CN102253377A - Target detection method for polarimetric interferometry synthetic aperture radar on basis of eigenvalue analysis - Google Patents
Target detection method for polarimetric interferometry synthetic aperture radar on basis of eigenvalue analysis Download PDFInfo
- Publication number
- CN102253377A CN102253377A CN201110102633XA CN201110102633A CN102253377A CN 102253377 A CN102253377 A CN 102253377A CN 201110102633X A CN201110102633X A CN 201110102633XA CN 201110102633 A CN201110102633 A CN 201110102633A CN 102253377 A CN102253377 A CN 102253377A
- Authority
- CN
- China
- Prior art keywords
- rightarrow
- coherence
- polarization
- matrix
- omega
- 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
Links
Images
Abstract
The invention discloses a target detection method for a polarimetric interferometry synthetic aperture radar on the basis of eigenvalue analysis, relating to a target detection method for a polarimetric interferometry synthetic aperture radar so as to solve the problem that a ground object can not be detected and identified through the traditional complete polarization and the single polarization synthetic aperture radars under the background of the stronger natural ground object clutter. The target detection method comprises the following steps of: reading in the data of a polarimetric interferometry synthetic aperture radar image according to an image data format; preprocessing the polarimetric interferometry synthetic aperture radar image; obtaining a simplified polarimetric interferometry matrix by two groups of polarized scattering vectors, and solving the characteristic value of a matrix; simplifying the matrix by similar diagonalization and a Jordan standard form to obtain an optimized scattering vector-based correlation coefficient; analyzing an eigenvalue and the statics characteristic of the correlation coefficient by selecting different samples; and constructing a target detector by the obtained statics characteristic to detect an interested target to obtain a result. The target detection method is used for the target detection for the polarimetric interferometry synthetic aperture radar.
Description
Technical field
The present invention relates to a kind of polarization interference synthetic aperture radar object detection method, belong to the remote sensing technology field.
Background technology
Synthetic-aperture radar as a kind of unique can round-the-clock, the remote sensing means of round-the-clock earth observation imaging, has irreplaceable effect in this field, and polarization interference synthetic aperture radar (PolInSAR) can combine the careful geometric configuration of atural object, structure, sensing and material composition and coherence, elevation information such as (sea level elevations), greatly promoted synthetic-aperture radar and extracted and the ability of analyzing characters of ground object, had broad application prospects in the remote sensing field.
The economic develop rapidly of China at present, urbanization process is constantly accelerated, and researching and analysing of mushroom town and combination area of city and country area better is familiar with development of urbanization trend with the help people, provides effective guidance for formulating further development plan.Therefore utilize synthetic-aperture radar to carry out cities and towns zone terrain analysis and have using value and wide application prospect by force with assessment.Tradition complete polarization and single polarization synthetic-aperture radar can realize classification and the identification to some basic atural objects, but can't solve the detection and the identification of man-made target under the strong natural feature on a map clutter background.
Summary of the invention
The purpose of this invention is to provide a kind of polarization interference synthetic aperture radar object detection method, can't realize the detection of man-made target under the strong natural feature on a map clutter background and the problem of identification to solve traditional complete polarization and single polarization synthetic-aperture radar based on Eigenvalue Analysis.
The present invention addresses the above problem the technical scheme of taking to be:
Polarization interference synthetic aperture radar object detection method based on Eigenvalue Analysis of the present invention, described method is realized by following steps:
Step 1: obtain pending view data by polarization interference synthetic aperture radar system acquisition image, read in the data of polarization interference synthetic aperture radar image according to image data format;
Step 2: image pre-service: the polarization interference synthetic aperture radar image that step 1 is read in carries out filtering, registration pre-service, obtains the Polarization scattering vector;
Step 3: the eigenwert and the Jordan standard form of the Polarization scattering vector computational short cut polarization interference coherence matrix that obtains according to step 2, calculating is based on the coefficient of coherence of Eigenvalue Analysis, three kinds of different atural object eigenwerts in zone, cities and towns and coefficient of coherence statistical property are carried out statistical study, and concrete steps are as follows:
Step 3 A: simplify the calculating of polarization interference coherence matrix:
Formula two
Wherein, [Ω
12] for simplifying the polarization interference coherence matrix;
(i=1,2) are Polarization scattering vector under the Pauli base; S
Pq(p, { h v}) is scattering amplitude to q ∈, and expression receives with q polarized state emission, p polarized state after the target of electromagnetic wave gained to multiple scattering coefficient, and h is a horizontal polarization state, and v is the vertical polarization state; The conjugate transpose of superscript H representing matrix; The transposition of superscript T representing matrix; Superscript * represents conjugation;
Step 3 B: the simplification polarization interference coherence matrix that step 3 A is calculated carries out characteristic value decomposition, and similar diagonalization obtains eigenwert and based on the optimization coefficient of coherence of Eigenvalue Analysis;
Step 3 C: choose the three kinds of different ground object sample of typical case in cities and towns: forest, farmland, buildings, with described three kinds of different ground object sample as detecting target, according to eigenwert and optimization coefficient of coherence that step 3 B obtains the eigenwert of described three kinds of different ground object sample and the statistical property of coefficient of coherence are analyzed, and then obtained being used for the result of feature extraction and target detection;
Step 4: the result who is used for feature extraction and target detection that step 3 C is obtained carries out the object detector design, is used for the polarization interference synthetic aperture radar image, obtains the man-made target testing result.
The invention has the beneficial effects as follows: the defective that 1, the invention solves polarimetric synthetic aperture radar man-made target feature extraction difficulty under the strong clutter background, and proposed to simplify the notion of polarization interference coherence matrix, utilize the eigenwert of this matrix and corresponding coefficient of coherence to distinguish the differently statistics difference on the thing feature of zone, cities and towns, and then the design object detecting device is realized the detection and the identification of man-made target under the strong natural feature on a map clutter background.2, the present invention assesses the cost less with respect to other polarization interference synthetic aperture radar analysis of image data methods, and can make full use of the atural object geometric properties, the information that does not comprise in single polarizations such as coherence, the polarimetric synthetic aperture radar image realizes that man-made target interested detects under the strong clutter background.
Description of drawings
Fig. 1 is the amplitude picture of polarization interference synthetic aperture radar image hh (horizontal polarization emission level polarized state receives the SAR image that obtains) passage; Fig. 2 a is a buildings Sample selection synoptic diagram; Fig. 2 b is a farmland Sample selection synoptic diagram; Fig. 2 c is a forest Sample selection synoptic diagram; Fig. 3 is buildings, the farmland distribution plan (among the figure, △ represents buildings, and represents the farmland) on the eigenwert plane; Fig. 4 is three kinds of different ground object sample coefficient of coherence distribution probability density maps (among the figure solid line represent buildings, dotted line represent that forest, dot-and-dash line represent the farmland); Fig. 5 is testing result figure of the present invention.
Embodiment
Embodiment one: the polarization interference synthetic aperture radar object detection method based on Eigenvalue Analysis of present embodiment, described method is realized by following steps:
Step 1: obtain pending view data by polarization interference synthetic aperture radar system acquisition image, read in the data (the hh channel image as shown in Figure 1) of polarization interference synthetic aperture radar image according to image data format;
Step 2: image pre-service: the polarization interference synthetic aperture radar image that step 1 is read in carries out filtering, registration pre-service, obtains the Polarization scattering vector;
Step 3: the eigenwert of the Polarization scattering vector computational short cut polarization interference coherence matrix that obtains according to step 2 and Jordan standard form are (referring to " matrix analysis study course " 68 pages, the Dong Zengfu chief editor, publishing house of Harbin Institute of Technology in April, 2005 second edition), calculating is based on the coefficient of coherence of Eigenvalue Analysis, three kinds of different atural object eigenwerts in zone, cities and towns and coefficient of coherence statistical property are carried out statistical study, and concrete steps are as follows:
Step 3 A: simplify the calculating of polarization interference coherence matrix:
Formula two
Wherein, [Ω
12] for simplifying the polarization interference coherence matrix;
(i=1,2) be Pauli (referring to Cloude S.R.and Papathanassiou K.P., Polarimetric SAR interferometry, IEEE Trans.on GRS, 1998,36 (5), 1551-1565) the following Polarization scattering vector of base; S
Pq(P, { h v}) is scattering amplitude to q ∈, and expression receives with q polarized state emission, p polarized state after the target of electromagnetic wave gained to multiple scattering coefficient, and h is a horizontal polarization state, and v is the vertical polarization state; The conjugate transpose of superscript H representing matrix; The transposition of superscript T representing matrix; Superscript * represents conjugation;
Step 3 B: the simplification polarization interference coherence matrix that step 3 A is calculated carries out characteristic value decomposition, and similar diagonalization obtains eigenwert and based on the optimization coefficient of coherence of Eigenvalue Analysis;
Step 3 C: choose the three kinds of different ground object sample of typical case in cities and towns: forest, farmland, buildings, with described three kinds of different ground object sample as detecting target, according to eigenwert and optimization coefficient of coherence that step 3 B obtains the eigenwert of described three kinds of different ground object sample and the statistical property of coefficient of coherence are analyzed, and then obtained being used for the result of feature extraction and target detection;
Step 4: the result who is used for feature extraction and target detection that step 3 C is obtained carries out the object detector design, is used for the polarization interference synthetic aperture radar image, obtains the man-made target testing result.
As shown in Figures 3 and 4, utilize eigenwert and linear restriction condition to remove the farmland clutter, utilize a coefficient of coherence and a constant thresholding to remove the forest clutter, testing result as shown in Figure 5.
Embodiment two: among the step 3 B of present embodiment, describedly carry out characteristic value decomposition to simplifying the polarization interference coherence matrix, similar diagonalization, obtain eigenwert and based on the optimization coefficient of coherence of eigenwert, concrete eigenwert, optimize that coefficient of coherence calculates and the similar diagonalization technical process of matrix is as follows:
The eigenwert of a matrix can comprehensively, accurately characterize the characteristic of matrix, is the important means and the instrument of matrix analysis, therefore finds the solution simplification polarization interference coherence matrix eigenwert and is used for extracting and analyzing based on the characters of ground object of simplifying the polarization interference coherence matrix; Simplifying the polarization interference coherence matrix is 3 * 3 complex matrix, can calculate its three complex eigenvalues and three corresponding multiple eigenvectors;
Can notice that off-diagonal element is the tolerance of different polarization interchannel signal coherency in the formula two, the coherence of obviously different polarization interchannel signals plays the effect of decoherence to the signal of equipolarization state.Therefore, only needing utilization to make off-diagonal element someway is the zero relevant optimization that can realize the equipolarization status signal.Certain this imagination can realize with the method for Eigenvalue Analysis equally;
If simplifying the polarization interference coherence matrix is simple matrix, can carry out similar diagonalization, utilize following formula three~12 to obtain described optimization coefficient of coherence:
[Ω
12]=[E]
-1[Λ] [E] formula three
Wherein: [Ω
12] for simplifying the polarization interference coherence matrix; The conjugate transpose of superscript H representing matrix;
(i=1,2) are Polarization scattering vector under the Pauli base;
(i=1,2) are the Scattering of Vector under the new scattering mechanism;
By the proper vector of simplifying the polarization interference coherence matrix
Constitute; [Λ]=diag (λ
1, λ
2, λ
3), by the eigenvalue of simplifying the polarization interference coherence matrix
1, λ
2, λ
3Constitute; [E]
H[E]
-1Column vector can be counted as three groups of Polarization scattering mechanism, that is,
So
Wherein:
[E]
H[E]
-1Column vector
I=1,2; J=1,2,3 are counted as three groups of Polarization scattering mechanism; The conjugate transpose of superscript H representing matrix;
Be Polarization scattering vector under the Pauli base; μ
Ij(i=1,2; J=1,2,3) be the projection value of Scattering of Vector i on the j scattering mechanism, scattering mechanism is by [E]
H[E]
-1Column vector determine;
(i=1,2) are the Scattering of Vector under the new scattering mechanism;
Under these three groups of Polarization scattering mechanism, coherences between different polarization channel signals are inhibited and decoherence between the equipolarization channel signal is minimized, the coherence is optimized, utilize following formula 11 and 12 to calculate three and optimize coefficient of coherence, and be used from polarization interference synthetic aperture radar analysis of image data and feature extraction with simplification polarization interference coherence matrix one;
Wherein, μ
Ij(i=1,2; J=1,2,3) be the projection value of Scattering of Vector i on the j scattering mechanism, scattering mechanism is by [E]
H[E]
-1Column vector determine;
I=1,2,3 is three pairs of optimization coefficient of coherence under the scattering mechanism;
(i=1,2) are the Scattering of Vector under the new scattering mechanism; The transposition of superscript T representing matrix;
If simplify the condition (under a few cases) that the polarization interference coherence matrix does not satisfy simple matrix, utilize the Jordan standard form to come the approximate similarity diagonalization, utilize formula six, four, five and seven~12 to obtain described optimization coefficient of coherence again:
[Ω
12]=[P]
-1[J] [P] formula six
Wherein: [Ω
12] for simplifying the polarization interference coherence matrix; [J] is [Ω
12] the Jordan standard form, [J] diagonal entry is [Ω
12] eigenwert, [J] off diagonal element except that the minor diagonal adjacent with diagonal line is zero, is similar diagonalizable a kind of approximate; [P] is the similarity transformation matrix.Other method step is identical with embodiment one.
Embodiment three: among the step 3 C of present embodiment, the eigenwert and the optimization coefficient of coherence that obtain according to step 3 B are analyzed as follows the eigenwert of three kinds of selected different ground object sample and the statistical property of coefficient of coherence:
Eigenwert with above-mentioned three kinds of different ground object sample is coordinate constitutive characteristic space or plane, add up the distribution situation of above-mentioned three kinds of different atural object sample points on feature space or plane, analyze the separability of above-mentioned three kinds of samples in feature space or plane, statistics is drawn three coefficient of coherence distribution probability density maps of three kinds of different ground object sample respectively, analyze the difference of three kinds of samples on this coefficient of coherence probability density figure by described three coefficient of coherence distribution probability density maps, utilize above-mentioned analysis means to analyze the difference of described three kinds of different atural objects, and then obtain being used for feature extraction and (promptly add up the distribution situation of eigenwert on characteristic plane and the distribution situation of coefficient of coherence of above-mentioned three kinds of different atural objects with the result of target detection, therefrom analyze the difference of described three kinds of different atural objects, and then be used for feature extraction and target detection).Other method step is identical with embodiment one.
Embodiment four: in the step 4 of present embodiment, the method for designing of described object detector is as follows:
The result who is used for feature extraction and target detection who obtains according to step 3 C is to determine the judgement plane on the feature space that constitutes of coordinate axis in eigenwert; Utilize three coefficient of coherence distribution probability density map setting thresholds of three kinds of different ground object sample, comprehensive above two kinds of methods realize target detection.Other method step is identical with embodiment one, two or three.
Present embodiment is an example with Fig. 3, Fig. 4, the linear judgment condition that is provided with on the characteristic plane that first and second eigenwert constitutes is as shown in Figure 3, Figure 4 removed the farmland, first coefficient of coherence is provided with the constant thresholding filtering forest about 1, realizes the detection of building target.Judgment condition in the practical application and thresholding should be set flexibly according to the statistical property that step 3 C obtains.
Embodiment five: among the step 3 A of present embodiment, the proposition of described simplification polarization interference coherence matrix (formula two) notion; Specifically describe as follows:
Conventional polar interference synthetic aperture radar image coherence's tolerance adopts the polarization interference coherence matrix, promptly
[T
6] be one 2 * 2 partitioned matrix (polarization interference coherence matrix), by three 3 * 3 complex matrix [T
11], [T
22] and [Ω
12] constitute, comprised the polarization information and the interference information of two width of cloth interference complex pattern simultaneously; Wherein, [T
11], [T
22] and [Ω
12] be defined as respectively
Obviously [T
11] and [T
22] only comprise the polarization information of two radars, and interfere irrelevantly, in the polarization interference data analysis a kind of data redundancy, therefore, definition [Ω
12] (Simplified Polarimetric Interferometric Coherency Matrix SPICM) is in order to simplify the polarization interference coherence matrix
Formula two
Each element of being simplified the polarization interference coherence matrix by formula two as can be seen is the tolerance of coherence between the different polarization of polarization interference synthetic aperture radar two antennas channel signal, comprises the required enough polarization interference information of data analysis.
Claims (4)
1. polarization interference synthetic aperture radar object detection method based on Eigenvalue Analysis, it is characterized in that: described method is realized by following steps:
Step 1: obtain pending view data by polarization interference synthetic aperture radar system acquisition image, read in the data of polarization interference synthetic aperture radar image according to image data format;
Step 2: image pre-service: the polarization interference synthetic aperture radar image that step 1 is read in carries out filtering, registration pre-service, obtains the Polarization scattering vector;
Step 3: the eigenwert and the Jordan standard form of the Polarization scattering vector computational short cut polarization interference coherence matrix that obtains according to step 2, calculating is based on the coefficient of coherence of Eigenvalue Analysis, three kinds of different atural object eigenwerts in zone, cities and towns and coefficient of coherence statistical property are carried out statistical study, and concrete steps are as follows:
Step 3 A: simplify the calculating of polarization interference coherence matrix:
Formula two
Wherein, [Ω
12] for simplifying the polarization interference coherence matrix;
(i=1,2) are Polarization scattering vector under the Pauli base; S
Pq(p, { h v}) is scattering amplitude to q ∈, and expression receives with q polarized state emission, p polarized state after the target of electromagnetic wave gained to multiple scattering coefficient, and h is a horizontal polarization state, and v is the vertical polarization state; The conjugate transpose of superscript H representing matrix; The transposition of superscript T representing matrix; Superscript * represents conjugation;
Step 3 B: the simplification polarization interference coherence matrix that step 3 A is calculated carries out characteristic value decomposition, and similar diagonalization obtains eigenwert and based on the optimization coefficient of coherence of Eigenvalue Analysis;
Step 3 C: choose the three kinds of different ground object sample of typical case in cities and towns: forest, farmland, buildings, with described three kinds of different ground object sample as detecting target, according to eigenwert and optimization coefficient of coherence that step 3 B obtains the eigenwert of described three kinds of different ground object sample and the statistical property of coefficient of coherence are analyzed, and then obtained being used for the result of feature extraction and target detection;
Step 4: the result who is used for feature extraction and target detection that step 3 C is obtained carries out the object detector design, is used for the polarization interference synthetic aperture radar image, obtains the man-made target testing result.
2. the polarization interference synthetic aperture radar object detection method based on Eigenvalue Analysis according to claim 1, it is characterized in that: among the step 3 B, describedly carry out characteristic value decomposition to simplifying the polarization interference coherence matrix, similar diagonalization, obtain eigenwert and based on the optimization coefficient of coherence of eigenwert, concrete eigenwert, optimize that coefficient of coherence calculates and the similar diagonalization technical process of matrix is as follows:
If simplifying the polarization interference coherence matrix is simple matrix, can carry out similar diagonalization, utilize following formula three~12 to obtain described optimization coefficient of coherence:
[Ω
12]=[E]
-1[Λ] [E] formula three
Wherein: [Ω
12] for simplifying the polarization interference coherence matrix; The conjugate transpose of superscript H representing matrix;
(i=1,2) are Polarization scattering vector under the Pauli base;
(i=1,2) are the Scattering of Vector under the new scattering mechanism;
By the proper vector of simplifying the polarization interference coherence matrix
Constitute; [Λ]=diag (λ
1, λ
2, λ
3), by the eigenvalue of simplifying the polarization interference coherence matrix
1, λ
2, λ
3Constitute; [E]
H[E]
-1Column vector can be counted as three groups of Polarization scattering mechanism, that is,
So
Wherein:
[E]
H[E]
-1Column vector
I=1,2; J=1,2,3 are counted as three groups of Polarization scattering mechanism; The conjugate transpose of superscript H representing matrix;
(i=1,2) are Polarization scattering vector under the Pauli base; μ
Ij(i=1,2; J=1,2,3) be the projection value of Scattering of Vector i on the j scattering mechanism, scattering mechanism is by [E]
H[E]
-1Column vector determine;
(i=1,2) are the Scattering of Vector under the new scattering mechanism;
Under these three groups of Polarization scattering mechanism, coherences between different polarization channel signals are inhibited and decoherence between the equipolarization channel signal is minimized, the coherence is optimized, utilize following formula 11 and 12 to calculate three and optimize coefficient of coherence, and be used from polarization interference synthetic aperture radar analysis of image data and feature extraction with simplification polarization interference coherence matrix one;
Wherein, μ
Ij(i=1,2; J=1,2,3) be the projection value of Scattering of Vector i on the j scattering mechanism, scattering mechanism is by [E]
H[E]
-1Column vector determine;
I=1,2,3 is three pairs of optimization coefficient of coherence under the scattering mechanism;
(i=1,2) are the Scattering of Vector under the new scattering mechanism; The transposition of superscript T representing matrix;
If simplify the condition that the polarization interference coherence matrix does not satisfy simple matrix, utilize the Jordan standard form to come the approximate similarity diagonalization, utilize formula six, four, five and seven~12 to obtain described optimization coefficient of coherence again:
[Ω
12]=[P]
-1[J] [P] formula six
Wherein: [Ω
12] for simplifying the polarization interference coherence matrix; [J] is [Ω
12] the Jordan standard form, [J] diagonal entry is [Ω
12] eigenwert, [J] off diagonal element except that the minor diagonal adjacent with diagonal line is zero, is similar diagonalizable a kind of approximate; [P] is the similarity transformation matrix.
3. the polarization interference synthetic aperture radar object detection method based on Eigenvalue Analysis according to claim 1, it is characterized in that: among the step 3 C, the eigenwert and the optimization coefficient of coherence that obtain according to step 3 B are analyzed as follows the eigenwert of three kinds of selected different ground object sample and the statistical property of coefficient of coherence:
Eigenwert with above-mentioned three kinds of different ground object sample is coordinate constitutive characteristic space or plane, add up the distribution situation of above-mentioned three kinds of different atural object sample points on feature space or plane, analyze the separability of above-mentioned three kinds of samples in feature space or plane, statistics is drawn three coefficient of coherence distribution probability density maps of three kinds of different ground object sample respectively, analyze the difference of three kinds of samples on this coefficient of coherence probability density figure by described three coefficient of coherence distribution probability density maps, utilize above-mentioned analysis means to analyze the difference of described three kinds of different atural objects, and then obtain being used for the result of feature extraction and target detection.Other method step is identical with embodiment one.
4. according to claim 1,2 or 3 described polarization interference synthetic aperture radar object detection methods based on Eigenvalue Analysis, it is characterized in that: in the step 4, the method for designing of described object detector is as follows:
The result who is used for feature extraction and target detection who obtains according to step 3 C is to determine the judgement plane on the feature space that constitutes of coordinate axis in eigenwert; Utilize three coefficient of coherence distribution probability density map setting thresholds of three kinds of different ground object sample, comprehensive above two kinds of methods realize target detection.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201110102633XA CN102253377B (en) | 2011-04-22 | 2011-04-22 | Target detection method for polarimetric interferometry synthetic aperture radar on basis of eigenvalue analysis |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201110102633XA CN102253377B (en) | 2011-04-22 | 2011-04-22 | Target detection method for polarimetric interferometry synthetic aperture radar on basis of eigenvalue analysis |
Publications (2)
Publication Number | Publication Date |
---|---|
CN102253377A true CN102253377A (en) | 2011-11-23 |
CN102253377B CN102253377B (en) | 2012-11-21 |
Family
ID=44980743
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201110102633XA Expired - Fee Related CN102253377B (en) | 2011-04-22 | 2011-04-22 | Target detection method for polarimetric interferometry synthetic aperture radar on basis of eigenvalue analysis |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN102253377B (en) |
Cited By (12)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103197304A (en) * | 2013-04-19 | 2013-07-10 | 哈尔滨工业大学 | PolSAR image double-layer target decomposition method based on nonreflecting symmetric scattering component extraction |
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 |
CN104360331A (en) * | 2014-12-11 | 2015-02-18 | 南京长峰航天电子科技有限公司 | Simulation method of polarization characteristics of broadband radar target |
CN104991241A (en) * | 2015-06-30 | 2015-10-21 | 西安电子科技大学 | Target signal extraction and super-resolution enhancement processing method in strong clutter condition |
CN106338775A (en) * | 2016-09-07 | 2017-01-18 | 民政部国家减灾中心(民政部卫星减灾应用中心) | Building damage degree evaluation method based on interference synthetic aperture radar data |
CN106772371A (en) * | 2016-11-21 | 2017-05-31 | 上海卫星工程研究所 | Polarimetric calibration parameter requirements analysis method based on polarimetric SAR interferometry classification application |
CN107121673A (en) * | 2017-04-17 | 2017-09-01 | 北京环境特性研究所 | Background clutter extracting method based on complete polarization technology |
CN107144842A (en) * | 2017-06-27 | 2017-09-08 | 哈尔滨工业大学 | A kind of improved polarimetric SAR interferometry vegetation height joint inversion method |
CN107167806A (en) * | 2017-05-22 | 2017-09-15 | 中国人民解放军国防科学技术大学 | Polarimetric synthetic aperture radar ShipTargets detection method based on depression filtering |
CN109754004A (en) * | 2018-12-25 | 2019-05-14 | 中国科学院国家空间科学中心 | A kind of antithesis G4U goal decomposition method of polarimetric SAR image |
CN112630741A (en) * | 2020-12-11 | 2021-04-09 | 江西师范大学 | Full-polarization synthetic aperture radar image target compensation PEOC method |
CN113643284A (en) * | 2021-09-09 | 2021-11-12 | 西南交通大学 | Polarimetric synthetic aperture radar image ship detection method based on convolutional neural network |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
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 |
CN101369019A (en) * | 2008-10-10 | 2009-02-18 | 清华大学 | Polarization interference synthetic aperture radar three-dimensional imaging method based on polarization data amalgamation |
CN101419284A (en) * | 2008-08-08 | 2009-04-29 | 哈尔滨工业大学 | Method for obtaining artificial target information from target parametric inversion model under forest cover |
CN101685155A (en) * | 2008-09-27 | 2010-03-31 | 中国科学院电子学研究所 | Method of optimizing interference coefficient of coherence on the basis of polarimetric synthetic aperture radar (SAR) |
-
2011
- 2011-04-22 CN CN201110102633XA patent/CN102253377B/en not_active Expired - Fee Related
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
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 |
CN101419284A (en) * | 2008-08-08 | 2009-04-29 | 哈尔滨工业大学 | Method for obtaining artificial target information from target parametric inversion model under forest cover |
CN101685155A (en) * | 2008-09-27 | 2010-03-31 | 中国科学院电子学研究所 | Method of optimizing interference coefficient of coherence on the basis of polarimetric synthetic aperture radar (SAR) |
CN101369019A (en) * | 2008-10-10 | 2009-02-18 | 清华大学 | Polarization interference synthetic aperture radar three-dimensional imaging method based on polarization data amalgamation |
Non-Patent Citations (4)
Title |
---|
张腊梅: "极化SAR图像人造目标特征提取与检测方法研究", 《中国博士学位论文全文数据库信息科技辑 I136-110》, 15 April 2011 (2011-04-15) * |
裴彩红: "基于目标分解和SVM的POL-SAR图像分类方法研究", 《中国优秀硕士学位论文全文数据库信息科技辑 I136-350》, 15 February 2009 (2009-02-15) * |
邹斌等: "PolSAR图像信息提取技术及应用的发展", 《遥感技术与应用》, vol. 24, no. 3, 30 June 2009 (2009-06-30) * |
邹斌等: "极化干涉合成孔径雷达图像信息提取技术的进展及未来", 《电子与信息学报》, vol. 28, no. 10, 31 October 2006 (2006-10-31) * |
Cited By (18)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN103197304B (en) * | 2013-04-19 | 2014-12-24 | 哈尔滨工业大学 | PolSAR image double-layer target decomposition method based on nonreflecting symmetric scattering component extraction |
CN103197304A (en) * | 2013-04-19 | 2013-07-10 | 哈尔滨工业大学 | PolSAR image double-layer target decomposition method based on nonreflecting symmetric scattering component extraction |
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 |
CN103323830B (en) * | 2013-05-20 | 2016-03-09 | 中国科学院电子学研究所 | Based on three element decomposition method and devices of polarization interference synthetic aperture radar |
CN104360331A (en) * | 2014-12-11 | 2015-02-18 | 南京长峰航天电子科技有限公司 | Simulation method of polarization characteristics of broadband radar target |
CN104991241A (en) * | 2015-06-30 | 2015-10-21 | 西安电子科技大学 | Target signal extraction and super-resolution enhancement processing method in strong clutter condition |
CN106338775B (en) * | 2016-09-07 | 2018-07-10 | 民政部国家减灾中心(民政部卫星减灾应用中心) | Building based on interference of data of synthetic aperture radar falls to damage degree assessment method |
CN106338775A (en) * | 2016-09-07 | 2017-01-18 | 民政部国家减灾中心(民政部卫星减灾应用中心) | Building damage degree evaluation method based on interference synthetic aperture radar data |
CN106772371A (en) * | 2016-11-21 | 2017-05-31 | 上海卫星工程研究所 | Polarimetric calibration parameter requirements analysis method based on polarimetric SAR interferometry classification application |
CN107121673A (en) * | 2017-04-17 | 2017-09-01 | 北京环境特性研究所 | Background clutter extracting method based on complete polarization technology |
CN107167806A (en) * | 2017-05-22 | 2017-09-15 | 中国人民解放军国防科学技术大学 | Polarimetric synthetic aperture radar ShipTargets detection method based on depression filtering |
CN107144842A (en) * | 2017-06-27 | 2017-09-08 | 哈尔滨工业大学 | A kind of improved polarimetric SAR interferometry vegetation height joint inversion method |
CN109754004A (en) * | 2018-12-25 | 2019-05-14 | 中国科学院国家空间科学中心 | A kind of antithesis G4U goal decomposition method of polarimetric SAR image |
CN109754004B (en) * | 2018-12-25 | 2020-10-23 | 中国科学院国家空间科学中心 | Dual G4U target decomposition method for polarized SAR image |
CN112630741A (en) * | 2020-12-11 | 2021-04-09 | 江西师范大学 | Full-polarization synthetic aperture radar image target compensation PEOC method |
CN112630741B (en) * | 2020-12-11 | 2023-04-14 | 江西师范大学 | Full-polarization synthetic aperture radar image target compensation PEOC method |
CN113643284A (en) * | 2021-09-09 | 2021-11-12 | 西南交通大学 | Polarimetric synthetic aperture radar image ship detection method based on convolutional neural network |
CN113643284B (en) * | 2021-09-09 | 2023-08-15 | 西南交通大学 | Polarized synthetic aperture radar image ship detection method based on convolutional neural network |
Also Published As
Publication number | Publication date |
---|---|
CN102253377B (en) | 2012-11-21 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN102253377B (en) | Target detection method for polarimetric interferometry synthetic aperture radar on basis of eigenvalue analysis | |
Park et al. | Polarimetric SAR remote sensing of the 2011 Tohoku earthquake using ALOS/PALSAR | |
CN104376330B (en) | Polarimetric SAR Image Ship Target Detection method based on super-pixel scattering mechanism | |
US10107904B2 (en) | Method and apparatus for mapping and characterizing sea ice from airborne simultaneous dual frequency interferometric synthetic aperture radar (IFSAR) measurements | |
Li et al. | A new approach to collapsed building extraction using RADARSAT-2 polarimetric SAR imagery | |
CN102629378B (en) | Remote sensing image change detection method based on multi-feature fusion | |
CN104698460A (en) | Ocean wind-field retrieval method of double-frequency coplanar synthetic aperture radar (SAR) | |
CN103226826B (en) | Based on the method for detecting change of remote sensing image of local entropy visual attention model | |
CN105335975B (en) | Polarization SAR image segmentation method based on low-rank decomposition and statistics with histogram | |
CN105321163A (en) | Method and apparatus for detecting variation region of fully polarimetric SAR (Synthetic Aperture Radar) image | |
CN102540157A (en) | Ground feature classifying method based on simplified polarization synthetic aperture radar data | |
Ramirez Jr et al. | Machine learning for seismic signal processing: Phase classification on a manifold | |
Liao et al. | Urban change detection based on coherence and intensity characteristics of SAR imagery | |
CN104166128A (en) | Multi-pass SAR coherent change detection method based on general likelihood ratio | |
CN103870842B (en) | Polarized SAR image classification method combining polarization feature and watershed | |
Li et al. | Enhanced automatic root recognition and localization in GPR images through a YOLOv4-based deep learning approach | |
CN104424373A (en) | Elaborate expression method for space variable correlation | |
Costantini et al. | Enhanced PSP SAR interferometry for analysis of weak scatterers and high definition monitoring of deformations over structures and natural terrains | |
Adriano et al. | Extraction of damaged areas due to the 2013 Haiyan typhoon using ASTER data | |
Guo et al. | Study of detecting method with advanced airborne and spaceborne synthetic aperture radar data for collapsed urban buildings from the Wenchuan earthquake | |
Thapa et al. | Monitoring land encroachment and land use & land cover (LULC) change in the Pachhua Dun, Dehradun District using landsat images 1989 and 2020 | |
Preiss et al. | Polarimetric SAR coherent change detection | |
He et al. | An improved method for phase triangulation algorithm based on the coherence matrix eigen-decomposition in time-series SAR interferometry | |
Lu et al. | Urban expansion detection with SPOT5 panchromatic images using textural features and PCA | |
Zhu et al. | Identification for building surface material based on hyperspectral remote sensing |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant | ||
C17 | Cessation of patent right | ||
CF01 | Termination of patent right due to non-payment of annual fee |
Granted publication date: 20121121 Termination date: 20130422 |