CN116299464A - A high-speed and high-maneuvering wide-format sector-scanning SAR imaging method - Google Patents
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Abstract
Description
技术领域technical field
本发明属于SAR成像技术领域,具体涉及一种高速高机动宽幅扇扫SAR成像方法。The invention belongs to the technical field of SAR imaging, and in particular relates to a high-speed, high-mobility and wide-width sector-scanning SAR imaging method.
背景技术Background technique
高机动平台在成像制导过程中,需要进行宽测绘带成像以实现大范围目标搜索。由于传统的多普勒波束锐化(DBS)成像拼接方法存在比较明显的拼接痕迹,成像效果较差,扫描合成孔径雷达(Scan SAR)模式存在扇贝效应与信噪比不一致等问题,如今,宽测绘带成像逐渐向成像效果更优、波束移动更灵活的循序渐进扫描(TOPS)模式发展。During the imaging guidance process of high mobility platform, wide swath imaging is required to realize large-scale target search. Because the traditional Doppler Beam Sharpening (DBS) imaging stitching method has obvious stitching traces, the imaging effect is poor, and the Scanning Synthetic Aperture Radar (Scan SAR) mode has problems such as scalloping effect and inconsistent signal-to-noise ratio. Swath imaging is gradually developing towards the progressive scanning (TOPS) mode with better imaging effect and more flexible beam movement.
而在低成本、小型化平台中,往往采用调频连续波雷达。这种新体制雷达结构简单、峰值功率低、调频周期长,导致传统的脉冲体制雷达的成像模型与成像算法在调频连续波信号上失效。因此,面对低成本、小型化平台宽幅成像的需求,需要对循序渐进扫描模式与调频连续波雷达相结合的成像方法进行研究。In low-cost, miniaturized platforms, frequency-modulated continuous-wave radar is often used. This new system radar has simple structure, low peak power, and long frequency modulation cycle, which lead to the failure of the imaging model and imaging algorithm of the traditional pulse system radar on the frequency modulation continuous wave signal. Therefore, in the face of the demand for low-cost, miniaturized platform wide-format imaging, it is necessary to study the imaging method combining the progressive scanning mode and frequency-modulated continuous wave radar.
Guan Y等人在文献“Study on Full Aperture Imaging Algorithm forAirborneTOPS Mode[J]. IEEE Access, 2018:16305-16313.”中提出了一种机载正侧视构型下的改进频率变标算法,在方位聚焦过程中去除了由于波束扫描引起的方位时域混叠的现象。现有技术针对机载正侧视构型下的循序渐进扫描模式成像,这种技术无法应对大斜视构型下距离与方位信号的高度耦合现象与方位空变现象。现有技术主要面向机载正侧视的构型条件,信号耦合较小且耦合形式与大斜视条件不同,若忽视信号耦合,会导致信号无法聚焦;由于成像范围大,存在严重的方位空变问题,若忽视方位空变,会导致成像聚焦深度浅,无法实现全孔径成像。In the document "Study on Full Aperture Imaging Algorithm for AirborneTOPS Mode[J]. IEEE Access, 2018:16305-16313.", Guan Y et al. proposed an improved frequency scaling algorithm under the airborne side-view configuration. The azimuth-time-domain aliasing phenomenon caused by beam scanning is removed during the azimuth focusing process. The existing technology is aimed at the progressive scanning mode imaging under the airborne side-looking configuration, which cannot deal with the high coupling phenomenon of distance and azimuth signals and the azimuth spatial variation phenomenon under the high squint configuration. The existing technology is mainly oriented to the configuration conditions of the airborne front and side view. The signal coupling is small and the coupling form is different from the high squint condition. If the signal coupling is ignored, the signal will not be able to focus; due to the large imaging range, there is serious azimuth space variation The problem is that if the azimuth space variation is ignored, the depth of focus of the imaging will be shallow, and full-aperture imaging cannot be achieved.
发明内容Contents of the invention
为了解决现有技术中存在的上述问题,本发明提供了一种高速高机动宽幅扇扫SAR成像方法。本发明要解决的技术问题通过以下技术方案实现:In order to solve the above-mentioned problems existing in the prior art, the present invention provides a high-speed, high-mobility, wide-range sector-scanning SAR imaging method. The technical problem to be solved in the present invention is realized through the following technical solutions:
本发明提供了一种高速高机动宽幅扇扫SAR成像方法,包括:The present invention provides a high-speed and high-mobility wide-range sector-scanning SAR imaging method, comprising:
S1:获得解线频调处理后的回波信号并进行瞬时斜距泰勒展开,得到瞬时斜距泰勒展开后的回波信号;S1: Obtain the echo signal after delineation and frequency modulation processing and perform instantaneous slant distance Taylor expansion to obtain the echo signal after instantaneous slant distance Taylor expansion ;
S2:对所述瞬时斜距泰勒展开后的回波信号进行一次方位时变误差校正,得到校正后的信号/>;S2: the echo signal after Taylor expansion of the instantaneous slant distance Perform an azimuth time-varying error correction to obtain the corrected signal /> ;
S3:利用解旋转滤波器对所述信号进行处理,获得方位不模糊的信号;S3: Use the derotation filter to process the signal Process to obtain a signal with an unambiguous orientation ;
S4:对所述方位不模糊的信号进行方位傅里叶变换,得到方位傅里叶变换后的信号/>;S4: Unambiguous signal for said bearing Perform azimuth Fourier transform to obtain the signal after azimuth Fourier transform/> ;
S5:利用方位空变时移校正滤波器对所述方位傅里叶变换后的信号进行处理,获得处理后的信号/>;S5: Use the azimuth-space-varying time-shift correction filter to transform the azimuth Fourier-transformed signal Perform processing to obtain the processed signal /> ;
S6:对所述信号进行方位逆傅里叶变换,得到方位逆傅里叶变换后的信号/>;S6: on the signal Perform azimuth inverse Fourier transform to obtain the signal after azimuth inverse Fourier transform/> ;
S7:利用距离方位解耦合滤波器对所述方位逆傅里叶变换后的信号进行处理,得到距离方位解耦合后的信号/>;S7: Utilize the range and azimuth decoupling filter to inverse Fourier transform the azimuth signal Perform processing to obtain the decoupled signal of distance and azimuth/> ;
S8:对所述信号进行距离傅里叶变换,得到距离聚焦的信号;S8: To the signal Perform distance Fourier transform to obtain distance-focused signals ;
S9:消除所述信号中解线频调处理引入的参考斜距,获得信号;S9: Eliminate the signal The reference slant distance introduced by the mid-line frequency tone processing is obtained to obtain the signal ;
S10:将多普勒调频率空变误差校正滤波器与所述信号/>相乘以消除信号方位空变性对方位向聚焦的影响,获得信号/>;S10: Correct the Doppler modulation frequency space-variant error correction filter with the signal /> multiplied to eliminate the effect of signal azimuth spatial variability on azimuth focusing, to obtain the signal /> ;
S11:对所述信号进行方位傅里叶变换,得到方位傅里叶变换后的;S11: To the signal Perform azimuth Fourier transform to obtain the azimuth Fourier transformed ;
S12:利用多普勒时变误差滤波器对所述信号/>进行处理,得到信号/>;S12: Using Doppler time-varying error filter to the signal /> Process and get the signal /> ;
S13:对所述信号进行方位逆傅里叶变换,得到二维聚焦的信号,以实现成像。S13: To the signal Perform azimuth inverse Fourier transform to obtain a two-dimensional focused signal , to achieve imaging.
在本发明的一个实施例中,所述S2包括:In one embodiment of the present invention, said S2 includes:
S2.1:构造一次方位时变误差校正滤波器:S2.1: Construct an azimuth time-varying error correction filter :
, ,
其中,表示距离快时间,/>表示方位慢时间,/>表示目标斜距引起的时延与解线频调处理中参考斜距引起的时延的差,/>表示虚数单位,/>表示一次方位时变误差,/>表示SAR系统平台的速度,/>表示目标斜视角,/>表示发射信号载频,/>表示光速,/>表示发射信号调频率;in, Indicates distance and time, /> Indicates the azimuth slow time, /> Indicates the difference between the time delay caused by the target slant distance and the time delay caused by the reference slant distance in the delineation and tone processing, /> Indicates the imaginary unit, /> Indicates a time-varying error in azimuth, /> Indicates the speed of the SAR system platform, /> Indicates the oblique angle of the target, /> Indicates the carrier frequency of the transmitted signal, /> represents the speed of light, /> Indicates the modulation frequency of the transmitted signal;
S2.2:将所述回波信号与所述一次方位时变误差校正滤波器/>相乘,得到校正后的信号/>:S2.2: the echo signal with the primary azimuth time-varying error correction filter /> Multiply to get the corrected signal /> :
, ,
其中,表示距离时域信号中的距离窗函数,/>表示方位时域信号中的方位窗函数,/>表示在合成孔径积累时间中每个采样时刻的目标斜距与参考斜距之差。in, Represents the range window function in the range-time domain signal, /> Represents the azimuth window function in the azimuth time domain signal, /> Indicates the difference between the target slant distance and the reference slant distance at each sampling moment in the synthetic aperture accumulation time.
在本发明的一个实施例中,所述S3包括:In one embodiment of the present invention, said S3 includes:
S3.1:构建解旋转滤波器:S3.1: Construct the derotation filter :
, ,
其中,为旋转因子,/>表示波束斜视角的旋转角速度;in, is the rotation factor, /> Indicates the rotational angular velocity of the oblique angle of the beam;
S3.2:将所述信号与所述解旋转滤波器/>相乘,获得方位不模糊的信号/>。S3.2: Put the signal with the derotation filter /> Multiply to get a signal with unambiguous orientation /> .
在本发明的一个实施例中,所述S5包括:In one embodiment of the present invention, said S5 includes:
S5.1:构建方位空变时移校正滤波器:S5.1: Construct azimuth-space-varying time-shift correction filter :
, ,
其中,表示解线频调处理引入的参考斜距;in, Indicates the reference slant distance introduced by the delineation and tone processing;
S5.2:将所述方位傅里叶变换后的信号与所述方位空变时移校正滤波器/>相乘,得到消除方位时移空变的信号/>:S5.2: Fourier transform the azimuth signal with the azimuth-space-varying time-shift correction filter /> multiplied to obtain a signal that eliminates time-shift and space-variation in azimuth/> :
, ,
其中,表示方位频率,/>表示方位频域信号中的方位频率窗函数,/>表示方位频率频移,/>表示信号/>与方位空变时移校正滤波器/>相乘后再对方位频率进行泰勒展开时的第0阶系数,/>表示信号/>与方位空变时移校正滤波器/>相乘后再对方位频率进行泰勒展开时的第/>阶系数。in, Indicates the azimuth frequency, /> Represents the azimuth frequency window function in the azimuth frequency domain signal, /> Indicates the azimuth frequency shift, /> Indicates the signal /> with azimuth-space-variant time-shift correction filter /> The 0th order coefficient when multiplying and then performing Taylor expansion on the azimuth frequency, /> Indicates the signal /> with azimuth-space-variant time-shift correction filter /> After multiplying and then performing Taylor expansion on the azimuth frequency, the first /> order coefficient.
在本发明的一个实施例中,所述S7包括:In one embodiment of the present invention, said S7 includes:
S7.1:构建距离方位解耦合滤波器:S7.1: Construct the range-azimuth decoupling filter :
, ,
其中,表示信号/>中相位对距离快时间的i阶泰勒展开系数;in, Indicates the signal /> The i -order Taylor expansion coefficient of the middle phase versus the fast time of the distance;
S7.2:将所述距离方位解耦合滤波器与方位逆傅里叶变换后的信号相乘,得到距离方位解耦合后的信号/>。S7.2: Decoupling the range-azimuth filter and azimuth inverse Fourier transformed signal Multiply to get the decoupled signal in range and azimuth /> .
在本发明的一个实施例中,所述S9包括:In one embodiment of the present invention, said S9 includes:
S9.1:构建参考斜距消除滤波器:S9.1: Construct reference slope distance elimination filter :
其中,表示目标斜距;in, Indicates the target slope distance;
S9.2:将所述参考斜距消除滤波器与信号/>相乘,得到参考斜距消除后的信号/>。S9.2: The reference slope distance elimination filter with signal /> Multiply to get the signal after the reference slant distance is eliminated /> .
在本发明的一个实施例中,所述S10包括:In one embodiment of the present invention, said S10 includes:
S10.1:构造多普勒调频率空变误差校正滤波器:S10.1: Construct Doppler modulation frequency space-variant error correction filter :
, ,
其中,为方位调频率/>阶空变误差因子;in, Frequency modulation for azimuth /> order space-varying error factor;
S10.2:将所述多普勒调频率空变误差校正滤波器与所述信号/>相乘,得到信号/>。S10.2: Apply the Doppler modulation frequency space variation error correction filter with the signal /> Multiply to get the signal /> .
在本发明的一个实施例中,所述S12包括:In one embodiment of the present invention, said S12 includes:
S12.1:构造多普勒时变误差滤波器:S12.1: Construction of Doppler time-varying error filter :
, ,
其中,其中,为信号/>中相位对方位频率/>进行泰勒展开的第/>阶系数;where, where, for signal /> Medium phase to azimuth frequency/> The first /> of the Taylor expansion order coefficient;
S12.2:将所述多普勒时变误差滤波器与所述信号/>相乘,得到信号/>。S12.2: apply the Doppler time-varying error filter with the signal /> multiplied to get the signal /> .
本发明的另一方面提供了一种存储介质,所述存储介质中存储有计算机程序,所述计算机程序用于执行上述实施例中任一项所述高速高机动宽幅扇扫SAR成像方法的步骤。Another aspect of the present invention provides a storage medium, in which a computer program is stored, and the computer program is used to execute the high-speed, high-mobility, wide-format sector-scanning SAR imaging method described in any one of the above-mentioned embodiments. step.
本发明的另一方面提供了一种电子设备,包括存储器和处理器,所述存储器中存储有计算机程序,所述处理器调用所述存储器中的计算机程序时实现如上述实施例中任一项所述高速高机动宽幅扇扫SAR成像方法的步骤。Another aspect of the present invention provides an electronic device, including a memory and a processor, wherein a computer program is stored in the memory, and when the processor invokes the computer program in the memory, any one of the above-mentioned embodiments is implemented. Steps of the high-speed, high-mobility, wide-range sector-scanning SAR imaging method.
与现有技术相比,本发明的有益效果有:Compared with prior art, the beneficial effect of the present invention has:
1、本发明的高速高机动宽幅扇扫SAR成像方法针对高机动平台大斜视构型的距离方位信号耦合严重的问题,在消除信号的方位模糊后,构造距离方位解耦合滤波器,可以快速实现信号距离与方位解耦合。1. The high-speed, high-maneuverability and wide-range sector-scanning SAR imaging method of the present invention aims at the problem of serious coupling of range and azimuth signals in the high squint configuration of the high-mobility platform. Realize the decoupling of signal distance and azimuth.
2、本发明针对信号方位幅宽较大,存在严重方位空变的问题,引入时域多普勒调频率空变误差校正滤波器来消除方位空变,实现了信号方位向统一聚焦处理。2. Aiming at the problem of serious azimuth space variation due to the large signal azimuth width, the present invention introduces a time-domain Doppler frequency modulation frequency space variation error correction filter to eliminate azimuth space variation, and realizes unified focus processing of signal azimuth.
3、本发明通过方位空变时移校正与多普勒调频率空变误差校正滤波器的加入,实现了不用插值的快速高机动平台大斜视调频连续波的循序渐进扫描模式成像。3. Through the addition of azimuth space-variation time-shift correction and Doppler frequency modulation space-variation error correction filter, the present invention realizes step-by-step scanning mode imaging of high squint FM continuous wave of fast high maneuvering platform without interpolation.
以下将结合附图及实施例对本发明做进一步详细说明。The present invention will be described in further detail below in conjunction with the accompanying drawings and embodiments.
附图说明Description of drawings
图1是本发明实施例提供的一种高速高机动宽幅扇扫SAR成像方法的流程图;FIG. 1 is a flow chart of a high-speed, high-mobility, wide-range sector-scanning SAR imaging method provided by an embodiment of the present invention;
图2是本发明实施例提供的一种SAR成像构型图;FIG. 2 is a SAR imaging configuration diagram provided by an embodiment of the present invention;
图3是利用本发明方法对点目标进行仿真成像的点目标场景图;Fig. 3 is the point target scene figure that utilizes the method of the present invention to carry out simulation imaging to point target;
图4是利用本发明方法对点目标进行仿真成像的结果图;Fig. 4 is the result figure that utilizes the method of the present invention to carry out simulation imaging to point target;
图5a至图5c是利用本发明方法对点目标进行仿真成像后选取的点目标的等高线图;Fig. 5a to Fig. 5c are the contour maps of point targets selected after the point target is simulated and imaged by using the method of the present invention;
图6a至图6c是利用现有方法对点目标进行仿真成像后选取的点目标的等高线图。Figures 6a to 6c are contour maps of point targets selected after simulation imaging of point targets using existing methods.
具体实施方式Detailed ways
为了进一步阐述本发明为达成预定发明目的所采取的技术手段及功效,以下结合附图及具体实施方式,对依据本发明提出的高速高机动宽幅扇扫SAR成像进行详细说明。In order to further explain the technical means and effects adopted by the present invention to achieve the intended purpose of the invention, the high-speed and high-mobility wide-format sector-scan SAR imaging according to the present invention will be described in detail below in conjunction with the accompanying drawings and specific implementation methods.
有关本发明的前述及其他技术内容、特点及功效,在以下配合附图的具体实施方式详细说明中即可清楚地呈现。通过具体实施方式的说明,可对本发明为达成预定目的所采取的技术手段及功效进行更加深入且具体地了解,然而所附附图仅是提供参考与说明之用,并非用来对本发明的技术方案加以限制。The aforementioned and other technical contents, features and effects of the present invention can be clearly presented in the following detailed description of specific implementations with accompanying drawings. Through the description of specific embodiments, the technical means and effects of the present invention to achieve the intended purpose can be understood more deeply and specifically, but the accompanying drawings are only for reference and description, and are not used to explain the technical aspects of the present invention. program is limited.
应当说明的是,在本文中,诸如第一和第二等之类的关系术语仅仅用来将一个实体或者操作与另一个实体或操作区分开来,而不一定要求或者暗示这些实体或操作之间存在任何这种实际的关系或者顺序。而且,术语“包括”、“包含”或者任何其他变体意在涵盖非排他性的包含,从而使得包括一系列要素的物品或者设备不仅包括那些要素,而且还包括没有明确列出的其他要素。在没有更多限制的情况下,由语句“包括一个……”限定的要素,并不排除在包括所述要素的物品或者设备中还存在另外的相同要素。It should be noted that in this document, relational terms such as first and second etc. are only used to distinguish one entity or operation from another entity or operation, and do not necessarily require or imply that there is a relationship between these entities or operations. There is no such actual relationship or order between them. Furthermore, the terms "comprises", "comprises" or any other variation are intended to cover a non-exclusive inclusion such that an article or device comprising a set of elements includes not only those elements but also other elements not expressly listed. Without further limitations, an element defined by the phrase "comprising a" does not exclude the presence of additional identical elements in the article or device comprising said element.
请参见图1,图1是本发明实施例提供的一种高速高机动宽幅扇扫SAR(SyntheticAperture Radar,合成孔径雷达)成像方法的流程图。该方法包括:Please refer to FIG. 1 . FIG. 1 is a flow chart of a high-speed, high-mobility, wide-range sector-scanning SAR (Synthetic Aperture Radar, synthetic aperture radar) imaging method provided by an embodiment of the present invention. The method includes:
S1:获得解线频调处理后的回波信号并进行瞬时斜距泰勒展开,得到瞬时斜距泰勒展开后的回波信号:S1: Obtain the echo signal after delineation and frequency modulation processing and perform instantaneous slant distance Taylor expansion to obtain the echo signal after instantaneous slant distance Taylor expansion :
, ,
其中,表示距离快时间,/>表示方位慢时间,/>表示虚数单位,/>表示发射信号的电磁波波长,/>表示距离时域信号中的距离窗函数,表征距离信号接收时间范围,表示方位时域信号中的方位窗函数,表征方位信号接收时间范围,/>表示在合成孔径积累时间中每个采样的目标斜距与参考斜距之差,/>表示解线频调处理引入的参考斜距,/>表示目标斜距与解线频调处理中参考斜距引起的时延之差,/>表示光速,/>表示发射信号调频率。in, Indicates distance and time, /> Indicates the azimuth slow time, /> Indicates the imaginary unit, /> Indicates the wavelength of the electromagnetic wave of the transmitted signal, /> Represents the range window function in the range time domain signal, characterizing the range of the range signal receiving time, Represents the azimuth window function in the azimuth time domain signal, representing the time range of azimuth signal reception, /> Indicates the difference between the target slant distance and the reference slant distance for each sample in the synthetic aperture accumulation time, /> Indicates the reference slant distance introduced by delineating and tone processing, /> Indicates the difference between the target slant distance and the time delay caused by the reference slant distance in the delineation and tone processing, /> represents the speed of light, /> Indicates the modulation frequency of the transmitted signal.
S2:对瞬时斜距泰勒展开后的回波信号进行一次方位时变误差校正,得到校正后的信号/>。S2: The echo signal after Taylor expansion of the instantaneous slope distance Perform an azimuth time-varying error correction to obtain the corrected signal /> .
在本实施例中,一次方位时变误差校正滤波器的表达式为:In this embodiment, the primary azimuth time-varying error correction filter The expression is:
, ,
其中,表示目标斜距引起的时延与解线频调处理中参考斜距引起的时延的差,表示一次方位时变误差,/>表示SAR系统平台的速度,/>表示目标斜视角,表示发射信号载频。in, Indicates the difference between the time delay caused by the target slant distance and the time delay caused by the reference slant distance in the delineation and tone processing, Indicates a time-varying error in azimuth, /> Indicates the speed of the SAR system platform, /> Indicates the oblique angle of the target, Indicates the carrier frequency of the transmitted signal.
将回波信号与一次方位时变误差校正滤波器/>相乘,得到校正后的信号/>为:echo signal with an azimuth time-varying error correction filter /> Multiply to get the corrected signal /> for:
。 .
S3:利用解旋转滤波器对信号进行处理,获得方位不模糊的信号。S3: Use the derotation filter to transform the signal Process to obtain a signal with an unambiguous orientation .
由于信号存在方位模糊的现象,其信号多普勒频率变化规律与波束斜视角的旋转角速度相关,因此可以通过信号/>与解旋转滤波器/>相乘得到方位不模糊的信号/>。Due to the phenomenon of azimuth ambiguity in the signal, the Doppler frequency change law of the signal is related to the rotation angular velocity of the oblique angle of the beam. related, so can pass the signal /> with the derotation filter /> Multiply to get a signal with unambiguous orientation /> .
在本实施例中,解旋转滤波器的表达式为:In this embodiment, the derotation filter The expression is:
, ,
其中,为旋转因子,/>表示波束斜视角的旋转角速度。in, is the rotation factor, /> Indicates the rotational angular velocity of the oblique angle of the beam.
进一步地,得到的方位不模糊的信号的表达式为:Further, the obtained azimuth signal is not ambiguous The expression is:
。 .
S4:基于驻定相位原理与级数反演,对信号进行方位傅里叶变换,得到方位傅里叶变换后的信号/>:S4: Based on the principle of stationary phase and series inversion, the signal Perform azimuth Fourier transform to obtain the signal after azimuth Fourier transform/> :
, ,
其中,表示方位频率,/>表示方位频域信号中的方位频率窗函数,/>表示方位频率频移,/>表示信号/>经方位傅里叶变换后仅与距离快时间相关的相位,/>表示信号/>经方位傅里叶变换后距离与方位信号耦合部分对方位频率进行泰勒展开时的第/>阶系数。in, Indicates the azimuth frequency, /> Represents the azimuth frequency window function in the azimuth frequency domain signal, /> Indicates the azimuth frequency shift, /> Indicates the signal /> After the Fourier transform of the azimuth, the phase is only related to the fast time of the range, /> Indicates the signal /> After the azimuth Fourier transform, the coupling part of the distance and azimuth signal performs Taylor expansion on the azimuth frequency order coefficient.
S5:利用方位空变时移校正滤波器对方位傅里叶变换后的信号进行处理,获得消除方位时移空变后的信号/>。S5: Use the azimuth-space-variant time-shift correction filter to transform the azimuth Fourier-transformed signal Process to obtain the signal after eliminating the azimuth time-shift and space-variation/> .
具体地,为了消除距离徙动的方位空变性,构造方位空变时移校正滤波器,将其与方位傅里叶变换后的信号/>相乘,得到消除方位时移空变的信号。Specifically, in order to eliminate the azimuth-space variability of range migration, azimuth-space-variant time-shift correction filter is constructed , and compare it with the azimuth Fourier transformed signal /> Multiply, get the signal that eliminates the time-shift and space-variation of azimuth .
在本实施例中,方位空变时移校正滤波器的表达式为:In this embodiment, the azimuth-space-varying time-shift correction filter The expression is:
; ;
进一步地,得到的消除距离徙动的方位空变性后的信号表达式为:Further, the obtained signal after eliminating the azimuth spatial variability of the distance migration The expression is:
, ,
其中,表示方位频率,/>表示方位频域信号中的方位频率窗函数,/>表示方位频率频移,/>表示信号/>与方位空变时移校正滤波器/>相乘后再对方位频率进行泰勒展开时的第0阶系数,也就是常数项系数,/>表示信号/>与方位空变时移校正滤波器/>相乘后再对方位频率进行泰勒展开时的第/>阶系数。in, Indicates the azimuth frequency, /> Represents the azimuth frequency window function in the azimuth frequency domain signal, /> Indicates the azimuth frequency shift, /> Indicates the signal /> with azimuth-space-variant time-shift correction filter /> After multiplication, the coefficient of the 0th order when performing Taylor expansion on the azimuth frequency, that is, the coefficient of the constant term, /> Indicates the signal /> with azimuth-space-variant time-shift correction filter /> After multiplying and then performing Taylor expansion on the azimuth frequency, the first /> order coefficient.
S6:对信号进行方位逆傅里叶变换,得到方位逆傅里叶变换后的信号:S6: pair signal Perform azimuth inverse Fourier transform to obtain the signal after azimuth inverse Fourier transform :
, ,
其中,表示目标斜距,/>为信号/>中的/>进行方位逆傅里叶变换并对方位时间/>进行泰勒展开后得到的第i阶系数。in, Indicates the target slope distance, /> for signal /> in /> Perform azimuth inverse Fourier transform and compare azimuth time /> The i-th order coefficient obtained after Taylor expansion.
S7:利用距离方位解耦合滤波器对方位逆傅里叶变换后的信号进行处理,得到距离方位解耦合后的信号/>。S7: Utilize the distance and azimuth decoupling filter to inverse Fourier transform the signal of azimuth Perform processing to obtain the decoupled signal of distance and azimuth/> .
具体地,构造距离方位解耦合滤波器,并将其与信号/>相乘,得到距离与方位信号解耦合后的信号/>。在本实施例中,该距离方位解耦合滤波器/>的表达式为:Specifically, construct the range-azimuth decoupling filter , and combine it with the signal /> Multiply to get the signal after decoupling the distance and azimuth signals /> . In this embodiment, the range-azimuth decoupling filter /> The expression is:
, ,
其中,表示/>中/>部分对距离快时间的i阶泰勒展开系数;in, means /> Medium /> Part of the i -order Taylor expansion coefficient for distance and fast time;
得到的距离方位解耦合后的信号表达式为:The obtained range and azimuth decoupled signal The expression is:
, ,
其中,为/>对距离快时间进行傅里叶变换的零阶项。in, for /> The zero-order term of the Fourier transform of the range-fast time.
S8:对信号进行距离傅里叶变换,得到距离聚焦的信号/>:S8: pair signal Perform distance Fourier transform to obtain distance-focused signal/> :
, ,
其中,表示距离频率,/>为/>中与距离快时间无关的常数项。in, Indicates the distance frequency, /> for /> A constant term in which is independent of distance and time.
S9:消除信号中解线频调处理引入的参考斜距,获得信号。S9: Eliminate the signal The reference slant distance introduced by the mid-line frequency tone processing is obtained to obtain the signal .
具体地,消除信号中解线频调处理引入的/>项,构建参考斜距消除滤波器/>,将其与信号/>相乘,得到信号/>。Specifically, eliminating the signal The /> introduced by neutral line tone processing item, constructing the reference slant distance cancellation filter /> , compare it with the signal /> Multiply to get the signal /> .
在本实施例中,参考斜距消除滤波器的表达式为:In this embodiment, the reference slope distance elimination filter The expression is:
。 .
得到的信号的表达式为:get the signal The expression is:
, ,
其中,为参考斜距消除滤波器/>中方位慢时间第/>阶系数。in, for the reference slope distance removal filter /> Middle position slow time No. /> order coefficient.
S10:将多普勒调频率空变误差校正滤波器与所述信号/>相乘以消除信号方位空变性对方位向聚焦的影响,获得信号/>。S10: Correct the Doppler modulation frequency space-variant error correction filter with the signal /> multiplied to eliminate the effect of signal azimuth spatial variability on azimuth focusing, to obtain the signal /> .
为消除信号方位空变性对方位向聚焦的影响,引入一个多普勒调频率空变误差校正滤波器,将该多普勒调频率空变误差校正滤波器/>与信号/>相乘,得到信号/>。在本实施例中,多普勒调频率空变误差校正滤波器/>的表达式为:In order to eliminate the influence of signal azimuth space variation on azimuth focusing, a Doppler modulation frequency space variation error correction filter is introduced , the Doppler modulation frequency space-variant error correction filter /> with signal /> Multiply to get the signal /> . In this embodiment, the Doppler modulation frequency space variation error correction filter /> The expression is:
, ,
其中,为方位调频率/>阶空变误差因子。in, Frequency modulation for azimuth /> order space-varying error factor.
得到的信号的表达式为:get the signal The expression is:
。 .
S11:对信号进行方位傅里叶变换,得到方位傅里叶变换后的:S11: pair signal Perform azimuth Fourier transform to obtain the azimuth Fourier transformed :
, ,
其中,为剩余常数相位,不影响成像效果,/>表示经过距离徙动校正后方位信号中斜距的表现形式,与目标斜距的关系为/>;/>为/>中的部分利用驻定相位原理进行方位傅里叶变换后的相位对/>进行泰勒展开的第/>阶系数。in, is the remaining constant phase, which does not affect the imaging effect, /> Indicates the expression form of the slant distance in the azimuth signal after distance migration correction, and the relationship with the target slant distance is /> ;/> for /> middle The phase pair after partial Fourier transform of azimuth using the principle of stationary phase /> The first /> of the Taylor expansion order coefficient.
S12:将信号与多普勒时变误差滤波器/>进行相乘,得到信号。S12: put the signal with Doppler time-varying error filter /> Multiply to get the signal .
在本实施例中,所述多普勒时变误差滤波器的表达式为:In this embodiment, the Doppler time-varying error filter The expression is:
, ,
得到的信号的表达式为:get the signal The expression is:
。 .
S13:对信号进行方位逆傅里叶变换,得到二维聚焦的信号,以实现成像,其中,二维聚焦的信号/>的表达式为:S13: pair signal Perform azimuth inverse Fourier transform to obtain a two-dimensional focused signal , to achieve imaging where the two-dimensionally focused signal/> The expression is:
。 .
本发明提出的高速高机动宽幅扇扫SAR成像方法的效果可以通过下述仿真实验得到进一步说明。The effect of the high-speed, high-mobility, wide-range sector-scanning SAR imaging method proposed by the present invention can be further illustrated through the following simulation experiments.
(一)仿真条件(1) Simulation conditions
请参见图2,图2是本发明实施例提供的一种SAR成像构型图。首先,以合成孔径中心时刻平台所在位置在地面的投影为原点O,平台运动速度方向在地面的投影为轴,从原点指向合成孔径中心时刻平台所在位置为/>轴,通过右手系确定/>轴建立坐标系。此时,平台以速度/>沿/>轴方向进行运动,波束的斜视角/>以角速度/>匀速转动,使得波束中心从变化到了/>的位置,得到了一个扇形区域。Please refer to FIG. 2 . FIG. 2 is a SAR imaging configuration diagram provided by an embodiment of the present invention. Firstly, taking the projection of the platform’s position on the ground at the center of the synthetic aperture as the origin O, the projection of the platform’s motion velocity direction on the ground is axis, pointing from the origin to the center of the synthetic aperture, the position of the platform is /> Axis, determined by right-hand system /> Axes create a coordinate system. At this time, the platform at speed /> along /> Axis movement, oblique angle of the beam /> at angular velocity /> Rotate at a constant speed so that the center of the beam moves from The change has arrived /> position, a fan-shaped area is obtained.
设调频连续波雷达系统的信号载频为35GHz,脉冲重复频率为4KHz,沿曲线轨迹运动。FMCW(调频连续波) SAR的场景布点示意图如图3所示,从图3中可以看出,成像域初始布点为3×7矩形点阵,均匀分布在场景中。Assume that the signal carrier frequency of the frequency modulation continuous wave radar system is 35GHz, the pulse repetition frequency is 4KHz, and it moves along the curved track. The schematic diagram of the scene layout of FMCW (frequency modulated continuous wave) SAR is shown in Figure 3. From Figure 3, it can be seen that the initial layout of the imaging domain is a 3×7 rectangular lattice, which is evenly distributed in the scene.
(二)仿真内容(2) Simulation content
在上述条件下,用本发明的高速高机动宽幅扇扫SAR成像方法对上述目标场景进行仿真,得到成像结果,如图4所示,其中,左图为本发明所提方法的全孔径成像结果斜距图,可以看出图像点成三行七列的分布,中心目标点成像清晰、聚焦效果良好,不同方位向的目标点成像效果与中心点十分相似,验证了本发明方法可以解决大斜视宽幅条件下全孔径信号存在较大方位空变难以实现成像的问题。右图为通过几何校正后的成像结果图,可以看出校正后目标点排列与图3仿真场景中目标点的排列方式一致,成像位置正确。Under the above-mentioned conditions, the above-mentioned target scene is simulated by using the high-speed, high-mobility, wide-range sector-scan SAR imaging method of the present invention, and the imaging result is obtained, as shown in Figure 4, wherein the left figure is the full-aperture imaging of the method proposed by the present invention As a result, it can be seen from the slant distance map that the image points are distributed in three rows and seven columns, the central target point has clear imaging, and the focusing effect is good. The imaging effects of target points in different azimuths are very similar to the central point. There is a problem that the full-aperture signal has a large azimuth space variation and it is difficult to achieve imaging under the condition of wide squint. The image on the right is the imaging result after geometric correction. It can be seen that the arrangement of the target points after correction is consistent with the arrangement of the target points in the simulation scene in Figure 3, and the imaging position is correct.
进一步地,选取成像场景中的边缘点1和21及中心点11,进行插值放大绘制等高线图,请参见图5a至图5c,图5a至图5c是利用本发明方法对点目标进行仿真成像后选取的点目标的等高线图,其中,图5a为边缘点1的等高线图,图5b为中心点11的等高线图,图5c为边缘点21的等高线图。本发明仿真处理的各目标点,由于考虑了高机动平台场景幅宽过大带来的空变影响,因此其场景边缘点1和21及场景中心点11均呈现出良好聚焦效果,聚焦深度良好。Further, select the edge points 1 and 21 and the
进一步地,请参见图6a和图6c,图6a和图6c是利用现有方法(文献“Study on FullAperture Imaging Algorithm for Airborne TOPS Mode”中所述方法)对点目标进行仿真成像后选取的点目标的等高线图,其中,图6a为边缘点1的等高线图,图6b为中心点11的等高线图,图6c为边缘点21的等高线图。Further, please refer to Fig. 6a and Fig. 6c. Fig. 6a and Fig. 6c are the point targets selected after the simulation imaging of the point target using the existing method (the method described in the document "Study on FullAperture Imaging Algorithm for Airborne TOPS Mode") , wherein, Fig. 6a is a contour map of
本发明实施例的方法实现了高机动平台大前斜TOPS SAR模式成像,相比于所述现有方法,针对高机动平台大前斜成像构型分析回波信号特性,提升了方位聚焦深度,提升了边缘点成像质量。其对比结果为:两种方法对于空变较小区域均能实现良好成像,如目标点11的等高线图所示。但是,本发明方法目标点1与21聚焦效果良好,剖面图中主瓣与旁瓣形状规则,聚焦效果良好,对比方法中方位空变较大的目标点1与21由于存在方位空变误差,剖面图形状不规则,边缘点成像质量差。The method of the embodiment of the present invention realizes the TOPS SAR mode imaging of the high maneuvering platform with a large forward slope. Compared with the existing method, the characteristics of the echo signal are analyzed for the imaging configuration of the high maneuverable platform with a large forward slope, and the azimuth focus depth is improved. Improved edge point imaging quality. The results of the comparison are: both methods can achieve good imaging for the area with small spatial variation, as shown in the contour map of the
本发明的高速高机动宽幅扇扫SAR成像方法针对高机动平台大斜视构型的距离徙动校正,在消除信号的方位模糊后,构造徙动空变校正滤波器与距离徙动滤波器,可以快速实现信号距离与方位解耦合。本发明针对信号方位幅宽较大,存在严重的方位空变问题,引入时域扰动因子消除方位空变,实现了信号在方位进行统一聚焦处理。本发明通过距离徙动空变校正与方位时域扰动函数的加入,实现了不用插值的快速高机动平台大斜视调频连续波的TOPS模式成像。The high-speed, high-mobility, wide-range sector-scanning SAR imaging method of the present invention is aimed at the range migration correction of the high-mobility platform's large squint configuration. After eliminating the azimuth ambiguity of the signal, a space-variant correction filter and a range migration filter are constructed. The decoupling of signal distance and azimuth can be quickly realized. Aiming at the problem of serious azimuth space variation due to the large azimuth width of the signal, the present invention introduces a time domain disturbance factor to eliminate the azimuth space variation, and realizes unified focus processing of the signal in azimuth. The invention realizes the TOPS mode imaging of high squint FM continuous wave of fast high maneuvering platform without interpolation by adding distance migration space variation correction and azimuth time domain disturbance function.
综上,本发明针对调频连续波体制分析了高机动平台场景下距离与方位信号的耦合与回波信号方位空变情况,实现了对场景目标点的精确聚焦,并通过仿真验证了本发明的准确性和有效性。To sum up, the present invention analyzes the coupling of distance and azimuth signals and the spatial variation of echo signal azimuth in high maneuvering platform scenarios for the FM continuous wave system, realizes precise focusing on the target points of the scene, and verifies the advantages of the present invention through simulation. Accuracy and Validity.
本发明的又一实施例提供了一种存储介质,所述存储介质中存储有计算机程序,所述计算机程序用于执行上述实施例中所述高速高机动宽幅扇扫SAR成像方法的步骤。本发明的再一方面提供了一种电子设备,包括存储器和处理器,所述存储器中存储有计算机程序,所述处理器调用所述存储器中的计算机程序时实现如上述实施例所述高速高机动宽幅扇扫SAR成像方法的步骤。具体地,上述以软件功能模块的形式实现的集成的模块,可以存储在一个计算机可读取存储介质中。上述软件功能模块存储在一个存储介质中,包括若干指令用以使得一台电子设备(可以是个人计算机,服务器,或者网络设备等)或处理器(processor)执行本发明各个实施例所述方法的部分步骤。而前述的存储介质包括:U盘、移动硬盘、只读存储器(Read-Only Memory,ROM)、随机存取存储器(Random Access Memory,RAM)、磁碟或者光盘等各种可以存储程序代码的介质。Another embodiment of the present invention provides a storage medium, in which a computer program is stored, and the computer program is used to execute the steps of the high-speed, high-mobility, wide-field sector-scan SAR imaging method described in the above-mentioned embodiments. Another aspect of the present invention provides an electronic device, including a memory and a processor, the memory stores a computer program, and when the processor invokes the computer program in the memory, the high-speed and high-speed Steps of the imaging method of the maneuverable wide-field sector-scanning SAR. Specifically, the above-mentioned integrated modules implemented in the form of software function modules may be stored in a computer-readable storage medium. The above-mentioned software function modules are stored in a storage medium, and include several instructions to make an electronic device (which may be a personal computer, server, or network device, etc.) or a processor (processor) execute the methods described in various embodiments of the present invention. partial steps. The aforementioned storage medium includes: U disk, mobile hard disk, read-only memory (Read-Only Memory, ROM), random access memory (Random Access Memory, RAM), magnetic disk or optical disk and other various media that can store program codes. .
以上内容是结合具体的优选实施方式对本发明所作的进一步详细说明,不能认定本发明的具体实施只局限于这些说明。对于本发明所属技术领域的普通技术人员来说,在不脱离本发明构思的前提下,还可以做出若干简单推演或替换,都应当视为属于本发明的保护范围。The above content is a further detailed description of the present invention in conjunction with specific preferred embodiments, and it cannot be assumed that the specific implementation of the present invention is limited to these descriptions. For those of ordinary skill in the technical field of the present invention, without departing from the concept of the present invention, some simple deduction or replacement can be made, which should be regarded as belonging to the protection scope of the present invention.
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Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117348011A (en) * | 2023-09-26 | 2024-01-05 | 宁波大学 | A method to quickly correct the SAR radial flow velocity inversion of the sea surface flow field |
CN117665817A (en) * | 2024-02-01 | 2024-03-08 | 西安电子科技大学 | A complete bistatic forward-looking SAR high-resolution imaging method that can be processed in real time |
RU2819757C1 (en) * | 2023-11-20 | 2024-05-23 | Виталий Сергеевич Грибков | Method of obtaining two-dimensional radar image of object during multifrequency pulsed probing, which enables to recover amplitude and phase of reflected signal |
Citations (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2007017536A (en) * | 2005-07-05 | 2007-01-25 | Ricoh Co Ltd | Projector apparatus |
US7277042B1 (en) * | 2006-05-12 | 2007-10-02 | Raytheon Company | Compensation of flight path deviation for spotlight SAR |
JP2012215568A (en) * | 2011-03-31 | 2012-11-08 | Mitsubishi Electric Research Laboratories Inc | High resolution sar imaging using non-uniform pulse timing |
CN103605131A (en) * | 2013-12-04 | 2014-02-26 | 西安电子科技大学 | High-resolution DBS imaging method based on multiple united wave positions |
CN103901428A (en) * | 2014-03-28 | 2014-07-02 | 西安电子科技大学 | Missile-borne SAR sub-aperture forward squint high-order nonlinear chirp scaling imaging method |
KR20150055812A (en) * | 2013-11-14 | 2015-05-22 | 한국항공우주연구원 | Method for sar processing |
EP3012658A1 (en) * | 2014-10-21 | 2016-04-27 | Institute of Electronics, Chinese Academy of Sciences | Method and device for implementing sar imaging |
CN106291556A (en) * | 2016-08-29 | 2017-01-04 | 西北工业大学 | A kind of high squint SAR imaging algorithm based on hyperbolic model |
CN106950567A (en) * | 2017-03-30 | 2017-07-14 | 中国人民解放军国防科学技术大学 | Ultra wide band based on high-order sub-aperture CS slides poly- SAR image processing methods |
CN114839626A (en) * | 2021-11-01 | 2022-08-02 | 北京遥测技术研究所 | Track association method based on linear multi-target method |
CN115291212A (en) * | 2022-08-02 | 2022-11-04 | 西安电子科技大学 | Space variable nonlinear track expansion mapping high-resolution imaging method |
-
2023
- 2023-05-17 CN CN202310555848.XA patent/CN116299464B/en active Active
Patent Citations (11)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2007017536A (en) * | 2005-07-05 | 2007-01-25 | Ricoh Co Ltd | Projector apparatus |
US7277042B1 (en) * | 2006-05-12 | 2007-10-02 | Raytheon Company | Compensation of flight path deviation for spotlight SAR |
JP2012215568A (en) * | 2011-03-31 | 2012-11-08 | Mitsubishi Electric Research Laboratories Inc | High resolution sar imaging using non-uniform pulse timing |
KR20150055812A (en) * | 2013-11-14 | 2015-05-22 | 한국항공우주연구원 | Method for sar processing |
CN103605131A (en) * | 2013-12-04 | 2014-02-26 | 西安电子科技大学 | High-resolution DBS imaging method based on multiple united wave positions |
CN103901428A (en) * | 2014-03-28 | 2014-07-02 | 西安电子科技大学 | Missile-borne SAR sub-aperture forward squint high-order nonlinear chirp scaling imaging method |
EP3012658A1 (en) * | 2014-10-21 | 2016-04-27 | Institute of Electronics, Chinese Academy of Sciences | Method and device for implementing sar imaging |
CN106291556A (en) * | 2016-08-29 | 2017-01-04 | 西北工业大学 | A kind of high squint SAR imaging algorithm based on hyperbolic model |
CN106950567A (en) * | 2017-03-30 | 2017-07-14 | 中国人民解放军国防科学技术大学 | Ultra wide band based on high-order sub-aperture CS slides poly- SAR image processing methods |
CN114839626A (en) * | 2021-11-01 | 2022-08-02 | 北京遥测技术研究所 | Track association method based on linear multi-target method |
CN115291212A (en) * | 2022-08-02 | 2022-11-04 | 西安电子科技大学 | Space variable nonlinear track expansion mapping high-resolution imaging method |
Non-Patent Citations (2)
Title |
---|
ZIQIANGMENG等: "MIMO-Based Forward-Looking SAR Imaging Algorithm and Simulation", INTERNATIONAL JOURNAL OF ANTENNAS AND PROPAGATION, pages 1 - 10 * |
李亚超等: "弹载雷达成像技术发展现状与趋势", 雷达学报, vol. 11, no. 6, pages 943 - 978 * |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117348011A (en) * | 2023-09-26 | 2024-01-05 | 宁波大学 | A method to quickly correct the SAR radial flow velocity inversion of the sea surface flow field |
RU2819757C1 (en) * | 2023-11-20 | 2024-05-23 | Виталий Сергеевич Грибков | Method of obtaining two-dimensional radar image of object during multifrequency pulsed probing, which enables to recover amplitude and phase of reflected signal |
CN117665817A (en) * | 2024-02-01 | 2024-03-08 | 西安电子科技大学 | A complete bistatic forward-looking SAR high-resolution imaging method that can be processed in real time |
CN117665817B (en) * | 2024-02-01 | 2024-04-30 | 西安电子科技大学 | Complete real-time processable bistatic forward-looking SAR high-resolution imaging method |
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