CN113341371A - DOA estimation method based on L array and two-dimensional ESPRIT algorithm - Google Patents

DOA estimation method based on L array and two-dimensional ESPRIT algorithm Download PDF

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CN113341371A
CN113341371A CN202110596959.6A CN202110596959A CN113341371A CN 113341371 A CN113341371 A CN 113341371A CN 202110596959 A CN202110596959 A CN 202110596959A CN 113341371 A CN113341371 A CN 113341371A
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CN113341371B (en
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林仕文
周亚文
邹炜钦
李万春
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University of Electronic Science and Technology of China
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Abstract

本发明属于雷达信号处理技术领域,具体涉及一种基于L阵和二维ESPRIT算法的DOA估计方法。本发明提出了一种基于L阵和二维ESPRIT算法的DOA估计方法,在阵列接收到辐射源信号后,利用L阵的阵列特点对阵列数据进行处理,构造用于二维ESPRIT算法运算的数据矩阵,得到估计角度,完成信号源的方向测量估计。本发明的有益效果为,本发明利用L阵构造大矩阵,得到的矩阵形式简单,在后续的测向过程中保持了较低的计算复杂度,同时有效去除了统计独立噪声源的影响,改善了在高斯噪声环境下的分辨能力和统计性能。

Figure 202110596959

The invention belongs to the technical field of radar signal processing, and in particular relates to a DOA estimation method based on an L-array and a two-dimensional ESPRIT algorithm. The invention proposes a DOA estimation method based on L-array and two-dimensional ESPRIT algorithm. After the array receives the radiation source signal, the array data is processed by using the array characteristics of the L-array to construct the data for the two-dimensional ESPRIT algorithm operation. matrix, obtain the estimated angle, and complete the direction measurement estimation of the signal source. The beneficial effects of the present invention are that the present invention utilizes the L array to construct a large matrix, and the obtained matrix has a simple form, maintains a low computational complexity in the subsequent direction finding process, effectively removes the influence of statistical independent noise sources, and improves the The resolving power and statistical performance in Gaussian noise environment are improved.

Figure 202110596959

Description

一种基于L阵和二维ESPRIT算法的DOA估计方法A DOA Estimation Method Based on L-Array and Two-Dimensional ESPRIT Algorithm

技术领域technical field

本发明属于雷达信号处理技术领域,具体涉及一种基于L阵和二维ESPRIT算法的DOA估计方法。The invention belongs to the technical field of radar signal processing, and in particular relates to a DOA estimation method based on an L-array and a two-dimensional ESPRIT algorithm.

背景技术Background technique

在雷达信号处理中,基于L阵实现对目标雷达辐射源信号的波达方向(directionof arrival,DOA)估计一直是研究的重点,然而随着现代电磁频谱的日益密集、脉冲密度越来越高以及大功率电子设备的应用,电磁环境越来越复杂,传统的基于MUSIC算法的DOA估计方法面临着测向精度不高,计算复杂度大的问题,同时,这些方法大多数研究仅适用于一维DOA估计,针对实际空间下二维角度的测向能力有所欠缺,在L阵上实现二维DOA估计仍然是一个比较大的挑战。所以寻求新的技术和手段是当务之急,迫切需要提升雷达接收阵列的信号处理能力、测向精确性能。In radar signal processing, the estimation of the direction of arrival (DOA) of the target radar radiation source signal based on the L-array has always been the focus of research. With the application of high-power electronic equipment, the electromagnetic environment is becoming more and more complex. The traditional DOA estimation method based on the MUSIC algorithm faces the problems of low direction finding accuracy and large computational complexity. At the same time, most of these methods are only applicable to one-dimensional For DOA estimation, the direction finding ability for two-dimensional angles in real space is lacking, and it is still a big challenge to realize two-dimensional DOA estimation on L-array. Therefore, it is urgent to seek new technologies and means, and it is urgent to improve the signal processing capability and direction finding accuracy of the radar receiving array.

ESPRIT算法其原理在于利用数据协方差矩阵信号子空间的旋转不变特性求解信号的入射角等信息,由于不需要进行谱峰搜索,其复杂度和计算量与MUSIC算法相比大幅降低,在DOA估计中得到了广泛的应用。针对基于L阵的二维测向,此前也有一些二维ESPRIT方法提出,但这些方法都存在构造形式复杂,计算量高的问题,且不能很好的抑制噪声影响,在进行雷达信号处理时不能很好地平衡性能与计算成本之间的关系,阵列测向结果始终会存在较大误差。The principle of the ESPRIT algorithm is to use the rotation invariant characteristics of the signal subspace of the data covariance matrix to solve the information such as the incident angle of the signal. Since it does not need to search for spectral peaks, its complexity and calculation amount are greatly reduced compared with the MUSIC algorithm. In DOA has been widely used in estimation. For the two-dimensional direction finding based on the L-array, some two-dimensional ESPRIT methods have been proposed before, but these methods have the problems of complex structure and high calculation amount, and can not suppress the influence of noise well, and cannot be used in radar signal processing. With a good balance between performance and computational cost, there will always be large errors in the array direction finding results.

发明内容SUMMARY OF THE INVENTION

本发明的目的,是针对上述问题,提出了一种基于L阵和二维ESPRIT算法的DOA估计方法,在阵列接收到辐射源信号后,利用L阵的阵列特点对阵列数据进行处理,构造用于二维ESPRIT算法运算的数据矩阵,得到估计角度,完成信号源的方向测量估计。The purpose of the present invention is to solve the above problems, and propose a DOA estimation method based on L-array and two-dimensional ESPRIT algorithm. Based on the data matrix operated by the two-dimensional ESPRIT algorithm, the estimated angle is obtained, and the direction measurement and estimation of the signal source is completed.

本发明的技术方案为:The technical scheme of the present invention is:

将L阵划分为四个子阵,通过对空间中目标信号接收数据进行处理,计算L阵中三个无共用阵元的子阵之间的互协方差矩阵,利用三个互协方差矩阵组成一个用于L阵子空间分解的大矩阵,根据旋转不变性得到两个旋转矩阵,对两个矩阵基于二维ESPRIT算法进行处理,通过特征分解得到两个旋转矩阵的特征值并进行特征值配对,最后求解得到信号的方位角和仰角,完成二维DOA估计。Divide the L array into four sub-arrays, and calculate the cross-covariance matrix between the three sub-arrays without shared array elements in the L-array by processing the received data of the target signal in the space, and use the three cross-covariance matrices to form a For the large matrix used for L-array subspace decomposition, two rotation matrices are obtained according to the rotation invariance, and the two matrices are processed based on the two-dimensional ESPRIT algorithm. Solve the azimuth and elevation of the obtained signal, and complete the two-dimensional DOA estimation.

本发明基于L阵的信号接收模型如图1所示,信号si(t)的波达方向(DOA)用矢量

Figure BDA0003091485480000021
表示:其中θ为方位角,范围为θ∈(-π,π),定义为波达方向在xoy平面的投影与x正半轴的夹角,
Figure BDA0003091485480000022
为仰角,范围为
Figure BDA0003091485480000023
定义为波达方向在yoz平面的投影与z正半轴的夹角。相邻阵元之间的间距为d。The signal receiving model based on the L-array of the present invention is shown in Figure 1, and the direction of arrival (DOA) of the signal si (t) uses a vector
Figure BDA0003091485480000021
Representation: where θ is the azimuth angle, the range is θ∈(-π,π), which is defined as the angle between the projection of the direction of arrival on the xoy plane and the positive semi-axis of x,
Figure BDA0003091485480000022
is the elevation angle, and the range is
Figure BDA0003091485480000023
It is defined as the angle between the projection of the direction of arrival on the yoz plane and the positive half-axis of z. The spacing between adjacent array elements is d.

为了简化分析过程和保证所构建的数学模型的合理性,本发明中基于L阵的信号接收模型基于如下假设:(1)不考虑接收天线阵列的阵元通道幅相误差;(2)阵列接收信号均为远场点源发出的窄带信号,信号的中心频率相同且已知,信号波长λ大于阵元间距d的两倍,即λ≥2d;(3)接收信号的相位是随机的,不考虑严格非圆信号等已知信号部分先验信息下的特殊情况。In order to simplify the analysis process and ensure the rationality of the constructed mathematical model, the signal receiving model based on the L-array in the present invention is based on the following assumptions: (1) the amplitude and phase errors of the array element channels of the receiving antenna array are not considered; (2) the array receives The signals are all narrowband signals from far-field point sources, the center frequencies of the signals are the same and known, and the signal wavelength λ is greater than twice the array element spacing d, that is, λ≥2d; (3) The phase of the received signal is random, not Consider the special case under the prior information of known signal parts such as strictly non-circular signals.

如图2所示,均匀L阵可划分为四个子阵:x轴上的前M个阵元组成子阵X1,后M个阵元组成子阵X2;y轴上的前M个阵元组成子阵Y1,后M个阵元组成子阵Y2As shown in Figure 2, a uniform L-array can be divided into four sub-arrays: the first M array elements on the x-axis form a sub-array X 1 , the last M array elements form a sub-array X 2 ; the first M array elements on the y-axis form a sub-array X 2 ; The elements form a sub-array Y 1 , and the last M array elements form a sub-array Y 2 .

子阵X1、X2和Y1、Y2接收的数据矩阵分别为:The data matrices received by the sub-arrays X 1 , X 2 and Y 1 , Y 2 are:

Figure BDA0003091485480000024
Figure BDA0003091485480000024

其中,xl、yl分别表示阵列X与阵列Y标号为l(l=0,1,2,…,M,M+1)的阵元接收的数据。Wherein, x l and y l respectively represent the data received by the array elements of the array X and the array Y whose labels are l (l=0, 1, 2, . . . , M, M+1).

基于L阵和二维ESPRIT的DOA估计方法,主要包括以下步骤:The DOA estimation method based on L-array and two-dimensional ESPRIT mainly includes the following steps:

S1、利用子阵X1、X2和Y1、Y2接收的数据矩阵构造得到三个互协方差矩阵:S1. Three cross-covariance matrices are obtained by constructing the data matrices received by the sub-arrays X 1 , X 2 and Y 1 , Y 2 :

Figure BDA0003091485480000025
Figure BDA0003091485480000025

由于子阵X1和Y2、子阵X2和Y1、子阵X2和Y2之间均没有共用阵元,且各阵元接收的噪声相互独立,因此得到的三个互协方差矩阵中都不存在噪声项。Since the sub-arrays X 1 and Y 2 , the sub-arrays X 2 and Y 1 , and the sub-arrays X 2 and Y 2 do not share array elements, and the noises received by each array element are independent of each other, the obtained three cross-covariances There are no noise terms in the matrix.

S2、将步骤S1中三个互协方差矩阵堆叠成一个大矩阵CL,矩阵的构造形式为S2. Stack the three cross-covariance matrices in step S1 into a large matrix CL , and the structure of the matrix is as follows

Figure BDA0003091485480000031
Figure BDA0003091485480000031

S3、对步骤S2中构造的大矩阵CL进行奇异值分解,将前N个大特征值对应的特征向量组成的矩阵作为信号子空间的估计得到信号子空间的估计ESS3. Perform singular value decomposition on the large matrix CL constructed in step S2, and use the matrix formed by the eigenvectors corresponding to the first N large eigenvalues as the estimation of the signal subspace to obtain the estimation E S of the signal subspace.

Figure BDA0003091485480000032
Figure BDA0003091485480000032

其中,E1、E2和E3为组成矩阵ES的三个M×M维块矩阵;Wherein, E 1 , E 2 and E 3 are three M×M-dimensional block matrices that form the matrix ES;

S4、计算两个旋转矩阵ΨX和ΨY,计算公式为S4. Calculate two rotation matrices Ψ X and Ψ Y , the calculation formula is

Figure BDA0003091485480000033
Figure BDA0003091485480000033

Figure BDA0003091485480000034
Figure BDA0003091485480000034

对这两个旋转矩阵进行特征分解,得到Eigen decomposition of these two rotation matrices, we get

Figure BDA0003091485480000035
Figure BDA0003091485480000035

Figure BDA0003091485480000036
Figure BDA0003091485480000036

其中,λ1,…,λN和γ1,…,γN分别是旋转矩阵ΨX和ΨY的特征值,ΦX和ΦY是特征值矩阵,T1和T2是由旋转矩阵ΨX和ΨY的特征向量组成的正交矩阵。where λ 1 ,…,λ N and γ 1 ,…,γ N are the eigenvalues of the rotation matrices Ψ X and Ψ Y respectively, Φ X and Φ Y are the eigenvalue matrices, T 1 and T 2 are the rotation matrices Ψ Orthogonal matrix of eigenvectors of X and Ψ Y.

S5、基于二维ESPRIT算法进行二维角度参数配对,确定两个旋转矩阵ΨX和ΨY的特征值之间的对应关系,具体步骤为:S5. Perform two-dimensional angle parameter pairing based on the two-dimensional ESPRIT algorithm to determine the correspondence between the eigenvalues of the two rotation matrices Ψ X and Ψ Y. The specific steps are:

S51、构造估计矩阵

Figure BDA0003091485480000037
构造形式为:S51. Construct an estimation matrix
Figure BDA0003091485480000037
The construction form is:

Figure BDA0003091485480000038
Figure BDA0003091485480000038

S52、取出矩阵

Figure BDA0003091485480000041
的对角元素u1,…,uN,并对这些元素取复数相角,并按照相角大小,从大到小对对角元素进行排序,得到排序后的对角元素
Figure BDA0003091485480000042
取矩阵ΨY特征值γ1,…,γN的相角,并按照相角的大小按从大到小对γ1,…,γN进行排序,得到排序后的特征值顺序
Figure BDA0003091485480000043
按照排序后的序号得到配对关系S52, take out the matrix
Figure BDA0003091485480000041
The diagonal elements u 1 ,…,u N of , take complex phase angles for these elements, and sort the diagonal elements according to the size of the phase angles, from large to small, to obtain the sorted diagonal elements
Figure BDA0003091485480000042
Take the phase angles of the eigenvalues γ 1 ,…,γ N of the matrix Ψ Y , and sort γ 1 ,…,γ N according to the size of the phase angles in descending order to obtain the sorted eigenvalue order
Figure BDA0003091485480000043
Get the pairing relationship according to the sorted sequence number

Figure BDA0003091485480000044
Figure BDA0003091485480000044

S53、根据步骤S52中对角元素

Figure BDA0003091485480000045
与矩阵T1中特征向量的对应关系,调整ΨX的特征值顺序(若
Figure BDA0003091485480000046
在矩阵
Figure BDA0003091485480000047
中的行序为j,那么其对应特征向量为矩阵T1的第j个列向量,对应的ΨX的特征值为λj),得到调整之后矩阵ΨX的特征值
Figure BDA0003091485480000048
以及配对关系为S53, according to the diagonal elements in step S52
Figure BDA0003091485480000045
The corresponding relationship with the eigenvectors in the matrix T1, adjust the eigenvalue order of ΨX (if
Figure BDA0003091485480000046
in the matrix
Figure BDA0003091485480000047
The row order in is j, then its corresponding eigenvector is the jth column vector of the matrix T 1 , and the corresponding eigenvalue of Ψ X is λ j ), and the eigenvalue of the matrix Ψ X after adjustment is obtained.
Figure BDA0003091485480000048
and the pairing relationship is

Figure BDA0003091485480000049
Figure BDA0003091485480000049

S54、根据步骤S52、S53得到的两组配对关系,得到矩阵ΨX和ΨY的特征值之间的配对关系为S54. According to the two groups of pairing relationships obtained in steps S52 and S53, the pairing relationship between the eigenvalues of the matrices Ψ X and Ψ Y is obtained as

Figure BDA00030914854800000410
Figure BDA00030914854800000410

S6、利用经过步骤S5配对后的特征值,计算目标辐射源信号的二维波达方向的数值解

Figure BDA00030914854800000411
完成二维DOA估计:S6, using the eigenvalues paired in step S5 to calculate the numerical solution of the two-dimensional direction of arrival of the target radiation source signal
Figure BDA00030914854800000411
Complete the 2D DOA estimation:

Figure BDA00030914854800000412
Figure BDA00030914854800000412

其中,in,

Figure BDA00030914854800000413
Figure BDA00030914854800000413

Figure BDA00030914854800000414
Figure BDA00030914854800000414

Figure BDA00030914854800000415
为第i个信号的方位角估值,
Figure BDA00030914854800000416
为第i个信号的仰角估值,函数“arctan(·)”和“arcsin(·)”分别表示反正切函数和反正弦函数。
Figure BDA00030914854800000415
is an estimate of the azimuth angle of the ith signal,
Figure BDA00030914854800000416
For the elevation angle estimation of the ith signal, the functions "arctan(·)" and "arcsin(·)" represent the arc tangent function and the arc sine function, respectively.

本发明的有益效果为,本发明利用L阵构造大矩阵,得到的矩阵形式简单,在后续的测向过程中保持了较低的计算复杂度,同时有效去除了统计独立噪声源的影响,改善了在高斯噪声环境下的分辨能力和统计性能。The beneficial effects of the present invention are that the present invention utilizes the L array to construct a large matrix, and the obtained matrix has a simple form, maintains a low computational complexity in the subsequent direction finding process, effectively removes the influence of statistical independent noise sources, and improves the The resolving power and statistical performance in Gaussian noise environment are improved.

附图说明Description of drawings

图1为L阵信号接收示意图;Figure 1 is a schematic diagram of L-array signal reception;

图2为L阵子阵划分示意图;Fig. 2 is a schematic diagram of L-array sub-array division;

图3为RMSE随SNR变化曲线;Figure 3 is the curve of RMSE versus SNR;

图4为RMSE随子阵数阵元数变化曲线;Fig. 4 is the change curve of RMSE with the number of sub-array elements;

图5为仿真运行时间随子阵阵元数变化曲线。Figure 5 shows the variation curve of the simulation running time with the number of sub-array elements.

具体实施方式Detailed ways

下面将结合附图和仿真,对本发明的性能进行说明。The performance of the present invention will be described below with reference to the accompanying drawings and simulations.

利用Matlab对本发明所提方法进行仿真验证。计算机仿真环境:MicrosoftWindows 10操作系统,Matlab 2020a软件,AMD R7-4800U处理器(支持AVX指令集),16GBDDR4-3200内存。The method proposed in the present invention is simulated and verified by using Matlab. Computer simulation environment: Microsoft Windows 10 operating system, Matlab 2020a software, AMD R7-4800U processor (supporting AVX instruction set), 16GBDDR4-3200 memory.

(一)本发明方法的DOA测向估计性能(1) DOA direction finding estimation performance of the method of the present invention

仿真1:方法的方向精度随信号信噪比变化情况Simulation 1: The direction accuracy of the method varies with the signal-to-noise ratio

空间中的L阵阵元总数为13,四个子阵的阵元数均为7,仿真信号数据长度为500个快拍,信号的来波方向为(60°,60°)。不同信噪比下均进行1000次Monte-Carlo实验,得到本发明方法的角度估计RMSE随SNR变化曲线如图3所示。The total number of L-array elements in the space is 13, the number of elements of the four sub-arrays is 7, the length of the simulated signal data is 500 snapshots, and the direction of arrival of the signal is (60°, 60°). 1000 times of Monte-Carlo experiments are carried out under different signal-to-noise ratios, and the curve of the angle estimated RMSE of the method of the present invention as a function of SNR is obtained as shown in Fig. 3 .

结论分析:从仿真结果来看,本发明L阵ESPRIT新方法的具有较高的波达方向估计精度,性能上的损失较少,测向效果颇佳。Conclusion analysis: From the simulation results, the new L-array ESPRIT method of the present invention has high DOA estimation accuracy, less performance loss, and good direction finding effect.

仿真2:方法的方向精度随接收阵列子阵阵元数变化情况Simulation 2: The direction accuracy of the method varies with the number of sub-array elements of the receiving array

空间中的L形阵列,四个子阵的阵元数均为M,仿真数据长度为200个快拍,信噪比为-10dB,信号的来波方向为(60°,60°),不同子阵数M下进行500次Monte-Carlo实验得到本发明ESPRIT算法的RMSE随子阵阵元数M的变化曲线如图4所示。In the L-shaped array in space, the number of array elements of the four sub-arrays are all M, the length of the simulated data is 200 snapshots, the signal-to-noise ratio is -10dB, the direction of arrival of the signal is (60°, 60°), and the different sub-arrays are 500 times of Monte-Carlo experiments are performed under the array number M to obtain the variation curve of the RMSE of the ESPRIT algorithm of the present invention with the number M of sub-array elements as shown in FIG. 4 .

结论分析:图4的结果表明,本发明方法的统计性能随子阵阵元数增多而增强。Conclusion analysis: The results in Figure 4 show that the statistical performance of the method of the present invention increases with the increase of the number of sub-array elements.

(二)本发明方法的运行时间(2) the running time of the method of the present invention

仿真1:方法的仿真时间Simulation 1: Simulation time of the method

空间中的L形阵列,四个子阵的阵元数均为M,信号的来波方向为(30°,30°),仿真数据长度为500个快拍,信噪比为0dB。对本发明方法进行仿真,得到不同子阵阵元数下该算法进行1000次Monte-Carlo实验的仿真时长。For the L-shaped array in space, the number of array elements of the four sub-arrays is M, the direction of arrival of the signal is (30°, 30°), the length of the simulated data is 500 snapshots, and the signal-to-noise ratio is 0dB. The method of the present invention is simulated to obtain the simulation duration of 1000 Monte-Carlo experiments performed by the algorithm under different numbers of sub-array elements.

将仿真时长数据绘制成曲线图得到该算法仿真时长随子阵阵元数变化曲线如图5所示。The simulation duration data is drawn into a curve graph to obtain the variation curve of the simulation duration of the algorithm with the number of sub-array elements, as shown in Figure 5.

结论分析:从图5的结果来看,随着子阵阵元数的增长,本发明算法的时长也随之增长,但增长幅度较小,这说明本发明计算成本较小,计算复杂度低,有着计算上的优势。Conclusion analysis: From the results of Figure 5, with the increase of the number of sub-array elements, the duration of the algorithm of the present invention also increases, but the increase is small, which shows that the present invention has a small computational cost and low computational complexity. , has a computational advantage.

综合以上仿真结果,本发明所提方法在计算成本和估计性能之间取得了更好的平衡。Based on the above simulation results, the method proposed in the present invention achieves a better balance between computational cost and estimation performance.

Claims (1)

1.一种基于L阵和二维ESPRIT算法的DOA估计方法,建立基于L阵的信号接收模型,信号si(t)的波达方向(DOA)用矢量
Figure FDA0003091485470000011
表示,其中θ为方位角,范围为θ∈(-π,π),定义为波达方向在xoy平面的投影与x正半轴的夹角,
Figure FDA0003091485470000012
为仰角,范围为
Figure FDA0003091485470000013
定义为波达方向在yoz平面的投影与z正半轴的夹角,相邻阵元之间的间距为d;均匀L阵划分为四个子阵:x轴上的前M个阵元组成子阵X1,后M个阵元组成子阵X2;y轴上的前M个阵元组成子阵Y1,后M个阵元组成子阵Y2;子阵X1、X2和Y1、Y2接收的数据矩阵分别为:
1. A DOA estimation method based on L-array and two-dimensional ESPRIT algorithm, establish a signal receiving model based on L-array, and the direction of arrival (DOA) of the signal s i (t) uses a vector
Figure FDA0003091485470000011
represents, where θ is the azimuth angle and the range is θ∈(-π,π), which is defined as the angle between the projection of the direction of arrival on the xoy plane and the positive semi-axis of x,
Figure FDA0003091485470000012
is the elevation angle, and the range is
Figure FDA0003091485470000013
Defined as the angle between the projection of the direction of arrival on the yoz plane and the positive half-axis of z, the distance between adjacent array elements is d; the uniform L array is divided into four sub-arrays: the first M array elements on the x-axis form sub-arrays Array X 1 , the last M array elements form a sub-array X 2 ; the first M array elements on the y-axis form a sub-array Y 1 , and the last M array elements form a sub-array Y 2 ; the sub-arrays X 1 , X 2 and Y The data matrices received by 1 and Y 2 are:
Figure FDA0003091485470000014
Figure FDA0003091485470000014
其中xl、yl分别表示阵列X与阵列Y标号为l的阵元接收的数据,l=0,1,2,…,M,M+1;where x l and y l respectively represent the data received by the array element labeled l in array X and array Y, and l=0,1,2,...,M,M+1; 其特征在于,DOA估计方法包括以下步骤:It is characterized in that, the DOA estimation method comprises the following steps: S1、利用子阵X1、X2和Y1、Y2接收的数据矩阵构造得到三个互协方差矩阵:S1. Three cross-covariance matrices are obtained by constructing the data matrices received by the sub-arrays X 1 , X 2 and Y 1 , Y 2 :
Figure FDA0003091485470000015
Figure FDA0003091485470000015
由于子阵X1和Y2、子阵X2和Y1、子阵X2和Y2之间均没有共用阵元,且各阵元接收的噪声相互独立,因此得到的三个互协方差矩阵中都不存在噪声项;Since the sub-arrays X 1 and Y 2 , the sub-arrays X 2 and Y 1 , and the sub-arrays X 2 and Y 2 do not share array elements, and the noises received by each array element are independent of each other, the obtained three cross-covariances There are no noise terms in the matrix; S2、将步骤S1中三个互协方差矩阵堆叠成一个矩阵CL,矩阵的构造形式为S2. Stack the three cross-covariance matrices in step S1 into a matrix CL , and the structure of the matrix is as follows
Figure FDA0003091485470000016
Figure FDA0003091485470000016
S3、对步骤S2中构造的矩阵CL进行奇异值分解,将前N个特征值对应的特征向量组成的矩阵作为信号子空间的估计得到信号子空间的估计ESS3. Perform singular value decomposition on the matrix CL constructed in step S2, and use the matrix composed of the eigenvectors corresponding to the first N eigenvalues as the estimation of the signal subspace to obtain the estimation of the signal subspace E S :
Figure FDA0003091485470000021
Figure FDA0003091485470000021
其中,E1、E2和E3为组成矩阵ES的三个M×M维块矩阵;Wherein, E 1 , E 2 and E 3 are three M×M-dimensional block matrices that form the matrix ES; S4、计算两个旋转矩阵ΨX和ΨY,计算公式为S4. Calculate two rotation matrices Ψ X and Ψ Y , the calculation formula is
Figure FDA0003091485470000022
Figure FDA0003091485470000022
Figure FDA0003091485470000023
Figure FDA0003091485470000023
对这两个旋转矩阵进行特征分解,得到Eigen decomposition of these two rotation matrices, we get
Figure FDA0003091485470000024
Figure FDA0003091485470000024
Figure FDA0003091485470000025
Figure FDA0003091485470000025
其中,λ1,…,λN和γ1,…,γN分别是旋转矩阵ΨX和ΨY的特征值,ΦX和ΦY是特征值矩阵,T1和T2是由旋转矩阵ΨX和ΨY的特征向量组成的正交矩阵;where λ 1 ,…,λ N and γ 1 ,…,γ N are the eigenvalues of the rotation matrices Ψ X and Ψ Y respectively, Φ X and Φ Y are the eigenvalue matrices, T 1 and T 2 are the rotation matrices Ψ Orthogonal matrix composed of eigenvectors of X and Ψ Y ; S5、基于二维ESPRIT算法进行二维角度参数配对,确定两个旋转矩阵ΨX和ΨY的特征值之间的对应关系,具体步骤为:S5. Perform two-dimensional angle parameter pairing based on the two-dimensional ESPRIT algorithm to determine the correspondence between the eigenvalues of the two rotation matrices Ψ X and Ψ Y. The specific steps are: S51、构造估计矩阵
Figure FDA0003091485470000026
构造形式为:
S51. Construct an estimation matrix
Figure FDA0003091485470000026
The construction form is:
Figure FDA0003091485470000027
Figure FDA0003091485470000027
S52、取出矩阵
Figure FDA0003091485470000028
的对角元素u1,…,uN,并对这些元素取复数相角,并按照相角大小,从大到小对对角元素进行排序,得到排序后的对角元素
Figure FDA0003091485470000029
取矩阵ΨY特征值γ1,…,γN的相角,并按照相角的大小按从大到小对γ1,…,γN进行排序,得到排序后的特征值顺序
Figure FDA00030914854700000210
按照排序后的序号得到配对关系
S52, take out the matrix
Figure FDA0003091485470000028
The diagonal elements u 1 ,…,u N of , take complex phase angles for these elements, and sort the diagonal elements according to the size of the phase angles, from large to small, to obtain the sorted diagonal elements
Figure FDA0003091485470000029
Take the phase angles of the eigenvalues γ 1 ,…,γ N of the matrix Ψ Y , and sort γ 1 ,…,γ N according to the size of the phase angles in descending order to obtain the sorted eigenvalue order
Figure FDA00030914854700000210
Get the pairing relationship according to the sorted sequence number
Figure FDA0003091485470000031
Figure FDA0003091485470000031
S53、根据步骤S52中对角元素
Figure FDA0003091485470000032
与矩阵T1中特征向量的对应关系,调整ΨX的特征值顺序,调整方式为,若
Figure FDA0003091485470000033
在矩阵
Figure FDA0003091485470000034
中的行序为j,那么其对应特征向量为矩阵T1的第j个列向量,对应的ΨX的特征值为λj,得到调整之后矩阵ΨX的特征值
Figure FDA0003091485470000035
以及配对关系为
S53, according to the diagonal elements in step S52
Figure FDA0003091485470000032
Corresponding relationship with the eigenvectors in the matrix T1, adjust the eigenvalue order of ΨX , the adjustment method is, if
Figure FDA0003091485470000033
in the matrix
Figure FDA0003091485470000034
The row order in is j, then its corresponding eigenvector is the jth column vector of matrix T 1 , and the corresponding eigenvalue of Ψ X is λ j , and the eigenvalue of matrix Ψ X after adjustment is obtained.
Figure FDA0003091485470000035
and the pairing relationship is
Figure FDA0003091485470000036
Figure FDA0003091485470000036
S54、根据步骤S52、S53得到的两组配对关系,得到矩阵ΨX和ΨY的特征值之间的配对关系为S54. According to the two groups of pairing relationships obtained in steps S52 and S53, the pairing relationship between the eigenvalues of the matrices Ψ X and Ψ Y is obtained as
Figure FDA0003091485470000037
Figure FDA0003091485470000037
S6、利用经过步骤S5配对后的特征值,计算目标辐射源信号的二维波达方向的数值解
Figure FDA0003091485470000038
完成二维DOA估计:
S6, using the eigenvalues paired in step S5 to calculate the numerical solution of the two-dimensional direction of arrival of the target radiation source signal
Figure FDA0003091485470000038
Complete the 2D DOA estimation:
Figure FDA0003091485470000039
Figure FDA0003091485470000039
其中,in,
Figure FDA00030914854700000310
Figure FDA00030914854700000310
Figure FDA00030914854700000311
Figure FDA00030914854700000311
Figure FDA00030914854700000312
为第i个信号的方位角估值,
Figure FDA00030914854700000313
为第i个信号的仰角估值,函数“arctan(·)”和“arcsin(·)”分别表示反正切函数和反正弦函数。
Figure FDA00030914854700000312
is an estimate of the azimuth angle of the ith signal,
Figure FDA00030914854700000313
For the elevation angle estimation of the ith signal, the functions "arctan(·)" and "arcsin(·)" represent the arc tangent function and the arc sine function, respectively.
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Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115308680A (en) * 2022-08-04 2022-11-08 中国科学院微小卫星创新研究院 Two-dimensional DOA estimation method, system and computer readable medium
CN115421098A (en) * 2022-07-12 2022-12-02 南京航空航天大学 2-D DOA Estimation Method Based on Nested Planar Array Descending Dimension Root-Finding MUSIC

Citations (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6278406B1 (en) * 1998-03-24 2001-08-21 Nec Corporation Direction finder and device for processing measurement results for the same
CN102253363A (en) * 2011-03-29 2011-11-23 西安交通大学 Device for estimating two-dimensional direction of arrival (DOA) of coherent signals based on L array and method thereof
CN102279381A (en) * 2011-03-29 2011-12-14 西安交通大学 L-shaped array-based two-dimensional wave arrival direction estimating device and method thereof
US20140145825A1 (en) * 2009-03-11 2014-05-29 Checkpoint Systems, Inc Localization Using Virtual Antenna Arrays in Modulated Backscatter Rfid Systems
CN106054123A (en) * 2016-06-06 2016-10-26 电子科技大学 Sparse L-shaped array and two-dimensional DOA estimation method thereof
US20170082730A1 (en) * 2015-09-17 2017-03-23 Panasonic Corporation Radar device
CN106872935A (en) * 2017-03-20 2017-06-20 北京理工大学 A kind of Electromagnetic Vector Sensor Array Wave arrival direction estimating method based on quaternary number
CN108663653A (en) * 2018-05-17 2018-10-16 西安电子科技大学 Wave arrival direction estimating method based on L-shaped Electromagnetic Vector Sensor Array
CN110286351A (en) * 2019-07-12 2019-09-27 电子科技大学 A two-dimensional DOA estimation method and device based on L-shaped nested matrix
CN110286350A (en) * 2019-07-12 2019-09-27 电子科技大学 An accurate pairing method and device for L-type sparse array DOA estimation
US20190377056A1 (en) * 2018-06-12 2019-12-12 Kaam Llc. Direction of Arrival Estimation of Acoustic-Signals From Acoustic Source Using Sub-Array Selection
CN110954859A (en) * 2019-11-22 2020-04-03 宁波大学 L-shaped array-based two-dimensional incoherent distributed non-circular signal parameter estimation method
CN111175690A (en) * 2019-10-29 2020-05-19 宁波大学 Joint diagonalization L-type MIMO radar circle and non-circle mixed direction finding method
CN111983554A (en) * 2020-08-28 2020-11-24 西安电子科技大学 High Accuracy 2D DOA Estimation under Nonuniform L Arrays
CN112763972A (en) * 2020-12-30 2021-05-07 长沙航空职业技术学院 Sparse representation-based double parallel linear array two-dimensional DOA estimation method and computing equipment

Patent Citations (15)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6278406B1 (en) * 1998-03-24 2001-08-21 Nec Corporation Direction finder and device for processing measurement results for the same
US20140145825A1 (en) * 2009-03-11 2014-05-29 Checkpoint Systems, Inc Localization Using Virtual Antenna Arrays in Modulated Backscatter Rfid Systems
CN102253363A (en) * 2011-03-29 2011-11-23 西安交通大学 Device for estimating two-dimensional direction of arrival (DOA) of coherent signals based on L array and method thereof
CN102279381A (en) * 2011-03-29 2011-12-14 西安交通大学 L-shaped array-based two-dimensional wave arrival direction estimating device and method thereof
US20170082730A1 (en) * 2015-09-17 2017-03-23 Panasonic Corporation Radar device
CN106054123A (en) * 2016-06-06 2016-10-26 电子科技大学 Sparse L-shaped array and two-dimensional DOA estimation method thereof
CN106872935A (en) * 2017-03-20 2017-06-20 北京理工大学 A kind of Electromagnetic Vector Sensor Array Wave arrival direction estimating method based on quaternary number
CN108663653A (en) * 2018-05-17 2018-10-16 西安电子科技大学 Wave arrival direction estimating method based on L-shaped Electromagnetic Vector Sensor Array
US20190377056A1 (en) * 2018-06-12 2019-12-12 Kaam Llc. Direction of Arrival Estimation of Acoustic-Signals From Acoustic Source Using Sub-Array Selection
CN110286351A (en) * 2019-07-12 2019-09-27 电子科技大学 A two-dimensional DOA estimation method and device based on L-shaped nested matrix
CN110286350A (en) * 2019-07-12 2019-09-27 电子科技大学 An accurate pairing method and device for L-type sparse array DOA estimation
CN111175690A (en) * 2019-10-29 2020-05-19 宁波大学 Joint diagonalization L-type MIMO radar circle and non-circle mixed direction finding method
CN110954859A (en) * 2019-11-22 2020-04-03 宁波大学 L-shaped array-based two-dimensional incoherent distributed non-circular signal parameter estimation method
CN111983554A (en) * 2020-08-28 2020-11-24 西安电子科技大学 High Accuracy 2D DOA Estimation under Nonuniform L Arrays
CN112763972A (en) * 2020-12-30 2021-05-07 长沙航空职业技术学院 Sparse representation-based double parallel linear array two-dimensional DOA estimation method and computing equipment

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
T.Q.XIA等: ""2-D angle of arrival estimation with two parallel uniform linear arrays for coherent signals"", 《2007 IEEE RADAR CONFERENCE》 *
夏铁骑: ""二维波达方向估计方法研究"", 《中国优秀博硕士学位论文全文数据库(博士)信息科技辑》 *
曾操等: ""一种基于双平行线阵相干源二维波达方向估计的新方法"", 《雷达科学与技术》 *
王爱莹: ""卫星干扰源定位及干扰抑制技术研究"", 《中国优秀博硕士学位论文全文数据库(硕士)信息科技辑》 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN115421098A (en) * 2022-07-12 2022-12-02 南京航空航天大学 2-D DOA Estimation Method Based on Nested Planar Array Descending Dimension Root-Finding MUSIC
CN115308680A (en) * 2022-08-04 2022-11-08 中国科学院微小卫星创新研究院 Two-dimensional DOA estimation method, system and computer readable medium

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