CN105589071B - Airborne radar high-resolution DBS imaging methods based on SPICE - Google Patents
Airborne radar high-resolution DBS imaging methods based on SPICE Download PDFInfo
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Abstract
Description
技术领域technical field
本发明属于雷达技术领域,特别涉及一种基于稀疏迭代协方差矩阵估计(Sparseiterative covariance-based estimation,SPICE)的机载雷达高分辨DBS成像方法,可用于在机载雷达发射脉冲数较少的情况下,获得较高的图像分辨率。The invention belongs to the field of radar technology, in particular to a high-resolution DBS imaging method for airborne radar based on Sparseiterative covariance-based estimation (SPICE), which can be used when the number of pulses transmitted by airborne radar is small , to obtain a higher image resolution.
背景技术Background technique
多普勒波束锐化(Doppler beam sharpening,DBS)成像是将雷达波束进行大范围扫描的一种非聚焦成像技术,一般在正侧视的情况下对观测区域进行成像。DBS成像技术虽然不像合成孔径雷达成像技术那样具有很高的横向分辨率,但是DBS成像的运算复杂度较低,并且其相对于实波束的横向分辨能力有了实质性的提高,可以在较短的时间内完成对大范围场景的成像。Doppler beam sharpening (DBS) imaging is a non-focused imaging technology that scans the radar beam in a large area, and generally images the observation area under the condition of frontal side view. Although DBS imaging technology does not have high lateral resolution like synthetic aperture radar imaging technology, the computational complexity of DBS imaging is low, and its lateral resolution ability has been substantially improved compared with real beams, which can be used in relatively Complete imaging of a wide range of scenes in a short period of time.
在雷达发射脉冲数充足的情况下,传统的基于傅里叶变换的DBS成像技术可以获得较高的图像分辨率。然而在实际情况中,雷达的发射脉冲数往往会受到各种因素的限制,例如,雷达波束扫描的范围、雷达扫描的重访时间等。当雷达发射脉冲数较多时,会导致观测场景范围的缩小,并延长雷达扫描的重访时间,在一定程度上影响了雷达对观测场景的实时监控;当减少雷达发射脉冲数时,虽然可以提高雷达对观测场景的重访率,但是,由于相干积累时间不足,导致DBS图像的分辨率严重下降。因此,通常满足图像分辨率要求的前提下,尽量提高雷达对观测场景的重访时间。而且传统的基于傅里叶变换的DBS成像技术,往往会导致信号能量的泄露,使得DBS图像的清晰度下降,并会对信号能量功率的估值过高。The traditional DBS imaging technology based on Fourier transform can obtain higher image resolution when the number of radar transmission pulses is sufficient. However, in actual situations, the number of radar transmission pulses is often limited by various factors, such as the range of radar beam scanning, the revisit time of radar scanning, and so on. When the number of pulses emitted by the radar is large, it will reduce the scope of the observation scene and prolong the revisit time of the radar scan, which affects the real-time monitoring of the observation scene by the radar to a certain extent; when the number of pulses emitted by the radar is reduced, although it can improve The radar revisited the observed scene, but the resolution of the DBS image was severely degraded due to insufficient coherent accumulation time. Therefore, under the premise of meeting the image resolution requirements, the revisit time of the radar observation scene should be increased as much as possible. Moreover, the traditional DBS imaging technology based on Fourier transform often leads to the leakage of signal energy, which reduces the definition of DBS images and overestimates the signal energy power.
发明内容Contents of the invention
针对上述现有技术的不足,本发明的目的在于提出一种基于SPICE的机载雷达高分辨DBS成像方法,该方法根据脉压处理后的回波信号建立地杂波回波信号的信号模型,并给出求解地杂波回波信号的功率值的优化模型,获得所有距离门的功率矩阵,即为最终的机载雷达回波数据矩阵,将其由载机坐标系转换至大地坐标系,得到最终的DBS图像。For above-mentioned deficiencies in the prior art, the object of the present invention is to propose a kind of airborne radar high-resolution DBS imaging method based on SPICE, this method sets up the signal model of ground clutter echo signal according to the echo signal after pulse pressure processing, And the optimization model for solving the power value of the ground clutter echo signal is given, and the power matrix of all range gates is obtained, which is the final airborne radar echo data matrix, which is converted from the aircraft coordinate system to the earth coordinate system, Get the final DBS image.
为了实现上述技术目的,本发明采用如下技术方案予以实现。In order to achieve the above-mentioned technical purpose, the present invention adopts the following technical solutions to achieve.
一种基于SPICE的机载雷达高分辨DBS成像方法,其特征在于,包括以下步骤:A kind of airborne radar high resolution DBS imaging method based on SPICE, is characterized in that, comprises the following steps:
步骤1,设定机载雷达接收的回波信号为 为第i个距离门的回波信号;在载机为参考原点的载机坐标系中,对机载雷达接收的回波信号在距离维进行脉冲压缩处理,得到脉压处理后的回波信号y,y=[y1,...,yi,...,yM],yi为脉压后的第i个距离门的回波信号;根据脉压后的第i个距离门的回波信号yi建立第i个距离门的地杂波回波信号xi的信号模型;其中,脉压后的第i个距离门的回波信号yi的维数为N×1,N为机载雷达发射的脉冲数,i=1,2,...,M,M为距离门个数;Step 1, set the echo signal received by the airborne radar as is the echo signal of the i-th range gate; in the aircraft coordinate system where the aircraft is the reference origin, the echo signal received by the airborne radar Perform pulse compression processing in the distance dimension to obtain the echo signal y after pulse pressure processing, y=[y 1 ,...,y i ,...,y M ], y i is the ith echo signal after pulse pressure The echo signal of the range gate; according to the echo signal y i of the i-th range gate after the pulse pressure, the signal model of the ground clutter echo signal x i of the i-th range gate is established; wherein, the i-th range gate after the pulse pressure The dimensionality of the echo signal y i of a range gate is N * 1, and N is the pulse number of airborne radar transmission, and i=1, 2,..., M, M is the number of range gates;
步骤2,求取脉压后的第i个距离门的回波信号yi的协方差矩阵Ri;Step 2, obtain the covariance matrix R i of the echo signal y i of the i-th range gate after the pulse pressure;
步骤3,根据脉压后的第i个距离门的回波信号yi的协方差矩阵Ri,给出求解第i个距离门的地杂波回波信号xi的功率值的优化模型:求解第i个距离门的地杂波回波信号xi的功率值的优化模型:得到第i个距离门的地杂波回波信号xi的第k个功率值pi,k;其中,k=1,2,...,2N,N为多普勒通道数,表示求F范数的平方,上标H表示共轭转置;Step 3, according to the covariance matrix R i of the echo signal y i of the i-th range gate after the pulse pressure, an optimization model for solving the power value of the ground clutter echo signal x i of the i-th range gate is given: Solve the optimization model of the power value of the ground clutter echo signal x i of the i-th range gate: Obtain the kth power value pi , k of the ground clutter echo signal x i of the i-th range gate; wherein, k=1, 2, ..., 2N, N is the number of Doppler channels, Indicates the square of the F norm, and the superscript H indicates the conjugate transpose;
步骤4,将第i个距离门的地杂波回波信号xi的前N个功率值依次排列,构成第i个距离门的地杂波回波信号xi的功率矢量pi,pi=[pi,1,pi,2,...,pi,N]T;进而得到所有M个距离门的功率矩阵P,P=[p1,p2,...,pM],所有M个距离门的功率矩阵P即为最终的机载雷达回波数据矩阵;Step 4: Arrange the first N power values of the ground clutter echo signal x i of the i-th range gate in order to form the power vector p i , p i of the ground clutter echo signal x i of the i-th range gate =[p i, 1 , p i, 2 ,..., p i, N ] T ; and then get the power matrix P of all M range gates, P=[p 1 , p 2 ,..., p M ], the power matrix P of all M range gates is the final airborne radar echo data matrix;
步骤5,将最终的机载雷达回波数据矩阵中每个元素对应的距离门转换为相应的斜距,将最终的机载雷达回波数据矩阵中每个元素对应的多普勒频率转换为相应的方位角,并将该斜距和方位角由载机坐标系转换至大地坐标系,再将最终的机载雷达回波数据矩阵中每个元素作为大地坐标系中对应位置的像素值,得到最终的DBS图像。Step 5, convert the range gate corresponding to each element in the final airborne radar echo data matrix to the corresponding slant distance, and convert the Doppler frequency corresponding to each element in the final airborne radar echo data matrix to The corresponding azimuth angle, and the slant distance and azimuth angle are converted from the aircraft coordinate system to the earth coordinate system, and then each element in the final airborne radar echo data matrix is used as the pixel value of the corresponding position in the earth coordinate system, Get the final DBS image.
本发明与现有技术相比所具有的优点:Compared with the prior art, the present invention has the following advantages:
1)本发明方法与传统的DBS成像方法相比,提高了雷达对观测区域的重访率,提高了雷达对观测区域进行DBS成像的实时性;1) Compared with the traditional DBS imaging method, the inventive method improves the revisit rate of the radar to the observation area, and improves the real-time performance of the DBS imaging of the observation area by the radar;
2)本发明方法在雷达发射脉冲数较少的情况下,可获得较高地面分辨率的DBS图像。2) The method of the present invention can obtain a DBS image with a higher ground resolution when the number of pulses transmitted by the radar is small.
附图说明Description of drawings
图1是本发明的流程图;Fig. 1 is a flow chart of the present invention;
图2a是经过FFT变换后的距离多普勒图;Figure 2a is the range-Doppler map after FFT transformation;
图2b是经过SPICE变换后的距离多普勒图;Figure 2b is the range-Doppler map after SPICE transformation;
图3a是经过FFT变换后的距离多普勒图的距离维的切面图;Figure 3a is a section view of the range dimension of the range-Doppler map after FFT transformation;
图3b是经过SPICE变换后的距离多普勒图的距离维的切面图;Figure 3b is a section view of the range dimension of the range-Doppler map after SPICE transformation;
图4a是基于FFT变换的DBS成像结果图;Fig. 4a is the DBS imaging result diagram based on FFT transformation;
图4b是基于SPICE变换的DBS成像结果图。Fig. 4b is the image of DBS imaging results based on SPICE transformation.
具体实施方式:detailed description:
参照图1,本发明的基于SPICE的机载雷达高分辨DBS成像方法,具体实现步骤如下:With reference to Fig. 1, the airborne radar high-resolution DBS imaging method based on SPICE of the present invention, concrete realization steps are as follows:
步骤1,设定机载雷达接收的回波信号为 为第i个距离门的回波信号;在载机为参考原点的载机坐标系中,对机载雷达接收的回波信号在距离维进行脉冲压缩处理,得到脉压处理后的回波信号y,y=[y1,...,yi,...,yM],yi为脉压后的第i个距离门的回波信号;根据脉压后的第i个距离门的回波信号yi建立第i个距离门的地杂波回波信号xi的信号模型;其中,脉压后的第i个距离门的回波信号yi的维数为N×1,N为机载雷达发射的脉冲数,i=1,2,...,M,M为距离门个数。Step 1, set the echo signal received by the airborne radar as is the echo signal of the i-th range gate; in the aircraft coordinate system where the aircraft is the reference origin, the echo signal received by the airborne radar Perform pulse compression processing in the distance dimension to obtain the echo signal y after pulse pressure processing, y=[y 1 ,...,y i ,...,y M ], y i is the ith echo signal after pulse pressure The echo signal of the range gate; according to the echo signal y i of the i-th range gate after the pulse pressure, the signal model of the ground clutter echo signal x i of the i-th range gate is established; wherein, the i-th range gate after the pulse pressure The dimension of the echo signal y i of the range gates is N×1, N is the number of pulses emitted by the airborne radar, i=1, 2, . . . , M, and M is the number of range gates.
所述第i个距离门的地杂波回波信号xi的信号模型为:The signal model of the ground clutter echo signal x i of the i-th range gate is:
yi=Bxi+ey i =B x i +e
其中,B是时域导向矢量矩阵,其N个行向量对应为N个不同的1×N维的时域导向矢量,e是杂波信号或干扰信号,其维数为N×1。Among them, B is a time-domain steering vector matrix, and its N row vectors correspond to N different 1×N-dimensional time-domain steering vectors, e is a clutter signal or an interference signal, and its dimension is N×1.
步骤2,求取脉压后的第i个距离门的回波信号yi的协方差矩阵Ri。Step 2, obtain the covariance matrix R i of the echo signal y i of the i-th range gate after the pulse pressure.
所述脉压后的第i个距离门的回波信号yi的协方差矩阵Ri为:The covariance matrix R i of the echo signal y i of the i-th range gate after the pulse pressure is:
其中,A=[B IN],B是时域导向矢量矩阵,其N个行向量对应为N个不同的1×N维的时域导向矢量,IN为N×N的单位矩阵,Pi是第i个距离门的地杂波回波信号xi的功率矩阵,是一个对角矩阵,其对角线上的第k个元素pi,k为第i个距离门的地杂波回波信号xi的第k个功率值,k=1,2,...,2N,上标H表示共轭转置。Among them, A=[BI N ], B is the time-domain steering vector matrix, and its N row vectors correspond to N different 1×N-dimensional time-domain steering vectors, I N is an N×N unit matrix, P i is the power matrix of the ground clutter echo signal x i of the i-th range gate, which is a diagonal matrix, and the k-th element p i on its diagonal, k is the ground clutter echo signal of the i-th range gate The kth power value of the wave signal x i , k=1, 2, . . . , 2N, the superscript H indicates conjugate transposition.
步骤3,根据脉压后的第i个距离门的回波信号yi的协方差矩阵Ri,给出求解第i个距离门的地杂波回波信号xi的功率值的优化模型:求解第i个距离门的地杂波回波信号xi的功率值的优化模型得到第i个距离门的地杂波回波信号xi的第k个功率值pi,k;其中,k=1,2,...,2N,N为多普勒通道数,表示求F范数的平方,上标H表示共轭转置。Step 3, according to the covariance matrix R i of the echo signal y i of the i-th range gate after the pulse pressure, an optimization model for solving the power value of the ground clutter echo signal x i of the i-th range gate is given: An optimization model for solving the power value of the ground clutter echo signal x i of the i-th range gate Obtain the kth power value pi , k of the ground clutter echo signal x i of the i-th range gate; wherein, k=1, 2, ..., 2N, N is the number of Doppler channels, Represents the square of the F norm, and the superscript H represents the conjugate transpose.
所述求解第i个距离门的地杂波回波信号xi的功率值的优化模型为:The optimization model of the power value of the ground clutter echo signal x i of the described solution i range gate is:
其中,tr(·)表示矩阵的迹,C为一个常数。Among them, tr(·) represents the trace of the matrix, and C is a constant.
将所述求解第i个距离门的地杂波回波信号xi的功率值的优化问题进行简化,得到其简化形式为:Simplify the optimization problem of solving the power value of the ground clutter echo signal x i of the i-th range gate, and obtain its simplified form as:
其中,wk为第i个距离门的地杂波回波信号xi的第k个功率权值,其表达式为:Among them, w k is the kth power weight of the ground clutter echo signal x i of the i-th range gate, and its expression is:
其中,bkk是时域导向矢量矩阵B的对角线上的第k个元素。where b kk is the kth element on the diagonal of the time-domain steering vector matrix B.
所述求解第i个距离门的地杂波回波信号xi的功率值的优化模型其具体子步骤为:The optimization model for solving the power value of the ground clutter echo signal x i of the i-th range gate Its specific sub-steps are:
3.1设定l为迭代次数,迭代次数l的初始值为1,设定第i个距离门的地杂波回波信号xi的第k个功率值pi,k的初始值 3.1 Set l as the number of iterations, the initial value of the number of iterations l is 1, set the kth power value p i of the ground clutter echo signal x i of the i-th range gate, the initial value of k
3.2计算第l次迭代的第i个距离门的地杂波回波信号xi的第k个功率值 3.2 Calculate the kth power value of the ground clutter echo signal x i of the i-th range gate in the l-th iteration
其中,ak为矩阵A的第k列,A=[B IN],B是时域导向矢量矩阵,wk为第i个距离门的地杂波回波信号xi的第k个功率权值,其表达式为:Among them, a k is the kth column of matrix A, A=[BI N ], B is the time-domain steering vector matrix, w k is the kth power weight of the ground clutter echo signal x i of the i-th range gate value, whose expression is:
其中,bkk是时域导向矢量矩阵B的对角线上的第k个元素;Wherein, b kk is the kth element on the diagonal of the time domain steering vector matrix B;
3.3如果第l次迭代的第i个距离门的地杂波回波信号xi的第k个功率值与第l-1次迭代的第i个距离门的地杂波回波信号xi的第k个功率值的差的绝对值大于设定值ε,设定值ε的取值趋近于0,则令迭代次数l增加1,返回步骤4.2,3.3 If the k-th power value of the ground clutter echo signal x i of the i-th range gate in the l-th iteration and the kth power value of the ground clutter echo signal x i of the ith range gate of the l-1th iteration The absolute value of the difference is greater than the set value ε, and the value of the set value ε approaches 0, then increase the number of iterations l by 1, and return to step 4.2.
如果第l次迭代的第i个距离门的地杂波回波信号xi的第k个功率值与第l-1次迭代的第i个距离门的地杂波回波信号xi的第k个功率值的差的绝对值小于或等于设定值ε,则将第l次迭代的第i个距离门的地杂波回波信号xi的第k个功率值作为第i个距离门的地杂波回波信号xi的第k个功率值pi,k。If the k-th power value of the ground clutter echo signal x i of the i-th range gate in the l-th iteration and the kth power value of the ground clutter echo signal x i of the ith range gate of the l-1th iteration The absolute value of the difference is less than or equal to the set value ε, then the kth power value of the ground clutter echo signal x i of the i-th range gate in the l-th iteration As the kth power value p i,k of the ground clutter echo signal x i of the ith range gate.
步骤4,将第i个距离门的地杂波回波信号xi的前N个功率值依次排列,构成第i个距离门的地杂波回波信号xi的功率矢量pi,pi=[pi,1,pi,2,...,pi,k]T;进而得到所有M个距离门的功率矩阵P,P=[p1,p2,...,pM],所有M个距离门的功率矩阵P即为最终的机载雷达回波数据矩阵。Step 4: Arrange the first N power values of the ground clutter echo signal x i of the i-th range gate in order to form the power vector p i , p i of the ground clutter echo signal x i of the i-th range gate =[p i, 1 , p i, 2 ,..., p i, k ] T ; and then get the power matrix P of all M range gates, P=[p 1 , p 2 ,..., p M ], the power matrix P of all M range gates is the final airborne radar echo data matrix.
步骤5,将最终的机载雷达回波数据矩阵中每个元素对应的距离门转换为相应的斜距,将最终的机载雷达回波数据矩阵中每个元素对应的多普勒频率转换为相应的方位角,并将该斜距和方位角由载机坐标系转换至大地坐标系,再将最终的机载雷达回波数据矩阵中每个元素作为大地坐标系中对应位置的像素值,得到最终的DBS图像。Step 5, convert the range gate corresponding to each element in the final airborne radar echo data matrix to the corresponding slant distance, and convert the Doppler frequency corresponding to each element in the final airborne radar echo data matrix to The corresponding azimuth angle, and the slant distance and azimuth angle are converted from the aircraft coordinate system to the earth coordinate system, and then each element in the final airborne radar echo data matrix is used as the pixel value of the corresponding position in the earth coordinate system, Get the final DBS image.
本发明的效果可通多以下仿真实验作进一步说明:Effect of the present invention can be further illustrated by following simulation experiments:
1)仿真条件:1) Simulation conditions:
获取选定地形的雷达照射的实测数据,截取其前128个脉冲的数据,分别进行基于FFT变换的DBS成像和本发明的基于SPICE变换的DBS成像。Obtain the measured data of the radar irradiation of the selected terrain, intercept the data of the first 128 pulses, and perform DBS imaging based on FFT transformation and DBS imaging based on SPICE transformation of the present invention respectively.
2)仿真内容及结果分析:2) Simulation content and result analysis:
1.分别绘制经过FFT变换和SPICE变换后的距离多普勒图,如图2a和图2b所示。1. Draw the range-Doppler diagram after FFT transformation and SPICE transformation respectively, as shown in Fig. 2a and Fig. 2b.
从图2a中可以看出,基于FFT变换进行DBS成像时所用的雷达发射脉冲数较少,图中的强点出现了扩散现象,导致距离多普勒图的整体效果比较模糊,特别是当两个强点相距比较近时,会被模糊到一起,影响后期的处理。It can be seen from Fig. 2a that the number of radar transmission pulses used in DBS imaging based on FFT transform is small, and the strong points in the figure appear to diffuse, resulting in a blurred overall effect of the range-Doppler map, especially when two When two strong points are relatively close to each other, they will be blurred together, which will affect the later processing.
从图2b中可以看出,基于SPICE变换进行DBS成像时对雷达发射脉冲数的要求并不高,所以在雷达发射脉冲数较少的情况下也取得了较好的DBS成像效果,图中的强点能量比较集中,没有出现严重的扩散现象,对于相距较近的强点也可以清晰的分离开。It can be seen from Figure 2b that the requirements for the number of radar transmission pulses are not high when performing DBS imaging based on SPICE transformation, so a better DBS imaging effect has been achieved when the number of radar transmission pulses is small. The energy of the strong points is relatively concentrated, there is no serious diffusion phenomenon, and the strong points that are close to each other can be clearly separated.
2.分别绘制经过FFT变换和SPICE变换后的距离多普勒图的距离维的切面图,如图图3a和图3b所示.2. Draw the section diagrams of the range dimension of the range-Doppler map after FFT transformation and SPICE transformation respectively, as shown in Fig. 3a and Fig. 3b.
从图3a和图3b中可以看出,图中曲线的整体走势是完全一致的,但是图3b中的主瓣和目标区域外的旁瓣区域的幅值都要比图3a的幅值低,接近于零,而且图3b中的幅度峰值也相对较高,说明经过SPICE变换处理的数据旁瓣能量低,没有出现明显的主瓣能量泄露现象。It can be seen from Figure 3a and Figure 3b that the overall trend of the curves in the figure is completely consistent, but the amplitude of the main lobe and the side lobe area outside the target area in Figure 3b are both lower than those in Figure 3a. It is close to zero, and the amplitude peak value in Figure 3b is also relatively high, indicating that the data processed by SPICE transformation has low sidelobe energy, and there is no obvious leakage of mainlobe energy.
3.分别绘制基于FFT变换和SPICE变换的DBS成像结果图。3. Draw the DBS imaging results based on FFT transformation and SPICE transformation respectively.
从图4a和图4b中可以看出,相比于基于FFT变换的DBS成像结果,基于SPICE变换的DBS成像结果要更加清晰,而且强点更加明显,充分说明了本发明的基于SPICE变换的DBS成像方法的有效性。As can be seen from Fig. 4a and Fig. 4b, compared with the DBS imaging result based on FFT transformation, the DBS imaging result based on SPICE transformation is clearer, and the strong points are more obvious, which fully illustrates the DBS transformation based on SPICE transformation of the present invention Effectiveness of imaging methods.
显然,本领域的技术人员可以对本发明进行各种改动和变型而不脱离本发明的精神和范围;这样,倘若本发明的这些修改和变型属于本发明权利要求及其等同技术的范围之内,则本发明也意图包含这些改动和变型在内。Obviously, those skilled in the art can carry out various modifications and variations to the present invention without departing from the spirit and scope of the present invention; Like this, if these modifications and variations of the present invention belong to the scope of the claims of the present invention and equivalent technologies thereof, It is intended that the present invention also encompasses such changes and modifications.
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