入射角,φdiff为子视差分干涉图中的差分干涉相位,△φtopo为地形误差相位,φatmo为对流层延迟误差相位,φnoise为随机噪声误差相位。where α 1 and α 2 represent two different azimuthal incident angles, φ diff is the differential interference phase in the subparallax interferogram, Δφ topo is the topographic error phase, φ atmo is the tropospheric delay error phase, and φ noise is the random noise error phase.

具体地,星载重复轨道InSAR在进行对地观测时,会受到大气、地表形变等多种因素的影响,因此,InSAR干涉相位表现为多种相位成分的叠加。Specifically, the space-borne repetitive orbit InSAR will be affected by various factors such as atmosphere and surface deformation during earth observation. Therefore, the InSAR interference phase appears as the superposition of various phase components.

为了保证干涉图的相位质量,本实施例选择时间基线较短的两个SAR影像,地表形变几乎为零,因此可以不考虑地表形变的影响;此外,相较于对流层延迟而言,电离层延迟的量级一般都比较小,所以忽略电离层延迟的影响。因此,本发明实施例针对InSAR地形测量,在不考虑地表形变和电离层延迟的影响下,将不同观测角度下干涉图的相位φint可以表示为:In order to ensure the phase quality of the interferogram, this embodiment selects two SAR images with short time baselines, and the surface deformation is almost zero, so the influence of the surface deformation can be ignored; in addition, compared with the tropospheric delay, the ionospheric delay The magnitude of is generally relatively small, so the effect of ionospheric delay is ignored. Therefore, for the InSAR terrain measurement in the embodiment of the present invention, without considering the influence of surface deformation and ionospheric delay, the phase φ int of the interferogram under different observation angles can be expressed as:

Figure BDA0002417446130000061
Figure BDA0002417446130000061

式中:where:

α1和α2代表两个不同的方位向入射角;α 1 and α 2 represent two different azimuthal incident angles;

φtopo是地形测量相关的地形相位,其与裸地表高程h和地表散射目标的高度△h有关;φ topo is the topographic phase related to topographic measurement, which is related to the bare surface elevation h and the height Δh of the surface scattering target;

φflat为平地相位,可以表示为:

Figure BDA0002417446130000062
可以根据卫星的轨道参数将其进行有效的去除;λ是雷达波长,B//是平行基线;φ flat is the flat-earth phase, which can be expressed as:
Figure BDA0002417446130000062
It can be effectively removed according to the orbital parameters of the satellite; λ is the radar wavelength, B // is the parallel baseline;

φorbit为轨道误差相位,是由不精确的轨道参数导致,在常规InSAR处理中,通常采用多项式模型拟合方法去除;φ orbit is the orbit error phase, which is caused by inaccurate orbit parameters. In conventional InSAR processing, polynomial model fitting method is usually used to remove it;

φnoise为随机噪声误差相位,可以采用干涉图滤波处理将其削弱;φ noise is the phase of random noise error, which can be weakened by interferogram filtering;

φatmo为对流层延迟误差相位,可以表示为:

Figure BDA0002417446130000071
主要产生原因为两次成像过程中微波信号受到不同水汽环境的干扰,干涉后以相位的形式体现在干涉图中。φ atmo is the tropospheric delay error phase, which can be expressed as:
Figure BDA0002417446130000071
The main reason is that the microwave signal is interfered by different water vapor environments during the two imaging processes, and is reflected in the interferogram in the form of phase after the interference.

根据以上对干涉图中相位成分的分析,干涉图中只有对流层延迟误差很难通过固定的模型进行有效的去除,其成为了星载重轨SAR地形测量的主要误差来源。According to the above analysis of the phase components in the interferogram, only the tropospheric delay error in the interferogram is difficult to be effectively removed by a fixed model, which has become the main source of error in the topographic measurement of spaceborne heavy-orbit SAR.

目前已有研究表明,方位向入射角的变化会导致后向散射特性的变化,因此不同子视干涉图具有不同的干涉相位中心。另外,由于不同方位向入射角下的子视影像共用了近似相同的轨道参数,由上述平地相位和轨道误差相位的分析可得,各子视干涉相位中包含了相同的平地相位和轨道误差相位。由于SAR传感器合成孔径时间一般都很短(一般为几秒),并且考虑到星载SAR传感器较小的波束宽度角,可以认为不同子孔径雷达波在传输过程中穿过的大气成分近似相同,进而导致不同子孔径影像含有相同的对流层延迟误差,这些相同的对流层延迟误差经过干涉处理,就转换为相同的对流层延迟误差相位。尽管各孔径影像只包含全孔径SAR影像频谱的一部分,但是其包含的对流层延迟误差相位是相同的。该特征为相同对流层延迟误差的提取和去除提供了可能。Studies have shown that the change of the azimuthal incident angle will lead to the change of the backscattering characteristics, so different sub-view interferograms have different interference phase centers. In addition, since the sub-view images under different azimuth incident angles share approximately the same orbital parameters, from the analysis of the above-mentioned flat-ground phase and orbit error phase, it can be obtained that each sub-view interference phase contains the same flat-ground phase and orbit error phase. . Since the synthetic aperture time of SAR sensors is generally very short (usually several seconds), and considering the small beam width angle of spaceborne SAR sensors, it can be considered that the atmospheric components that different sub-aperture radar waves pass through during transmission are approximately the same, As a result, different sub-aperture images contain the same tropospheric delay error, and these same tropospheric delay errors are converted into the same tropospheric delay error phase after interference processing. Although each aperture image contains only a portion of the full-aperture SAR image spectrum, it contains the same tropospheric delay error phase. This feature makes it possible to extract and remove the same tropospheric delay errors.

在本步骤3中,为了提取相同的对流层延迟误差相位,需要先将各子视干涉图中的裸地高程对应的地形相位、平地相位和轨道误差相位成分进行去除。In this step 3, in order to extract the same tropospheric delay error phase, it is necessary to first remove the terrain phase, flat phase and orbit error phase components corresponding to the bare ground elevation in each sub-view interferogram.

首先采用差分干涉技术进行去地形处理,即采用外部DEM数据模拟地形相位,将地形相位从干涉相位中去除:First, the differential interference technology is used to remove the terrain, that is, the terrain phase is simulated by using external DEM data, and the terrain phase is removed from the interference phase:

Figure BDA0002417446130000072
Figure BDA0002417446130000072

Figure BDA0002417446130000073
Figure BDA0002417446130000073

式中,

Figure BDA0002417446130000074
为采用外部DEM数据h模拟得到的地形相位,△φtopo为地形误差相位,由外部DEM数据的不准确所导致;B代表垂直基线的长度,λ为雷达信号波长,R1和R2分别表示主、辅影像的天线中心到地面目标点的距离。In the formula,
Figure BDA0002417446130000074
is the terrain phase simulated by the external DEM data h, Δφ topo is the terrain error phase, which is caused by the inaccuracy of the external DEM data; B represents the length of the vertical baseline, λ is the radar signal wavelength, R 1 and R 2 respectively Indicates the distance from the antenna center of the main and auxiliary images to the ground target point.

尽管不同方位向观测角度下的干涉图对应着不同的相位中心,在差分干涉进行去地形处理过程中,如果采用同一个外部DEM数据来去除不同极化干涉图中的地形相位,会导致各子视影像对应的子视差分干涉图中含有相似的地形误差相位,这将严重干扰后续相同对流层延迟误差相位的提取。因此,本实施例分别采用不同技术手段获取的外部DEM数据进行去地形处理,分别去除相应子视干涉图中的地形相位,可以增强最终得到的两个子视差分干涉图的区分度,从而极大提高对流层延迟误差的估计精度。Although the interferograms at different azimuth observation angles correspond to different phase centers, in the process of removing the topography by differential interferometry, if the same external DEM data is used to remove the topographic phases in the interferograms of different polarizations, it will lead to various sub-interferences. The subparallax interferograms corresponding to the visual images contain similar terrain error phases, which will seriously interfere with the subsequent extraction of the same tropospheric delay error phase. Therefore, in this embodiment, the external DEM data obtained by different technical means are used to perform terrain removal processing, and the terrain phases in the corresponding sub-view interferograms are respectively removed, which can enhance the discrimination of the two finally obtained sub-parallax differential interferograms. Improve estimation accuracy of tropospheric delay error.

然后,使用平地相位计算公式

Figure BDA0002417446130000081
根据卫星的轨道参数λ、R2、R1计算平地相位,进而将平地相位从子视干涉相位中去除:Then, use the flat-earth phase calculation formula
Figure BDA0002417446130000081
Calculate the flat-earth phase according to the satellite's orbital parameters λ, R 2 , and R 1 , and then remove the flat-earth phase from the sub-view interference phase:

Figure BDA0002417446130000082
Figure BDA0002417446130000082

再后,使用融入地表高程h的多项式模型拟合轨道误差相位,通过最小二乘法解算多项式中的未知参数,然后将轨道误差相位从子视差分干涉图中对应像素点的解缠相位中去除,得到新的子视差分干涉图。Then, use the polynomial model integrated into the surface elevation h to fit the orbit error phase, solve the unknown parameters in the polynomial by the least square method, and then remove the orbit error phase from the unwrapped phase of the corresponding pixel in the subparallax interferogram. , to obtain a new subparallax interferogram.

具体在本实施例中,使用多项式a0+a1x+a2y+a3h拟合轨道误差相位φorbit,得到轨道误差相位模型为:

Figure BDA0002417446130000083
其中x,y是像素点在雷达坐标系的坐标,hi为第i个像素对应的地表高程,a1,a2,a3为待求参数;Specifically in this embodiment, the orbit error phase φ orbit is fitted by using the polynomial a 0 +a 1 x+a 2 y+a 3 h, and the orbit error phase model is obtained as:
Figure BDA0002417446130000083
where x, y are the coordinates of the pixel in the radar coordinate system, hi is the surface elevation corresponding to the ith pixel, and a 1 , a 2 , and a 3 are the parameters to be determined;

为了准确估计未知参数a1,a2,a3的值,可以采用上述轨道误差相位模型对解缠后的子视差分干涉相位进行拟合,然后采用最小二乘方法解算未知参数a1,a2,a3;随后即可以根据出每一像素对应的坐标x,y与地表高程hi,通过上述轨道误差相位模型计算其轨道误差相位φorbitIn order to accurately estimate the values of the unknown parameters a 1 , a 2 , a 3 , the above orbital error phase model can be used to fit the unwrapped subparallax interferometric phase, and then the least squares method can be used to solve the unknown parameters a 1 , a 2 , a 3 ; then, according to the coordinates x, y and the surface elevation hi corresponding to each pixel , the orbit error phase φ orbit can be calculated through the above orbit error phase model.

另外需要注意的是:对于非线性的轨道误差相位,在实际应用中可以通过选择高次多项式来替代本实施例中的多项a0+a1x+a2y+a3h进行计算。It should also be noted that: for the nonlinear track error phase, in practical applications, a high-order polynomial can be selected to replace the polynomial a 0 +a 1 x+a 2 y+a 3 h in this embodiment for calculation.

将轨道误差相位φorbit从子视差分干涉图中对应像素点的解缠相位中去除,即可得到新的子视差分干涉图:The orbit error phase φ orbit is removed from the unwrapping phase of the corresponding pixel in the sub-parallax interferogram, and a new sub-parallax interferogram can be obtained:

Figure BDA0002417446130000084
Figure BDA0002417446130000084

其中,φdiff为子视差分干涉图中的差分干涉相位。Among them, φ diff is the differential interference phase in the sub-parallax differential interferogram.

步骤4,对两个子视差分干涉图进行小波分解,对两个子视差分干涉图在每个分解尺度下的高频小波系数进行相关性分析,得到对应分解尺度下两个高频小波系数之间的相关值,根据相关值和任一高频小波系数计算得到对流层延迟误差相位相关的小波系数;然后对所述与对流层延迟误差相位相关的小波系数进行小波逆变换,即可得到对流层延迟误差相位。Step 4: Perform wavelet decomposition on the two sub-parallax differential interferograms, perform correlation analysis on the high-frequency wavelet coefficients of the two sub-parallax differential interferograms at each decomposition scale, and obtain the difference between the two high-frequency wavelet coefficients at the corresponding decomposition scale. The correlation value of , and the wavelet coefficient related to the tropospheric delay error phase is calculated according to the correlation value and any high-frequency wavelet coefficient; then the wavelet coefficient related to the tropospheric delay error phase is subjected to wavelet inverse transformation to obtain the tropospheric delay error phase. .

对于对流层延迟误差在空间上分布的复杂性,使得我们难以通过简单的空间滤波将其进行有效的分离。然而,差分干涉图中不同的相位成分在频率域表现为了不同的波长成分,因此小波变换可以将差分干涉图分解为不同的波长成分,允许我们在不同尺度下对其进行研究。因此,本发明实施例采用小波变换将差分干涉图分解到不同的尺度,并在每一分解尺度下估计对流层延迟误差相位的大小。The complexity of the spatial distribution of tropospheric delay errors makes it difficult to separate them effectively by simple spatial filtering. However, different phase components in the differential interferogram appear as different wavelength components in the frequency domain, so wavelet transform can decompose the differential interferogram into different wavelength components, allowing us to study them at different scales. Therefore, the embodiments of the present invention use wavelet transform to decompose the differential interferogram into different scales, and estimate the magnitude of the tropospheric delay error phase in each decomposition scale.

对子视差分干涉图进行小波分解表示为:The wavelet decomposition of the subparallax interferogram is expressed as:

Figure BDA0002417446130000091
Figure BDA0002417446130000091

式中,m和n分别表示干涉图的行数和列数,x,y是像素点在雷达坐标系的坐标,ix和iy分别表示干涉图的第ix行和第iy列,Φ和Ψ分别表示小波分解的平移函数和母小波函数,J表示最优分解尺度,j代表不同的分解尺度,v,w分别表示低频小波系数和高频小波系数,ε=1,2,3分别对应水平、垂直和对角方向;In the formula, m and n represent the number of rows and columns of the interferogram, respectively, x, y are the coordinates of the pixel in the radar coordinate system, i x and i y represent the ith row and the ith column of the interferogram, respectively, Φ and Ψ represent the translation function and mother wavelet function of wavelet decomposition, respectively, J represents the optimal decomposition scale, j represents different decomposition scales, v, w represent low-frequency wavelet coefficients and high-frequency wavelet coefficients, ε=1, 2, 3 Corresponding to the horizontal, vertical and diagonal directions respectively;

在两个子视差分干涉图中,如前述分析对流层延迟误差相位相同,且对流层延迟误差在频率域通常表现为长波长的高频信息,因此它们的高频小波系数间具有一定的相似性,然后对不同子视干涉图每一分解尺度下的高频系数(分别表示为

Figure BDA0002417446130000092
)分别进行如下的整体相关性分析计算:In the two subparallax interferograms, the phase of the tropospheric delay error is the same as analyzed above, and the tropospheric delay error is usually expressed as long-wavelength high-frequency information in the frequency domain, so their high-frequency wavelet coefficients have a certain similarity, then For the high-frequency coefficients of different sub-view interferograms at each decomposition scale (represented as
Figure BDA0002417446130000092
) respectively perform the following overall correlation analysis and calculation:

Figure BDA0002417446130000093
Figure BDA0002417446130000093

在小波分解得到ε=1,2,3时的高频小波系数

Figure BDA0002417446130000094
Figure BDA0002417446130000095
时,代入上述相关性计算公式中,即可通过方程组计算得到两个子视差分干涉图在分解尺度j时的相关值fj和整体偏移系数cj;High-frequency wavelet coefficients obtained when ε = 1, 2, 3 are obtained from wavelet decomposition
Figure BDA0002417446130000094
and
Figure BDA0002417446130000095
When , substituting into the above correlation calculation formula, the correlation value f j and the overall offset coefficient c j of the two sub-parallax differential interferograms at the decomposition scale j can be obtained through the equation system calculation;

再使用两个子视差分干涉图在分解尺度j时的相关性fj和整体偏移系数cj,按以下公式计算对流层延迟误差相位对应的高频小波系数:Then use the correlation f j of the two sub-parallax differential interferograms when decomposing scale j and the overall offset coefficient c j to calculate the high-frequency wavelet coefficient corresponding to the tropospheric delay error phase according to the following formula:

Figure BDA0002417446130000096
Figure BDA0002417446130000096

式中,

Figure BDA0002417446130000097
代表对流层延迟误差相位所对应的高频小波系数;
Figure BDA0002417446130000098
表示方位向入射角为αi子视差分干涉图的在分解尺度j时高频小波系数。对流层延迟误差相位对应的高频小波系数时,具体可取两个方位向入射角中任意一个对应的子视差分干涉图得到的高频小波系数
Figure BDA0002417446130000101
进行计算。In the formula,
Figure BDA0002417446130000097
represents the high-frequency wavelet coefficient corresponding to the tropospheric delay error phase;
Figure BDA0002417446130000098
Represents the high-frequency wavelet coefficients at the decomposition scale j of the subparallax interferogram whose azimuthal incident angle is α i . When the high-frequency wavelet coefficient corresponding to the tropospheric delay error phase, the high-frequency wavelet coefficient obtained from the sub-parallax interferogram corresponding to any one of the two azimuth incident angles can be used.
Figure BDA0002417446130000101
Calculation.

最后,为了提取子视差分干涉图中包含的对流层延迟误差相位,对上述得到的与对流层延迟误差相位相关的小波系数进行小波逆变换,即可得到全孔径干涉图相位中包含的对流层延迟误差相位。Finally, in order to extract the tropospheric delay error phase contained in the subparallax interferogram, the wavelet coefficients related to the tropospheric delay error phase obtained above are subjected to wavelet inverse transformation, and the tropospheric delay error phase contained in the phase of the full aperture interferogram can be obtained. .

步骤5,对全孔径干涉图进行解缠处理,将步骤4得到的对流层延迟误差相位从全孔径干涉图的解缠相位中去除;最后,根据卫星轨道参数以及去除对流层延迟误差相位的全孔径干涉图解缠相位,按下以公式计算得到地表高程数据h:In step 5, the full aperture interferogram is unwrapped, and the tropospheric delay error phase obtained in step 4 is removed from the unwrapped phase of the full aperture interferogram; finally, according to the satellite orbit parameters and the full aperture interferogram that removes the tropospheric delay error phase To plot the entanglement phase, the surface elevation data h can be calculated by the following formula:

Figure BDA0002417446130000102
Figure BDA0002417446130000102

式中,θ为主影像各像素点的天线入射角,α为基线倾角,φ'topo表示去除对流层延迟误差相位的全孔径干涉图解缠相位。In the formula, θ is the antenna incident angle of each pixel point of the main image, α is the baseline inclination angle, and φ' topo represents the full-aperture interferogram wrapping phase with the tropospheric delay error phase removed.

在更优的实施例中,还包括对全孔径干涉图解缠相位φ'topo进行噪声滤除处理,即去除随机噪声误差相位,再将随机噪声误差相位和对流层延迟误差相位从全孔径干涉图的解缠相位中去除,将此时的地形相位记为φ”topo,然后使用公式计算得到更高精度的地表高程数据:In a more preferred embodiment, it also includes performing noise filtering processing on the full-aperture interferogram wrapping phase φ' topo , that is, removing the random noise error phase, and then extracting the random noise error phase and the tropospheric delay error phase from the full-aperture interferogram. Remove it from the unwrapping phase, record the terrain phase at this time as φ” topo , and then use the formula to calculate the surface elevation data with higher precision:

Figure BDA0002417446130000103
Figure BDA0002417446130000103

如图4所示,其中图4(a)-(c)分别表示直接使用全孔径SAR影像处理(未进行对流层延迟误差改正)得到的地表高程数据InSAR DEM1、使用本发明实施例去除对流层延迟误差相位后再计算得到的地表高程数据InSAR DEM2以及USGS提供的地表高程数据SRTM DEM;然后将SRTM DEM作为参考数据分别对InSAR DEM1和InSAR DEM2进行了定性分析,得到InSAR DEM1和InSAR DEM2的高程误差分别如图4(d)和4(e)分别所示,可以看到本发明实施方法可以有效的去除InSAR地形测量中的对流层延迟误差。As shown in Figure 4, Figure 4(a)-(c) respectively represent the surface elevation data InSAR DEM1 obtained by directly using the full-aperture SAR image processing (without tropospheric delay error correction), and using the embodiment of the present invention to remove the tropospheric delay error The surface elevation data InSAR DEM2 and the surface elevation data SRTM DEM provided by USGS after calculating the phase; then, the SRTM DEM is used as the reference data to carry out qualitative analysis on InSAR DEM1 and InSAR DEM2 respectively, and the elevation errors of InSAR DEM1 and InSAR DEM2 are obtained respectively. As shown in Figures 4(d) and 4(e) respectively, it can be seen that the implementation method of the present invention can effectively remove the tropospheric delay error in the InSAR topographic measurement.

本发明还提供一种基于单基线的地表高程校正装置,与上述方法实施例相对应,包括:The present invention also provides a single-baseline-based surface elevation correction device, corresponding to the above method embodiments, including:

子孔径分解模块,用于:获取两个全孔径SAR影像,采用子孔径分解技术将每个全孔径SAR影像分解为两个与方位向入射角对应的子视影像;The sub-aperture decomposition module is used to: acquire two full-aperture SAR images, and use the sub-aperture decomposition technology to decompose each full-aperture SAR image into two sub-view images corresponding to the azimuth incident angle;

数据预处理模块,用于:对两个全孔径SAR影像进行预处理得到全孔径干涉图;对同一方位向入射角的两个子视影像进行预处理,得到与方位向入射角对应的子视干涉图;The data preprocessing module is used to: preprocess the two full-aperture SAR images to obtain the full-aperture interferogram; preprocess the two sub-view images with the same azimuth incident angle to obtain the sub-view interference corresponding to the azimuth incident angle picture;

差分干涉相位建模模块,用于:对两个子视干涉图,均使用DEM数据并采用差分干涉技术进行去地形处理,然后再去除平地相位和轨道误差相位处理,得到两个如以下公式所示的子视差分干涉图:The differential interferometric phase modeling module is used to: use DEM data for two sub-view interferograms and use differential interferometric technology to perform topographic processing, and then remove the flat phase and orbit error phase processing, and obtain two as shown in the following formulas The subparallax interferogram of :

Figure BDA0002417446130000111
Figure BDA0002417446130000111

式中,α1和α2分别代表两个不同的方位向入射角,φdiff为子视差分干涉图中的差分干涉相位,△φtopo为地形误差相位,φatmo为对流层延迟误差相位,φnoise为随机噪声误差相位;where α 1 and α 2 represent two different azimuthal incident angles, respectively, φ diff is the differential interference phase in the subparallax interferogram, Δφ topo is the topographic error phase, φ atmo is the tropospheric delay error phase, φ noise is the random noise error phase;

对流层延迟误差相位提取模块,用于:对两个子视差分干涉图进行小波分解,对两个子视差分干涉图在每个分解尺度下的高频小波系数进行相关性分析,取相关性大于预设阈值的高频小波系数,均作为对流层延迟误差相位相关的小波系数;然后对所述与对流层延迟误差相位相关的小波系数进行小波逆变换,即可得到对流层延迟误差相位;The tropospheric delay error phase extraction module is used to: perform wavelet decomposition on the two sub-parallax differential interferograms, perform correlation analysis on the high-frequency wavelet coefficients of the two sub-parallax differential interferograms at each decomposition scale, and take the correlation greater than the preset value. The high-frequency wavelet coefficients of the threshold are all used as the wavelet coefficients related to the phase of the tropospheric delay error; then the wavelet coefficients related to the phase of the tropospheric delay error are subjected to wavelet inverse transformation to obtain the tropospheric delay error phase;

地表高程数据校正模块,用于:将得到的对流层延迟误差相位从全孔径干涉图中去除;最后,根据卫星轨道参数以及去除对流层延迟误差相位的全孔径干涉图,计算得到地表高程数据。The surface elevation data correction module is used to: remove the obtained tropospheric delay error phase from the full aperture interferogram; finally, calculate the surface elevation data according to the satellite orbit parameters and the full aperture interferogram from which the tropospheric delay error phase is removed.

本发明还提供一种设备,包括处理器和存储器;其中:所述存储器用于存储计算机指令;所述处理器用于执行所述存储器存储的计算机指令,具体执行上述方法实施例所述的步骤。The present invention further provides a device including a processor and a memory; wherein: the memory is used to store computer instructions; the processor is used to execute the computer instructions stored in the memory, and specifically perform the steps described in the above method embodiments.

本发明还提供一种计算机存储介质,用于存储程序,所述程序被执行时,用于实现上述方法实施例所述的方法。The present invention also provides a computer storage medium for storing a program, and when the program is executed, it is used to implement the method described in the above method embodiments.

以上实施例为本申请的优选实施例,本领域的普通技术人员还可以在此基础上进行各种变换或改进,在不脱离本申请总的构思的前提下,这些变换或改进都应当属于本申请要求保护的范围之内。The above embodiments are the preferred embodiments of the application, and those of ordinary skill in the art can also carry out various transformations or improvements on this basis. Without departing from the general concept of the application, these transformations or improvements should belong to the present application. within the scope of the application for protection.

Claims (10)

1. A single-baseline-based surface elevation correction method is characterized by comprising the following steps:
step 1, acquiring two full-aperture SAR images of a research area, and decomposing each full-aperture SAR image into two sub-view images corresponding to azimuth incident angles by adopting a sub-aperture decomposition technology;
step 2, preprocessing the two full-aperture SAR images to obtain a full-aperture interferogram; preprocessing two sub-view images with the same azimuth incident angle to obtain a sub-view interferogram corresponding to the azimuth incident angle;
step 3, for the two sub-view interferograms, DEM data are used, a differential interference technology is adopted for terrain removing processing, then flat ground phase and orbit error phase removing processing are carried out, and two sub-view interferograms shown in the following formulas are obtained:
Figure FDA0002417446120000011
in the formula, α1And α2Representing two different azimuthal angles of incidence, phidiffIs the differential interference phase in the sub-parallax partial interference pattern, △ phitopoFor the phase of the terrain error, phiatmoFor tropospheric delay error phase, phinoiseIs a random noise error phase;
step 4, performing wavelet decomposition on the two sub-view differential interferograms, performing correlation analysis on the high-frequency wavelet coefficients of the two sub-view differential interferograms under each decomposition scale to obtain correlation values between the two high-frequency wavelet coefficients under the corresponding decomposition scale, and calculating to obtain wavelet coefficients related to troposphere delay error phases according to the correlation values and any one high-frequency wavelet coefficient; then, performing inverse wavelet transform on the wavelet coefficient related to the troposphere delay error phase to obtain a troposphere delay error phase;
step 5, carrying out unwrapping processing on the full-aperture interferogram, and removing the troposphere delay error phase obtained in the step 4 from the unwrapping phase of the full-aperture interferogram; and finally, calculating to obtain the earth surface elevation data according to the satellite orbit parameters and the wrapped phase of the full-aperture interference diagram with the troposphere delay error phase removed.
2. The method of claim 1, wherein the two sub-view interferograms are topographically processed using two DEM data obtained from different techniques.
3. The method of claim 1, wherein the wavelet decomposition of the sub-view differential interferogram is represented as:
Figure FDA0002417446120000012
in the formula, m and n respectively represent the number of rows and columns of the interference pattern, x and y are coordinates of pixel points in a radar coordinate system, ixAnd iyI th representing interference patterns, respectivelyxRow and ithyColumns, Φ and Ψ respectively represent the translation function and mother wavelet function of the wavelet decomposition, J represents the optimal decomposition scale, J represents different decomposition scales, v, w respectively represent the low-frequency wavelet coefficient and high-frequency wavelet coefficient, and ∈ 1,2,3 respectively corresponds to the horizontal, vertical and diagonal directions;
the correlation analysis method in the step 4 is that the high-frequency wavelet coefficient of the two sub-view difference interferograms under each decomposition scale is taken
Figure FDA0002417446120000021
And
Figure FDA0002417446120000022
the correlation value calculation is performed according to the following formula:
Figure FDA0002417446120000023
high-frequency wavelet coefficient when epsilon is 1,2,3 obtained by wavelet decomposition
Figure FDA0002417446120000024
And
Figure FDA0002417446120000025
then, the correlation value f of the two sub-view differential interferograms in the decomposition scale j can be obtained by calculation of an equation set by substituting the correlation value f into the correlation calculation formulajAnd global offset coefficient cj
Reuse of the correlation f of two sub-view differential interferograms at the decomposition scale jjAnd global offset coefficient cjCalculating a high-frequency wavelet coefficient corresponding to the troposphere delay error phase according to the following formula:
Figure FDA0002417446120000026
in the formula (I), the compound is shown in the specification,
Figure FDA0002417446120000027
representing a high-frequency wavelet coefficient corresponding to the troposphere delay error phase;
Figure FDA0002417446120000028
indicating an azimuthal angle of incidence of αiThe sub-parallax partial interferograms are high frequency wavelet coefficients at decomposition scale j.
4. The method of claim 1, wherein when removing the flat phase, the calculation formula of the flat phase is:
Figure FDA0002417446120000029
in the formula, phiflatIs the phase of the flat ground, λ is the wavelength of the radar signal, B//Is the parallel baseline length.
5. The method of claim 1, wherein the track error phase is removed by: and fitting the orbit error phase by using a polynomial model fused into the earth surface elevation h, resolving unknown parameters in the polynomial model by using a least square method, and then removing the orbit error phase from the unwrapping phase of the corresponding pixel point in the sub-parallax partial interferogram to obtain a new sub-parallax partial interferogram.
6. The method of claim 1, wherein the step 1 of decomposing the full aperture SAR image by using the sub-aperture decomposition technique comprises:
firstly, carrying out one-dimensional Fourier transform on a full-aperture SAR image to obtain a frequency spectrum of the SAR image in the azimuth direction;
then, dividing the frequency spectrum of the SAR image in the azimuth direction according to different azimuth direction incidence angles to obtain a frequency spectrum corresponding to the azimuth direction incidence angle;
and finally, performing inverse Fourier transform on all frequency spectrums corresponding to the azimuth incident angles to obtain images corresponding to the azimuth incident angles, namely the sub-view images corresponding to the azimuth incident angles.
7. The method of claim 1, wherein preprocessing the full aperture SAR image comprises: co-registering the 2 full-aperture SAR images, and then carrying out pixel-by-pixel conjugate multiplication to generate a full-aperture interferogram;
the preprocessing of the 2 sub-view images corresponding to each azimuth incident angle of the main image and the auxiliary image comprises the following steps: and carrying out pixel-by-pixel conjugate multiplication on the 2 sub-view images corresponding to the current azimuth incident angle to obtain a sub-view interference image corresponding to the current azimuth incident angle.
8. A single baseline-based surface elevation correction apparatus, comprising:
a sub-aperture decomposition module to: acquiring two full-aperture SAR images, and decomposing each full-aperture SAR image into two sub-view images corresponding to azimuth incident angles by adopting a sub-aperture decomposition technology;
a data pre-processing module to: preprocessing the two full-aperture SAR images to obtain a full-aperture interferogram; preprocessing two sub-view images with the same azimuth incident angle to obtain a sub-view interferogram corresponding to the azimuth incident angle;
a differential interferometric phase modeling module to: for the two sub-view interferograms, DEM data are used, a differential interference technology is adopted for terrain removing processing, then flat ground phase and orbit error phase removing processing are carried out, and two sub-parallax partial interferograms shown in the following formulas are obtained:
Figure FDA0002417446120000031
in the formula, α1And α2Respectively representing two different azimuthal angles of incidence, phidiffIs the differential interference phase in the sub-parallax partial interference pattern, △ phitopoFor the phase of the terrain error, phiatmoFor tropospheric delay error phase, phinoiseIs a random noise error phase;
a tropospheric delay error phase extraction module for: performing wavelet decomposition on the two sub-view differential interferograms, performing correlation analysis on high-frequency wavelet coefficients of the two sub-view differential interferograms under each decomposition scale to obtain correlation values between the two high-frequency wavelet coefficients under the corresponding decomposition scale, and calculating to obtain wavelet coefficients related to troposphere delay error phases according to the correlation values and any high-frequency wavelet coefficient; then, performing inverse wavelet transform on the wavelet coefficient related to the troposphere delay error phase to obtain a troposphere delay error phase;
a surface elevation data correction module to: carrying out unwrapping processing on the full-aperture interferogram, and removing the obtained troposphere delay error phase from the unwrapping phase of the full-aperture interferogram; and finally, calculating to obtain the earth surface elevation data according to the satellite orbit parameters and the wrapped phase of the full-aperture interference diagram with the troposphere delay error phase removed.
9. An apparatus comprising a processor and a memory; wherein: the memory is to store computer instructions; the processor is configured to execute the computer instructions stored by the memory, in particular to perform the method according to any one of claims 1 to 7.
10. A computer storage medium storing a program which, when executed, performs the method of any one of claims 1 to 7.
CN202010195430.9A 2020-03-19 2020-03-19 Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline Active CN111239736B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202010195430.9A CN111239736B (en) 2020-03-19 2020-03-19 Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202010195430.9A CN111239736B (en) 2020-03-19 2020-03-19 Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline

Publications (2)

Publication Number Publication Date
CN111239736A true CN111239736A (en) 2020-06-05
CN111239736B CN111239736B (en) 2022-02-11

Family

ID=70869555

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202010195430.9A Active CN111239736B (en) 2020-03-19 2020-03-19 Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline

Country Status (1)

Country Link
CN (1) CN111239736B (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111812600A (en) * 2020-06-29 2020-10-23 中南林业科技大学 An Adaptive Terrain Dependent SRTM-DEM Correction Method
CN111833446A (en) * 2020-06-24 2020-10-27 浙江省测绘科学技术研究院 Overhead ground object rapid correction method based on characteristic line extraction
CN112816983A (en) * 2021-01-06 2021-05-18 中南大学 Time sequence InSAR turbulence atmospheric delay correction method based on optimized interferogram set
CN116736306A (en) * 2023-08-15 2023-09-12 成都理工大学 Time sequence radar interference monitoring method based on third high-resolution
CN117665809A (en) * 2023-12-21 2024-03-08 西南林业大学 Inversion method for forest canopy height
CN119805416A (en) * 2024-12-13 2025-04-11 北京空间机电研究所 A method for correcting sea surface ranging errors using satellite-borne single-photon lidar
CN119828138A (en) * 2024-11-22 2025-04-15 武汉工程大学 Multi-baseline InSAR residual phase error correction method and system based on flat land priori information

Citations (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1998002761A1 (en) * 1996-07-11 1998-01-22 Science Applications International Corporation Terrain elevation measurement by interferometric synthetic aperture radar (ifsar)
WO2000054006A2 (en) * 1999-03-08 2000-09-14 Lockheed Martin Corporation Single-pass interferometric synthetic aperture radar
CN101339245A (en) * 2008-08-08 2009-01-07 西安电子科技大学 Multi-Baseline Interferometric Synthetic Aperture Radar Interferometric Phase Unwrapping Method
EP2017647A1 (en) * 2007-07-19 2009-01-21 Consiglio Nazionale delle Ricerche Method for processing data sensed by a synthetic aperture radar (SAR) and related remote sensing system
CN101609151A (en) * 2009-07-17 2009-12-23 重庆大学 A Moving Target Detection Method Based on Eigenvalue Decomposition of Single-Channel Synthetic Aperture Radar (SAR) Image Sequence
CN101706577A (en) * 2009-12-01 2010-05-12 中南大学 Method for monitoring roadbed subsidence of express way by InSAR
US20120019410A1 (en) * 2009-07-08 2012-01-26 Politecnico Di Milano Process for filtering interferograms obtained from sar images acquired on the same area
CN103323830A (en) * 2013-05-20 2013-09-25 中国科学院电子学研究所 Three-element decomposition method and device based on polarization interference synthetic aperture radar
CN103675790A (en) * 2013-12-23 2014-03-26 中国国土资源航空物探遥感中心 Method for improving earth surface shape change monitoring precision of InSAR (Interferometric Synthetic Aperture Radar) technology based on high-precision DEM (Digital Elevation Model)
CN104459696A (en) * 2014-12-24 2015-03-25 中南大学 SAR interference baseline precise estimating method based on flat-earth phase
CN106772342A (en) * 2017-01-11 2017-05-31 西南石油大学 A kind of Timing Difference radar interference method suitable for big gradient surface subsidence monitoring
EP3229038A1 (en) * 2014-12-01 2017-10-11 Institute of Electronics, Chinese Academy of Sciences Wavelet domain insar interferometric phase filtering method in combination with local frequency estimation
CN107991676A (en) * 2017-12-01 2018-05-04 中国人民解放军国防科技大学 Troposphere error correction method of satellite-borne single-navigation-pass InSAR system
EP3349037A1 (en) * 2017-01-11 2018-07-18 Institute of Electronics, Chinese Academy of Sciences Method and device for imaging by bistatic synthetic aperture radar
CN108362200A (en) * 2018-02-24 2018-08-03 深圳市北斗智星勘测科技有限公司 A kind of method of quick update InSAR Deformation Series results
CN108761397A (en) * 2018-05-30 2018-11-06 中南大学 Polarization SAR model decomposition evaluation method based on electromagnetic scattering simulation
CN109254270A (en) * 2018-11-01 2019-01-22 西南交通大学 A kind of spaceborne X-band interfering synthetic aperture radar calibrating method
CN109375222A (en) * 2018-12-17 2019-02-22 中国国土资源航空物探遥感中心 A kind of synthetic aperture radar interferometry ionosphere phase estimation and compensation method
CN110058237A (en) * 2019-05-22 2019-07-26 中南大学 InSAR point Yun Ronghe and three-dimensional deformation monitoring method towards High-resolution SAR Images
CN110487241A (en) * 2019-08-15 2019-11-22 中国测绘科学研究院 Laser satellite surveys high extraction building area vertical control point method
CN110658521A (en) * 2019-10-16 2020-01-07 中国地质大学(北京) A GBInSAR atmospheric correction method and system based on winding phase

Patent Citations (21)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1998002761A1 (en) * 1996-07-11 1998-01-22 Science Applications International Corporation Terrain elevation measurement by interferometric synthetic aperture radar (ifsar)
WO2000054006A2 (en) * 1999-03-08 2000-09-14 Lockheed Martin Corporation Single-pass interferometric synthetic aperture radar
EP2017647A1 (en) * 2007-07-19 2009-01-21 Consiglio Nazionale delle Ricerche Method for processing data sensed by a synthetic aperture radar (SAR) and related remote sensing system
CN101339245A (en) * 2008-08-08 2009-01-07 西安电子科技大学 Multi-Baseline Interferometric Synthetic Aperture Radar Interferometric Phase Unwrapping Method
US20120019410A1 (en) * 2009-07-08 2012-01-26 Politecnico Di Milano Process for filtering interferograms obtained from sar images acquired on the same area
CN101609151A (en) * 2009-07-17 2009-12-23 重庆大学 A Moving Target Detection Method Based on Eigenvalue Decomposition of Single-Channel Synthetic Aperture Radar (SAR) Image Sequence
CN101706577A (en) * 2009-12-01 2010-05-12 中南大学 Method for monitoring roadbed subsidence of express way by InSAR
CN103323830A (en) * 2013-05-20 2013-09-25 中国科学院电子学研究所 Three-element decomposition method and device based on polarization interference synthetic aperture radar
CN103675790A (en) * 2013-12-23 2014-03-26 中国国土资源航空物探遥感中心 Method for improving earth surface shape change monitoring precision of InSAR (Interferometric Synthetic Aperture Radar) technology based on high-precision DEM (Digital Elevation Model)
EP3229038A1 (en) * 2014-12-01 2017-10-11 Institute of Electronics, Chinese Academy of Sciences Wavelet domain insar interferometric phase filtering method in combination with local frequency estimation
CN104459696A (en) * 2014-12-24 2015-03-25 中南大学 SAR interference baseline precise estimating method based on flat-earth phase
CN106772342A (en) * 2017-01-11 2017-05-31 西南石油大学 A kind of Timing Difference radar interference method suitable for big gradient surface subsidence monitoring
EP3349037A1 (en) * 2017-01-11 2018-07-18 Institute of Electronics, Chinese Academy of Sciences Method and device for imaging by bistatic synthetic aperture radar
CN107991676A (en) * 2017-12-01 2018-05-04 中国人民解放军国防科技大学 Troposphere error correction method of satellite-borne single-navigation-pass InSAR system
CN108362200A (en) * 2018-02-24 2018-08-03 深圳市北斗智星勘测科技有限公司 A kind of method of quick update InSAR Deformation Series results
CN108761397A (en) * 2018-05-30 2018-11-06 中南大学 Polarization SAR model decomposition evaluation method based on electromagnetic scattering simulation
CN109254270A (en) * 2018-11-01 2019-01-22 西南交通大学 A kind of spaceborne X-band interfering synthetic aperture radar calibrating method
CN109375222A (en) * 2018-12-17 2019-02-22 中国国土资源航空物探遥感中心 A kind of synthetic aperture radar interferometry ionosphere phase estimation and compensation method
CN110058237A (en) * 2019-05-22 2019-07-26 中南大学 InSAR point Yun Ronghe and three-dimensional deformation monitoring method towards High-resolution SAR Images
CN110487241A (en) * 2019-08-15 2019-11-22 中国测绘科学研究院 Laser satellite surveys high extraction building area vertical control point method
CN110658521A (en) * 2019-10-16 2020-01-07 中国地质大学(北京) A GBInSAR atmospheric correction method and system based on winding phase

Non-Patent Citations (7)

* Cited by examiner, † Cited by third party
Title
H. Q. FU, J. J. ZHU, C. C. WANG, R. ZHAO AND Q. H. XIE: "Underlying Topography Estimation Over Forest Areas Using Single-Baseline InSAR Data", 《IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING》 *
HAI QIANG FU;JIAN JUN ZHU;CHANG CHENG WANG;HUI QIANG WANG;RONG Z: "A Wavelet Decomposition and Polynomial Fitting-Based Method for the Estimation of Time-Varying Residual Motion Error in Airborne Interferometric SAR", 《IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING》 *
M. SHIRZAEI: "Topography correlated atmospheric delay correction in radar interferometry using wavelet transforms", 《GEOPHYSICAL RESEARCH LETTERS》 *
MARYAM RAHNEMOONFAR;BETH PLALE: "DEM Generation with SAR Interferometry Based on Weighted Wavelet Phase Unwrapping", 《2013 FOURTH INTERNATIONAL CONFERENCE ON COMPUTING FOR GEOSPATIAL RESEARCH AND APPLICATION》 *
焦明连: "《 合成孔径雷达干涉测量理论与应用》", 31 March 2009 *
胡波,朱建军,张长书: "InSAR提取DEM的原理与实践", 《测绘工程》 *
赵蓉;胡俊;章浙涛;占文俊;付海强: "多分辨率分析的干涉技术大气改正算法", 《测绘科学》 *

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN111833446A (en) * 2020-06-24 2020-10-27 浙江省测绘科学技术研究院 Overhead ground object rapid correction method based on characteristic line extraction
CN111812600A (en) * 2020-06-29 2020-10-23 中南林业科技大学 An Adaptive Terrain Dependent SRTM-DEM Correction Method
CN111812600B (en) * 2020-06-29 2023-09-08 中南林业科技大学 An adaptive terrain-related SRTM-DEM correction method
CN112816983A (en) * 2021-01-06 2021-05-18 中南大学 Time sequence InSAR turbulence atmospheric delay correction method based on optimized interferogram set
CN112816983B (en) * 2021-01-06 2023-09-19 中南大学 Time-series InSAR turbulent atmospheric delay correction method based on optimized interferometric atlas
CN116736306A (en) * 2023-08-15 2023-09-12 成都理工大学 Time sequence radar interference monitoring method based on third high-resolution
CN116736306B (en) * 2023-08-15 2023-10-24 成都理工大学 A time-series radar interference monitoring method based on Gaofen-3
CN117665809A (en) * 2023-12-21 2024-03-08 西南林业大学 Inversion method for forest canopy height
CN119828138A (en) * 2024-11-22 2025-04-15 武汉工程大学 Multi-baseline InSAR residual phase error correction method and system based on flat land priori information
CN119828138B (en) * 2024-11-22 2025-10-17 武汉工程大学 A multi-baseline InSAR residual phase error correction method and system based on flat ground prior information
CN119805416A (en) * 2024-12-13 2025-04-11 北京空间机电研究所 A method for correcting sea surface ranging errors using satellite-borne single-photon lidar

Also Published As

Publication number Publication date
CN111239736B (en) 2022-02-11

Similar Documents

Publication Publication Date Title
CN111239736A (en) Method, Apparatus, Equipment and Storage Medium for Surface Elevation Correction Based on Single Baseline
CN109633648B (en) Multi-baseline phase estimation device and method based on likelihood estimation
CN108594222B (en) Elevation reconstruction method and device for dual-frequency interference synthetic aperture radar
CN111273293A (en) InSAR residual motion error estimation method and device considering terrain fluctuation
KR101712084B1 (en) Method and Apparatus for Correcting Ionospheric Distortion based on multiple aperture interferometry
CN115060208A (en) Power transmission and transformation line geological disaster monitoring method and system based on multi-source satellite fusion
CN111856459B (en) An Improved DEM Maximum Likelihood Constrained Multibaseline InSAR Phase Unwrapping Method
CN112711021B (en) Multi-resolution InSAR (interferometric synthetic Aperture Radar) interactive interference time sequence analysis method
CN119780923B (en) Method, system, equipment and medium for extracting under-forest topography based on interferometric radar image
CN118244268A (en) DEM generation method, device, equipment and medium based on ICESat-2 corrected track error
CN119199850B (en) Method and device for measuring boundary of subsidence basin in coal mine goaf
CN110297243B (en) Phase Error Compensation Method and Device in Synthetic Aperture Radar Tomography 3D Imaging
CN112363165B (en) A method, device, equipment and medium for terrain inversion under forest
CN113341410B (en) A method, device, equipment and medium for estimating large-scale forest terrain
Yamashita et al. Mitigation of ionospheric noise in azimuth offset based on the split-spectrum method
CN112649807B (en) A method for removing airborne InSAR orbit errors based on wavelet multi-scale correlation analysis
CN115267779A (en) An InSAR Time Series DEM Error Estimation Method
CN109946682A (en) Baseline estimation method of GF3 data based on ICESat/GLAS
CN110297242A (en) Compressed sensing based synthetic aperture radar chromatography three-D imaging method and device
CN115616575B (en) Interference phase diagram winding method assisted by satellite-borne SAR (synthetic aperture radar) stereo measurement
CN119415833A (en) A multi-scale adaptive time-series InSAR surface deformation extraction method
CN118731945A (en) A method and device for monitoring landslide deformation by satellite-borne radar interference
CN117761716A (en) InSAR landslide deformation time series monitoring method and storage medium integrating CR and GNSS
CN111696207B (en) A Multi-Baseline DEM Fusion Method Based on Guided Filtering
Li et al. Atmospheric phase delay correction of D-InSAR based on Sentinel-1A

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant