CN107102291B - The relatively prime array Wave arrival direction estimating method of mesh freeization based on virtual array interpolation - Google Patents
The relatively prime array Wave arrival direction estimating method of mesh freeization based on virtual array interpolation Download PDFInfo
- Publication number
- CN107102291B CN107102291B CN201710302902.4A CN201710302902A CN107102291B CN 107102291 B CN107102291 B CN 107102291B CN 201710302902 A CN201710302902 A CN 201710302902A CN 107102291 B CN107102291 B CN 107102291B
- Authority
- CN
- China
- Prior art keywords
- array
- virtual
- matrix
- virtual array
- signal
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
- 238000000034 method Methods 0.000 title claims abstract description 61
- 239000011159 matrix material Substances 0.000 claims abstract description 110
- 238000005070 sampling Methods 0.000 claims abstract description 26
- 238000005457 optimization Methods 0.000 claims abstract description 23
- 238000003491 array Methods 0.000 claims description 16
- 238000001228 spectrum Methods 0.000 claims description 10
- 230000003595 spectral effect Effects 0.000 claims description 3
- 239000000203 mixture Substances 0.000 claims 1
- 238000001514 detection method Methods 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 7
- 238000004088 simulation Methods 0.000 description 4
- 230000021615 conjugation Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 238000004364 calculation method Methods 0.000 description 1
- 238000004891 communication Methods 0.000 description 1
- 238000012938 design process Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 230000004807 localization Effects 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 230000009897 systematic effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/02—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
- G01S3/14—Systems for determining direction or deviation from predetermined direction
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/78—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using electromagnetic waves other than radio waves
- G01S3/782—Systems for determining direction or deviation from predetermined direction
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/80—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using ultrasonic, sonic or infrasonic waves
- G01S3/802—Systems for determining direction or deviation from predetermined direction
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Electromagnetism (AREA)
- Variable-Direction Aerials And Aerial Arrays (AREA)
- Measurement Of Velocity Or Position Using Acoustic Or Ultrasonic Waves (AREA)
Abstract
本发明公开了一种基于虚拟阵列内插的无网格化互质阵列波达方向估计方法,主要解决现有技术中虚拟阵列的非均匀性所导致的信息损失问题。其实现步骤是:接收端架构互质阵列;利用互质阵列接收入射信号并建模;计算互质阵列接收信号所对应的等价虚拟信号;构造内插虚拟阵列并建模;构造内插虚拟阵列的多采样快拍信号及其采样协方差矩阵;构造投影矩阵并定义与该投影矩阵相关的投影运算;设计基于内插虚拟阵列信号协方差矩阵核范数最小化的优化问题并求解;根据重建的内插虚拟阵列协方差矩阵进行波达方向估计。本发明提高了波达方向估计的自由度及分辨率,可用于无源定位和目标探测。
The invention discloses a method for estimating the direction of arrival of a gridless coprime array based on virtual array interpolation, which mainly solves the problem of information loss caused by the non-uniformity of virtual arrays in the prior art. The implementation steps are: constructing a coprime array at the receiving end; using the coprime array to receive the incident signal and modeling; calculating the equivalent virtual signal corresponding to the signal received by the coprime array; constructing an interpolation virtual array and modeling; constructing an interpolation virtual array Multi-sampling snapshot signal of the array and its sampling covariance matrix; construct the projection matrix and define the projection operation related to the projection matrix; design and solve the optimization problem based on the minimization of the kernel norm of the interpolated virtual array signal covariance matrix; according to The reconstructed interpolated virtual array covariance matrix is used for DOA estimation. The invention improves the degree of freedom and resolution of the direction of arrival estimation, and can be used for passive positioning and target detection.
Description
技术领域technical field
本发明属于信号处理技术领域,尤其涉及对雷达信号、声学信号及电磁信号的波达方向估计,具体是一种基于虚拟阵列内插的无网格化互质阵列波达方向估计方法,可用于无源定位和目标探测。The invention belongs to the technical field of signal processing, in particular to the estimation of direction of arrival of radar signals, acoustic signals and electromagnetic signals, in particular to a method for estimation of direction of arrival of a gridless coprime array based on virtual array interpolation, which can be used for Passive localization and object detection.
背景技术Background technique
波达方向(Direction-of-Arrival,DOA)估计是阵列信号处理领域的一个重要分支,它是指利用阵列天线接收空域信号,并通过现代信号处理技术和各类优化方法实现对接收信号统计量的有效处理,从而实现信号的DOA估计,在雷达、声呐、语音、无线通信等领域有着重要的应用价值。Direction-of-Arrival (DOA) estimation is an important branch in the field of array signal processing. It can effectively process the signal to realize DOA estimation of the signal, which has important application value in the fields of radar, sonar, voice, wireless communication and so on.
DOA估计方法的自由度是指其能够估计的入射信号源的个数。现有的DOA估计方法通常采用均匀线性阵列进行信号的接收与建模,但是基于均匀线性阵列方法的自由度受限于实际天线阵元个数。具体而言,对于一个包含L个天线阵元的均匀线性阵列,其自由度为L-1。因此,当某个空域范围内入射信号源的个数大于或等于阵列中天线阵元的个数时,现有采用均匀线性阵列的方法将无法进行有效的DOA估计。The degree of freedom of the DOA estimation method refers to the number of incident signal sources it can estimate. The existing DOA estimation methods usually use uniform linear arrays for signal reception and modeling, but the degree of freedom of the methods based on uniform linear arrays is limited by the actual number of antenna elements. Specifically, for a uniform linear array containing L antenna elements, the degree of freedom is L-1. Therefore, when the number of incident signal sources in a certain spatial range is greater than or equal to the number of antenna elements in the array, the existing methods using uniform linear arrays cannot perform effective DOA estimation.
互质阵列能够在天线阵元个数一定的前提下增加DOA估计的自由度,因而受到了学术界的广泛关注。作为互质采样技术在空间域上的一个典型表现形式,互质阵列提供了一个系统化的稀疏阵列架构方案,并能够突破传统均匀线性阵列自由度受限的瓶颈,实现DOA估计方法自由度性能的提升。现有的基于互质阵列的DOA估计方法主要通过利用质数的性质将互质阵列推导到虚拟域,并形成等价虚拟均匀线性阵列接收信号以实现DOA估计。由于虚拟阵列中包含的虚拟阵元数大于实际的天线阵元数,自由度因此得到了有效的提升。但是由于从互质阵列推导而来的虚拟阵列属于非均匀阵列,因此很多现有基于均匀线性阵列的信号处理方法无法直接应用于虚拟阵列等价接收信号以实现有效的DOA估计。当前采用互质阵列的DOA估计方法常用的一个解决方案是,仅利用虚拟阵列中连续的阵元部分形成一个虚拟均匀线阵以进行DOA估计,但是这造成了部分原始信息的丢失和相关估计性能的降低。The coprime array can increase the DOA estimation degree of freedom under the premise of a certain number of antenna elements, so it has received extensive attention from the academic community. As a typical manifestation of coprime sampling technology in the spatial domain, coprime array provides a systematic sparse array architecture solution, and can break through the bottleneck of limited degrees of freedom of traditional uniform linear arrays and achieve DOA estimation method. improvement. The existing DOA estimation methods based on coprime arrays mainly derive the coprime arrays into the virtual domain by using the properties of prime numbers, and form an equivalent virtual uniform linear array to receive signals to achieve DOA estimation. Since the number of virtual array elements contained in the virtual array is larger than the actual number of antenna array elements, the degree of freedom is effectively improved. However, since the virtual array derived from the coprime array is a non-uniform array, many existing signal processing methods based on uniform linear arrays cannot be directly applied to the virtual array to equivalently receive signals to achieve effective DOA estimation. A commonly used solution for DOA estimation methods using coprime arrays is to use only the continuous elements in the virtual array to form a virtual uniform linear array for DOA estimation, but this results in the loss of part of the original information and the performance of correlation estimation. decrease.
同时,目前众多DOA估计方法在优化问题的设计过程中,需要预先设置信号假定波达方向的空间网格点。随着对波达方向估计结果精度要求的提高,这些DOA估计方法需要预先设置的空间网格点将变得越来越密集,这导致了计算复杂度的急剧增加。不仅如此,在实际情况中,难免会有一些信号的波达方向无法完全落在预先设置的网格点上,从而造成了固有的模型失配误差。At the same time, many DOA estimation methods currently need to pre-set the spatial grid points of the assumed direction of arrival of the signal in the design process of the optimization problem. With the improvement of the accuracy requirements for direction of arrival estimation results, the pre-set spatial grid points for these DOA estimation methods will become denser and denser, which leads to a sharp increase in computational complexity. Not only that, but in practical situations, it is inevitable that the direction of arrival of some signals cannot completely fall on the preset grid points, resulting in inherent model mismatch errors.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于针对上述现有技术存在的不足,提出一种基于虚拟阵列内插的无网格化互质阵列波达方向估计方法,充分利用了非均匀虚拟阵列所提供的全部信息,并保证了无网格化的波达方向估计,从而提高了DOA估计的自由度与分辨率,并在一定程度上降低了DOA估计的计算复杂度。The purpose of the present invention is to propose a method for estimating the direction of arrival of a gridless coprime array based on virtual array interpolation, which fully utilizes all the information provided by the non-uniform virtual array, and It ensures the estimation of direction of arrival without meshing, thereby improving the DOA estimation degree of freedom and resolution, and reducing the computational complexity of DOA estimation to a certain extent.
本发明的目的是通过以下技术方案来实现的:一种基于虚拟阵列内插的无网格化互质阵列波达方向估计方法,包含以下步骤:The object of the present invention is achieved through the following technical solutions: a method for estimating the direction of arrival of a gridless coprime array based on virtual array interpolation, comprising the following steps:
(1)接收端使用M+N-1个天线,并按照互质阵列结构进行架构;其中M与N为互质整数;(1) The receiving end uses M+N-1 antennas, and is structured according to the co-prime array structure; where M and N are co-prime integers;
(2)假设有K个来自θ1,θ2,…,θK方向的远场窄带非相干信号源,则(M+N-1)×1维互质阵列接收信号x(t)可建模为:(2) Assuming that there are K far-field narrow-band incoherent signal sources from the directions of θ 1 , θ 2 ,..., θ K , then the (M+N-1)×1-dimensional coprime array received signal x(t) can be constructed The model is:
其中,sk(t)为信号波形,n(t)为与各信号源相互独立的噪声分量,a(θk)为θk方向的导引矢量,表示为:Among them, sk (t) is the signal waveform, n(t) is the noise component independent of each signal source, a(θ k ) is the steering vector in the direction of θ k , expressed as:
其中,pid,i=1,2,…,M+N-1表示互质阵列中第i个物理天线阵元的实际位置,且p1=0;d为入射窄带信号波长λ的一半,即d=λ/2,[·]T表示转置操作。共采集T个采样快拍,得到互质阵列接收信号的采样协方差矩阵 Among them, p i d,i=1,2,...,M+N-1 represents the actual position of the i-th physical antenna element in the coprime array, and p 1 =0; d is half of the incident narrowband signal wavelength λ , that is, d=λ/2, [ ] T represents the transpose operation. A total of T sampling snapshots are collected to obtain the sampling covariance matrix of the received signal of the coprime array
这里,(·)H表示共轭转置操作;Here, ( ) H represents the conjugate transpose operation;
(3)计算互质阵列接收信号所对应的等价虚拟信号:矢量化互质阵列接收信号的采样协方差矩阵获得虚拟阵列等价接收信号v:(3) Calculate the equivalent virtual signal corresponding to the received signal of the coprime array: the sampling covariance matrix of the received signal of the vectorized coprime array Obtain the virtual array equivalent received signal v:
其中,为(M+N-1)2×K维虚拟阵列导引矩阵,包含K个入射信号源的功率,为噪声功率,iv=vec(IM+N-1)。这里,vec(·)表示矢量化操作,即把矩阵中的各列依次堆叠以形成一个新的矢量,(·)*表示共轭操作,表示克罗内克积,IM+N-1表示(M+N-1)×(M+N-1)维单位矩阵。矢量v对应的虚拟阵列中各虚拟阵元的位置为 in, is (M+N-1) 2 ×K-dimensional virtual array steering matrix, contains the power of the K incident signal sources, is the noise power, i v =vec( IM+N-1 ). Here, vec( ) represents the vectorization operation, that is, stacking the columns in the matrix to form a new vector, ( ) * represents the conjugation operation, Represents the Kronecker product, and IM+N-1 represents the (M+N-1)×(M+N-1) dimensional identity matrix. The position of each virtual array element in the virtual array corresponding to the vector v is
去除集合中重复的元素所对应位置上的重复虚拟阵元,得到一个非均匀的虚拟阵列其对应的等价虚拟信号vc可通过选取矢量v中相对应位置上的元素获得;remove set The repeated virtual array elements at the corresponding positions of the repeated elements in , get a non-uniform virtual array Its corresponding equivalent virtual signal v c can be obtained by selecting the element at the corresponding position in the vector v;
(4)构造内插虚拟阵列及其接收信号并建模:首先对于非均匀的虚拟阵列在保留其原有虚拟阵元位置不变的前提下,向其中非连续的位置插入若干虚拟阵元,从而将非均匀虚拟阵列转化为间距为d、阵列孔径与互质阵列相同、且虚拟阵元数目增加的均匀虚拟阵列该内插均匀虚拟阵列共包含个虚拟阵元,其中|·|表示集合的势,其对应的等价虚拟信号vI可通过往矢量vc中插入0获得,插入0的位置与中插入的虚拟阵元的位置相对应;(4) Construct an interpolated virtual array and its received signal and model it: First, for a non-uniform virtual array Under the premise of keeping the original position of the virtual array element unchanged, insert several virtual array elements into the non-consecutive positions, so that the non-uniform virtual array Converted to a uniform virtual array with a spacing of d, the array aperture is the same as that of a coprime array, and the number of virtual array elements is increased The interpolated uniform virtual array contains a total of virtual array elements, where |·| represents the potential of the set, and the corresponding equivalent virtual signal v I can be obtained by inserting 0 into the vector vc , and the position of inserting 0 is the same as The position of the virtual array element inserted in corresponds to;
(5)构造内插虚拟阵列多采样快拍信号及其采样协方差矩阵:将切割为LI个长度为LI的连续子阵列,其中(5) Construct the interpolated virtual array multi-sampling snapshot signal and its sampling covariance matrix: cut into L I contiguous subarrays of length L I , where
相应地,内插虚拟阵列的多采样快拍信号可通过截取矢量vI中对应的元素获得,即:vI,l,l=1,2,…,LI由vI中第LI+1-l到第2LI-l个元素组成。接着,VI的采样协方差矩阵Rv可以由如下方式得到:Correspondingly, interpolate the virtual array The multi-sampled snapshot signal of can be obtained by intercepting the corresponding elements in the vector v I , namely: v I,l ,l=1,2,...,L I consists of L I +1-1th to 2L I -1th elements in v I. Next, the sampling covariance matrix R v of VI can be obtained as follows:
其中,<vI>i表示位置为id的虚拟阵元所对应的等价接收信号;Wherein, <v I > i represents the equivalent received signal corresponding to the virtual array element whose position is id;
(6)构造投影矩阵并定义投影运算:投影矩阵P的维度与Rv相同,如果矩阵Rv中某个元素为0,则投影矩阵P中相同位置的元素值也为0;反之投影矩阵P中相应位置的元素值为1。定义为投影运算,其中括号内变量为与P维度相同的矩阵,投影运算通过变量矩阵中每一个元素与投影矩阵P中相应位置上的元素一一相乘实现,得到一个与矩阵P维度相同的矩阵;(6) Construct the projection matrix and define the projection operation: the dimension of the projection matrix P is the same as that of R v . If an element in the matrix R v is 0, the value of the element at the same position in the projection matrix P is also 0; otherwise, the projection matrix P The value of the element in the corresponding position is 1. definition It is the projection operation, in which the variable in parentheses is a matrix with the same dimension as P, and the projection operation is realized by multiplying each element in the variable matrix with the element at the corresponding position in the projection matrix P, and a matrix with the same dimension as the matrix P is obtained. ;
(7)设计基于内插虚拟阵列信号协方差矩阵核范数最小化的优化问题并求解。利用(5)得到的内插虚拟阵列协方差矩阵Rv作为参考值,寻找一个核范数最小的Toeplitz矩阵作为内插虚拟阵列信号的协方差矩阵,且要求其与Rv的差异小于某一阈值,可构建如下以矢量z为变量的优化问题:(7) Design and solve the optimization problem based on the minimization of the kernel norm of the interpolated virtual array signal covariance matrix. Using the interpolated virtual array covariance matrix R v obtained in (5) as a reference value, find a Toeplitz matrix with the smallest nuclear norm as the covariance matrix of the interpolated virtual array signal, and the difference between it and R v is required to be less than a certain Threshold, the following optimization problem with vector z as a variable can be constructed:
其中,表示的核范数,表示以矢量z为第一列的厄米特对称Toeplitz矩阵;∈为阈值常数,用于约束协方差矩阵的重建误差;保证了重建的协方差矩阵满足半正定的条件;‖·‖F表示Frobenius范数。求解上述凸优化问题可得到最优化值相应地,重建的Toeplitz矩阵为内插虚拟阵列协方差矩阵;in, express The nuclear norm of , represents the Hermitian symmetric Toeplitz matrix with the vector z as the first column; ∈ is the threshold constant, which is used to constrain the reconstruction error of the covariance matrix; It is guaranteed that the reconstructed covariance matrix satisfies the condition of positive semi-definite; ‖·‖ F represents the Frobenius norm. Solving the above convex optimization problem can get the optimal value Correspondingly, the reconstructed Toeplitz matrix is the interpolated virtual array covariance matrix;
(8)根据重建的内插虚拟阵列协方差矩阵进行波达方向估计。(8) According to the reconstructed interpolated virtual array covariance matrix Do direction of arrival estimation.
进一步地,步骤(1)所述的互质阵列结构可具体描述为:首先选取一对互质整数M、N;然后,构造一对稀疏均匀线性子阵列,其中第一个子阵列包含M个间距为Nd的天线阵元,其位置为0,Nd,…,(M-1)Nd,第二个子阵列包含N个间距为Md的天线阵元,其位置为0,Md,…,(N-1)Md;接着,将两个子阵列按照首个阵元重叠的方式进行子阵列组合,获得实际包含M+N-1个天线阵元的非均匀互质阵列架构。Further, the coprime array structure described in step (1) can be specifically described as: first select a pair of coprime integers M, N; then, construct a pair of sparse uniform linear subarrays, wherein the first subarray contains M The antenna array elements with spacing Nd are located at 0,Nd,…,(M-1)Nd, and the second sub-array contains N antenna elements with spacing Md, whose positions are 0,Md,…,(N -1) Md; then, the two sub-arrays are combined in a manner that the first array element overlaps to obtain a non-uniform co-prime array structure that actually contains M+N-1 antenna elements.
进一步地,步骤(5)所构建的VI的采样协方差矩阵Rv也可以由下述方法等价得到:Further, the sampling covariance matrix R v of VI constructed in step (5) can also be equivalently obtained by the following method:
进一步地,步骤(7)中的凸优化问题可转化为如下以矢量z为变量的优化问题:Further, the convex optimization problem in step (7) can be transformed into the following optimization problem with vector z as a variable:
其中μ为正则化参数,用于在最小化过程中权衡矩阵重建误差和z的核范数。where μ is the regularization parameter used to trade off the matrix during minimization Reconstruction error and kernel norm of z.
进一步地,步骤(8)中的波达方向估计,可采用以下方法:多重信号分类方法、旋转不变子空间方法、求根多重信号分类方法、协方差矩阵稀疏重建方法等。Further, the DOA estimation in step (8) may adopt the following methods: multiple signal classification method, rotation invariant subspace method, multiple signal classification method for root finding, covariance matrix sparse reconstruction method, etc.
进一步地,步骤8中,通过多重信号分类方法进行波达方向估计,具体为:画出虚拟域空间谱PMUSIC(θ):Further, in step 8, the direction of arrival is estimated by the multiple signal classification method, which is specifically: draw the virtual domain spatial spectrum P MUSIC (θ):
其中d(θ)是LI×1维内插虚拟阵列导引矢量,对应于位置为由0到(LI-1)d的一段虚拟均匀阵列;En是LI×(LI-K)维矩阵,表示内插虚拟阵列协方差矩阵的噪声子空间;θ是假定的信号波达方向;通过谱峰搜索寻找空间谱PMUSIC(θ)上的峰值,并将这些峰值所对应的响应值从大到小排列,取前K个峰值所对应的角度方向,即为波达方向估计结果。where d(θ) is the L I ×1-dimensional interpolation virtual array steering vector, corresponding to a segment of virtual uniform array from 0 to (L I -1)d; En is L I ×(L I -K ) dimension matrix, representing the interpolated virtual array covariance matrix θ is the assumed direction of arrival of the signal; find the peaks on the spatial spectrum P MUSIC (θ) through spectral peak search, and arrange the response values corresponding to these peaks from large to small, and take the first K peaks The corresponding angular direction is the result of DOA estimation.
本发明与现有技术相比具有以下优点:Compared with the prior art, the present invention has the following advantages:
(1)本发明在互质阵列等价虚拟域上引入了阵列内插的思想,充分利用了虚拟阵列提供的全部信息。通过在非均匀虚拟阵列中内插虚拟阵元的方式构建出均匀线性虚拟阵列,在保留了由原始非均匀虚拟阵列接收到的全部信息的同时,使得构建的虚拟域信号模型满足奈奎斯特采样定律;(1) The present invention introduces the idea of array interpolation in the equivalent virtual field of the coprime array, and makes full use of all the information provided by the virtual array. A uniform linear virtual array is constructed by interpolating virtual array elements in the non-uniform virtual array. While retaining all the information received by the original non-uniform virtual array, the constructed virtual domain signal model satisfies the Nyquist signal model. sampling law;
(2)本发明基于内插虚拟阵列信号协方差矩阵核范数最小化的思想设计优化问题,在优化问题设计的过程中无需预先定义空间网格点,实现了无网格化的波达方向估计,同时保证了波达方向估计的分辨率以及计算效率;(2) The present invention designs the optimization problem based on the idea of minimizing the kernel norm of the covariance matrix of the interpolated virtual array signal, and does not need to pre-define the space grid points in the process of designing the optimization problem, and realizes the direction of arrival without grids estimation, while ensuring the resolution and computational efficiency of DOA estimation;
(3)本发明所提出的基于内插虚拟阵列协方差矩阵重建的优化问题保证了优化求解结果为厄米特对称的Toeplitz矩阵,使得最优解与理论协方差矩阵之间的误差更小。由于均匀线性阵列非相干接收信号的理论协方差矩阵满足Toeplitz结构,因此利用它的Toeplitz特性作为先验约束条件进行协方差矩阵的重建,可以使得重建结果与真实值差异更小,从而提高DOA估计的性能。(3) The optimization problem based on the reconstruction of the interpolated virtual array covariance matrix proposed by the present invention ensures that the optimal solution result is a Hermitian symmetric Toeplitz matrix, so that the error between the optimal solution and the theoretical covariance matrix is smaller. Since the theoretical covariance matrix of the uniform linear array incoherent received signal satisfies the Toeplitz structure, the reconstruction of the covariance matrix using its Toeplitz characteristic as a prior constraint can make the difference between the reconstruction result and the real value smaller, thereby improving the DOA estimation performance.
附图说明Description of drawings
图1是本发明的方法总体流程框图。FIG. 1 is a block diagram showing the overall flow of the method of the present invention.
图2是本发明中组成互质阵列的一对稀疏均匀子阵列结构示意图。FIG. 2 is a schematic structural diagram of a pair of sparse uniform sub-arrays forming a coprime array in the present invention.
图3是本发明中互质阵列的结构示意图。FIG. 3 is a schematic structural diagram of a coprime array in the present invention.
图4是本发明中内插虚拟阵列的结构示意图。FIG. 4 is a schematic structural diagram of an interpolation virtual array in the present invention.
图5是本发明中内插虚拟阵列分割方法的示意图。FIG. 5 is a schematic diagram of a method for dividing an interpolation virtual array in the present invention.
图6是用于体现本发明所提方法自由度性能的空间功率谱示意图。FIG. 6 is a schematic diagram of the spatial power spectrum used to reflect the degree of freedom performance of the method proposed in the present invention.
图7是用于体现本发明所提方法分辨率性能的归一化空间谱示意图。FIG. 7 is a schematic diagram of a normalized spatial spectrum used to reflect the resolution performance of the method proposed in the present invention.
具体实施方式Detailed ways
以下参照附图,对本发明的技术方案和效果作进一步的详细说明。The technical solutions and effects of the present invention will be described in further detail below with reference to the accompanying drawings.
对于DOA估计在实际系统中的应用,互质阵列由于其可以通过等价虚拟阵列信号的计算和统计信号处理,突破物理阵元数量对自由度的限制而备受关注。但是受限于虚拟阵列的非均匀性,目前很多方法都会选择利用其中连续的虚拟阵元部分进行DOA估计,从而造成了信息损失。同时,很多方法在进行DOA估计之前会预先设置假定波达信号方向的空间网格点,这造成了固有失配误差以及计算复杂度与估计精度之间的矛盾。为了充分利用非均匀虚拟阵列中所包含的所有信息,并避免由于预定义空间网格点所造成的估计分辨率受限问题,本发明提供了一种基于虚拟阵列内插的无网格化互质阵列波达方向估计方法,参照图1,本发明的实现步骤如下:For the application of DOA estimation in practical systems, coprime arrays have attracted much attention because they can break through the limitation of the number of physical array elements on the degree of freedom through the calculation and statistical signal processing of equivalent virtual array signals. However, limited by the non-uniformity of virtual arrays, many methods currently choose to use continuous virtual array elements for DOA estimation, resulting in information loss. At the same time, many methods pre-set the spatial grid points of the assumed direction of arrival signal before performing DOA estimation, which causes inherent mismatch errors and conflicts between computational complexity and estimation accuracy. In order to make full use of all the information contained in the non-uniform virtual array and avoid the problem of limited estimation resolution caused by the predefined spatial grid points, the present invention provides a gridless interactive grid based virtual array interpolation. The method for estimating the direction of arrival of the mass array, referring to FIG. 1, the implementation steps of the present invention are as follows:
步骤一:在接收端使用M+N-1个天线阵元架构互质阵列;首先,选取一组互质整数M、N;然后,参照图2,构造一对稀疏均匀线性子阵列,其中第一个子阵列包含M个间距为Nd的天线阵元,其位置为0,Nd,…,(M-1)Nd;第二个子阵列包含N个间距为Md的天线阵元,其位置为0,Md,…,(N-1)Md;单位间距d取为入射窄带信号波长的一半,即d=λ/2;接着,将两个子阵列的首个天线阵元视为参考阵元,参照图3,将两个子阵的参考阵元重叠以实现子阵列组合,获得实际包含M+N-1个天线阵元的非均匀互质阵列架构。Step 1: use M+N-1 antenna array elements at the receiving end to construct a coprime array; first, select a set of coprime integers M and N; then, referring to Figure 2, construct a pair of sparse uniform linear sub-arrays, in which the first One sub-array contains M antenna elements with a spacing of Nd, and their positions are 0, Nd,..., (M-1)Nd; the second sub-array contains N antenna elements with a spacing of Md, and their positions are 0 ,Md,...,(N-1)Md; the unit spacing d is taken as half of the wavelength of the incident narrowband signal, that is, d=λ/2; then, the first antenna element of the two sub-arrays is regarded as the reference array element, refer to In Fig. 3, the reference array elements of the two sub-arrays are overlapped to realize the sub-array combination, and a non-uniform co-prime array structure actually containing M+N-1 antenna array elements is obtained.
步骤二:采用互质阵列接收信号并建模。假设有K个来自θ1,θ2,…,θK方向的远场窄带非相干信号源,采用步骤一架构的非均匀互质阵列接收入射信号,得到(M+N-1)×1维互质阵列接收信号x(t),可建模为:Step 2: Use a coprime array to receive the signal and model it. Assuming that there are K far-field narrow-band incoherent signal sources from the directions of θ 1 , θ 2 ,..., θ K , the non-uniform coprime array with the structure of step 1 is used to receive the incident signal, and the (M+N-1)×1 dimension is obtained. The coprime array receives the signal x(t), which can be modeled as:
其中,sk(t)为信号波形,n(t)为与各信号源相互独立的噪声分量,a(θk)为θk方向的互质阵列导引矢量,表示为Among them, sk (t) is the signal waveform, n(t) is the noise component independent of each signal source, a(θ k ) is the coprime array steering vector in the direction of θ k , expressed as
其中,pid,i=1,2,…,M+N-1表示互质阵列中第i个物理天线阵元的实际位置,且p1=0;d为入射窄带信号波长λ的一半,即d=λ/2,[·]T表示转置操作。共采集T个采样快拍,得到互质阵列接收信号的采样协方差矩阵 Among them, p i d,i=1,2,...,M+N-1 represents the actual position of the i-th physical antenna element in the coprime array, and p 1 =0; d is half of the incident narrowband signal wavelength λ , that is, d=λ/2, [ ] T represents the transpose operation. A total of T sampling snapshots are collected to obtain the sampling covariance matrix of the received signal of the coprime array
其中,(·)H表示共轭转置操作。where (·) H represents the conjugate transpose operation.
步骤三:计算互质阵列接收信号所对应的等价虚拟信号。矢量化互质阵列接收信号的采样协方差矩阵获得虚拟阵列等价接收信号v:Step 3: Calculate the equivalent virtual signal corresponding to the signal received by the coprime array. Sampling Covariance Matrix of Received Signals of Vectorized Coprime Array Obtain the virtual array equivalent received signal v:
其中,为(M+N-1)2×K维虚拟阵列导引矩阵,包含K个入射信号源的功率,为噪声功率,iv=vec(IM+N-1)。这里,vec(·)表示矢量化操作,即把矩阵中的各列依次堆叠以形成一个新的矢量,(·)*表示共轭操作,表示克罗内克积,IM+N-1表示(M+N-1)×(M+N-1)维单位矩阵。矢量v对应的虚拟阵列中各虚拟阵元的位置为其中in, is (M+N-1) 2 ×K-dimensional virtual array steering matrix, contains the power of the K incident signal sources, is the noise power, i v =vec( IM+N-1 ). Here, vec( ) represents the vectorization operation, that is, stacking the columns in the matrix to form a new vector, ( ) * represents the conjugation operation, Represents the Kronecker product, and IM+N-1 represents the (M+N-1)×(M+N-1) dimensional identity matrix. The position of each virtual array element in the virtual array corresponding to the vector v is in
去除集合中重复的元素所对应位置上的重复虚拟阵元,得到一个非均匀的虚拟阵列其对应的等价虚拟信号vc可通过选取矢量v中相对应位置上的元素获得。remove set The repeated virtual array elements at the corresponding positions of the repeated elements in , get a non-uniform virtual array Its corresponding equivalent virtual signal v c can be obtained by selecting elements at corresponding positions in the vector v.
步骤四:构造内插虚拟阵列及其接收信号建模。参照图4,对于非均匀的虚拟阵列在保留其原有虚拟阵元位置不变的前提下,向其中存在孔洞的位置插入若干虚拟阵元(如图4中的空心圆所示),从而将非均匀虚拟阵列转化为间距为d、阵列孔径与互质阵列相同、且虚拟阵元数目增加的均匀虚拟阵列内插虚拟阵列共包含个虚拟阵元,其中|·|表示集合的势。内插虚拟阵列对应的等价虚拟信号vI可通过往矢量vc中孔洞的相应位置填入0获得。Step 4: Construct the interpolation virtual array and its received signal modeling. Referring to Figure 4, for a non-uniform virtual array Under the premise of keeping the original position of the virtual array element unchanged, insert several virtual array elements (as shown by the hollow circle in Fig. Converted to a uniform virtual array with a spacing of d, the array aperture is the same as that of a coprime array, and the number of virtual array elements is increased The interpolated virtual array contains a total of virtual array elements, where |·| represents the potential of the set. The equivalent virtual signal v I corresponding to the interpolated virtual array can be obtained by filling the corresponding positions of the holes in the vector vc with 0.
步骤五:构造内插虚拟阵列多采样快拍信号及其采样协方差矩阵。参照图5,将内插虚拟阵列切割为LI个长度为LI的连续子阵列,其中Step 5: Construct an interpolated virtual array multi-sampling snapshot signal and its sampling covariance matrix. Referring to Figure 5, the virtual array will be interpolated cut into L I contiguous subarrays of length L I , where
由于中的虚拟阵元以零位对称分布,始终为奇数,故LI为整数。相应地,内插虚拟阵列的多采样快拍信号可通过截取矢量vI中对应的元素获得,即:VI=[vI,1,vI,2,…,vI,LI],其中vI,l,l=1,2,…,LI由vI中第LI+1-l到第2LI-l个元素组成。接着,VI的采样协方差矩阵Rv可以由如下方式得到:because The virtual array elements in are symmetrically distributed with zero positions, is always odd, so L I is an integer. Correspondingly, interpolate the virtual array The multi-sampling snapshot signal can be obtained by intercepting the corresponding elements in the vector v I , namely: V I =[v I,1 ,v I,2 ,...,v I,LI ], where v I,l ,l= 1,2,...,L I consists of L I +1-1th to 2L I -1th elements in v I. Next, the sampling covariance matrix R v of VI can be obtained as follows:
其中,〈vI〉i表示位置为id的虚拟阵元所对应的等价接收信号。由于内插虚拟阵列中虚拟阵元关于零位对称分布,因此其上的等价虚拟接收信号对应于零位呈共轭关系,所以上述采样协方差矩阵也可以通过如下方式等价得到:Wherein, <v I > i represents the equivalent received signal corresponding to the virtual array element whose position is id. Since the virtual array elements in the interpolated virtual array are symmetrically distributed with respect to the null position, the equivalent virtual received signal on it is in a conjugate relationship with the null position, so the above sampling covariance matrix can also be equivalently obtained in the following way:
步骤六:构造投影矩阵并定义投影运算。由于步骤五所得的协方差矩阵Rv中包含有在步骤四中插入的0,因此其相应位置对角线上的元素全部为0。根据这样的结构定义一个与Rv维度相同的投影矩阵P,如果Rv中某一位置上的元素是0,则投影矩阵P中相同位置的元素值也为0;反之则投影矩阵P中相应位置的元素值为1。定义为投影运算,其中括号内变量为与P维度相同的矩阵,投影运算通过变量矩阵的每一个元素与投影矩阵P中相应位置上的元素一一相乘实现,得到一个与矩阵P维度相同的矩阵。Step 6: Construct the projection matrix and define the projection operation. Since the covariance matrix R v obtained in step 5 contains 0 inserted in step 4, all the elements on the diagonal line of its corresponding position are 0. According to such a structure, a projection matrix P with the same dimension as R v is defined. If an element at a certain position in R v is 0, the value of the element at the same position in the projection matrix P is also 0; otherwise, the corresponding element in the projection matrix P is 0. The element value of position is 1. definition It is the projection operation, where the variable in the parentheses is a matrix with the same dimension as P, and the projection operation is realized by multiplying each element of the variable matrix with the element at the corresponding position in the projection matrix P, and a matrix with the same dimension as the matrix P is obtained. .
步骤七:设计基于内插虚拟阵列信号协方差矩阵核范数最小化的优化问题并求解。利用步骤五得到的内插虚拟阵列协方差矩阵Rv作为参考值,寻找一个核范数最小的Toeplitz矩阵作为内插虚拟阵列信号的协方差矩阵,且要求其与Rv的差异小于某一阈值,可构建如下以矢量z为变量的优化问题:Step 7: Design and solve the optimization problem based on the minimization of the kernel norm of the interpolated virtual array signal covariance matrix. Using the interpolated virtual array covariance matrix R v obtained in step 5 as a reference value, find a Toeplitz matrix with the smallest nuclear norm as the covariance matrix of the interpolated virtual array signal, and the difference between it and R v is required to be less than a certain threshold , the optimization problem with the vector z as a variable can be constructed as follows:
其中,表示的核范数,表示以矢量z为第一列的厄米特对称Toeplitz矩阵;∈为阈值常数,用于约束协方差矩阵的重建误差;保证了重建的协方差矩阵满足半正定的条件;‖·‖F表示Frobenius范数。求解上述凸优化问题可得到最优化值上述凸优化问题可转化为以下以矢量z为变量的优化问题:in, express The nuclear norm of , represents the Hermitian symmetric Toeplitz matrix with the vector z as the first column; ∈ is the threshold constant, which is used to constrain the reconstruction error of the covariance matrix; It is guaranteed that the reconstructed covariance matrix satisfies the condition of positive semi-definite; ‖·‖ F represents the Frobenius norm. Solving the above convex optimization problem can get the optimal value The above convex optimization problem can be transformed into the following optimization problem with the vector z as a variable:
其中μ为正则化参数,用于在最小化过程中权衡矩阵重建误差和z的核范数。求解上述凸优化问题可得到最优化值相应地,重建的Toeplitz矩阵为内插虚拟阵列协方差矩阵。where μ is the regularization parameter used to trade off the matrix during minimization Reconstruction error and kernel norm of z. Solving the above convex optimization problem can get the optimal value Correspondingly, the reconstructed Toeplitz matrix is the interpolated virtual array covariance matrix.
步骤八:根据重建的内插虚拟阵列协方差矩阵进行波达方向估计。通过引入经典的方法,如多重信号分类方法、旋转不变子空间方法、求根多重信号分类方法、协方差矩阵稀疏重建方法等对重建的内插虚拟阵列协方差矩阵进行操作,可以求得波达方向估计结果。以多重信号分类方法为例,画出虚拟域空间谱PMUSIC(θ):Step 8: According to the reconstructed interpolated virtual array covariance matrix Do direction of arrival estimation. By introducing classical methods, such as multiple signal classification method, rotation invariant subspace method, root multiple signal classification method, covariance matrix sparse reconstruction method, etc., the reconstructed interpolated virtual array covariance matrix By performing the operation, the DOA estimation result can be obtained. Taking the multiple signal classification method as an example, draw the virtual domain spatial spectrum P MUSIC (θ):
其中d(θ)是LI×1维内插虚拟阵列导引矢量,对应于位置为由0到(LI-1)d的一段虚拟均匀阵列;En是LI×(LI-K)维矩阵,表示内插虚拟阵列协方差矩阵的噪声子空间;θ是假定的信号波达方向;通过谱峰搜索寻找空间谱PMUSIC上的峰值,并将这些峰值所对应的响应值从大到小排列,取前K个峰值所对应的角度方向,即为波达方向估计结果。where d(θ) is the L I ×1-dimensional interpolation virtual array steering vector, corresponding to a segment of virtual uniform array from 0 to (L I -1)d; En is L I ×(L I -K ) dimension matrix, representing the interpolated virtual array covariance matrix θ is the assumed direction of arrival of the signal; find the peaks on the spatial spectrum P MUSIC through spectral peak search, and arrange the response values corresponding to these peaks from large to small, and take the corresponding values of the first K peaks. The angular direction is the result of DOA estimation.
本发明一方面引入虚拟阵列内插的思想,在推导的原始虚拟阵列基础上内插入虚拟阵元,从而将原始的非均匀虚拟阵列转化为虚拟均匀阵列,同时保留了原始非均匀虚拟阵列上的所有信息,避免了因原始虚拟阵列的非均匀性所导致的统计信号处理模型失配及传统方法截取虚拟均匀子阵所导致的信息损失问题;另一方面,引入了基于虚拟阵列信号协方差矩阵核范数最小化的思想来设计优化问题,以重建内插虚拟阵列的协方差矩阵,实现了虚拟域上的无网格化波达方向估计。On the one hand, the present invention introduces the idea of virtual array interpolation, and inserts virtual array elements on the basis of the derived original virtual array, thereby converting the original non-uniform virtual array into a virtual uniform array, while retaining the original non-uniform virtual array. All information avoids the mismatch of statistical signal processing models caused by the non-uniformity of the original virtual array and the information loss problem caused by the traditional method of intercepting the virtual uniform sub-array; on the other hand, the signal covariance matrix based on the virtual array is introduced. The idea of kernel norm minimization is used to design the optimization problem to reconstruct the covariance matrix of the interpolated virtual array, and realize the meshless DOA estimation on the virtual domain.
下面结合仿真实例对本发明的效果做进一步的描述。The effect of the present invention will be further described below in conjunction with a simulation example.
仿真实例1:采用互质阵列接收入射信号,其参数选取为M=3,N=5,即架构的互质阵列共包含M+N-1=7个物理阵元。假定入射窄带信号个数为9,且入射方向均匀分布于-50°至50°这一空间角度域范围内;信噪比设置为30dB,采样快拍数T=500;正则化参数μ设置为0.25。Simulation example 1: The co-prime array is used to receive the incident signal, and its parameters are selected as M=3, N=5, that is, the co-prime array of the architecture includes M+N-1=7 physical array elements. Assume that the number of incident narrowband signals is 9, and the incident direction is uniformly distributed in the spatial angle domain of -50° to 50°; the signal-to-noise ratio is set to 30dB, the number of sampling snapshots is T=500; the regularization parameter μ is set to 0.25.
本发明所提出的基于虚拟阵列内插的无网格化互质阵列波达方向估计方法空间功率谱如图6所示,其中垂直虚线代表入射信号源的实际方向。可以看出,本发明所提方法能够有效分辨这9个入射信号源。而对于传统采用均匀线性阵列的方法,利用7个物理天线阵元最多只能分辨6个入射信号,以上结果体现了本发明所提方法实现了自由度的增加。The spatial power spectrum of the method for estimating the direction of arrival of a gridless coprime array based on virtual array interpolation proposed by the present invention is shown in FIG. 6 , where the vertical dotted line represents the actual direction of the incident signal source. It can be seen that the method proposed in the present invention can effectively distinguish the nine incident signal sources. For the traditional method using a uniform linear array, only 6 incident signals can be resolved by using 7 physical antenna elements. The above results show that the method proposed in the present invention achieves an increase in the degree of freedom.
仿真实例2:采用互质阵列接收入射信号,其参数同样选取为M=3,N=5,即架构的互质阵列共包含M+N-1=7个物理天线阵元;假定入射窄带信号个数为2,且入射方向为-0.5°至0.5°,其余参数设置与仿真实例1保持一致。由图7所示的归一化空间谱可以看出,本发明所提方法可以有效地分辨出这两个近距离信号的波达方向,说明了本方法良好的分辨率性能。Simulation example 2: The co-prime array is used to receive the incident signal, and its parameters are also selected as M=3, N=5, that is, the co-prime array of the architecture contains M+N-1=7 physical antenna elements in total; it is assumed that the incident narrowband signal The number is 2, and the incident direction is -0.5° to 0.5°. The rest of the parameter settings are the same as those of simulation example 1. It can be seen from the normalized spatial spectrum shown in FIG. 7 that the method proposed in the present invention can effectively distinguish the directions of arrival of the two short-range signals, which shows the good resolution performance of the method.
综上所述,本发明所提方法充分利用了非均匀虚拟阵列上的全部信息,能够在信号源个数大于等于物理天线个数的情况下实现入射信号的无网格化估计,增加了DOA估计的自由度和分辨率。此外,与传统采用均匀线性阵列的方法相比,本发明所提方法在实际应用中所需的物理天线阵元及射频模块也能够相应减少,体现了经济性和高效性。To sum up, the method proposed in the present invention makes full use of all the information on the non-uniform virtual array, and can realize the grid-free estimation of the incident signal when the number of signal sources is greater than or equal to the number of physical antennas, and the DOA is increased. Estimated degrees of freedom and resolution. In addition, compared with the traditional method using uniform linear array, the physical antenna array elements and radio frequency modules required in practical application of the method proposed by the present invention can also be correspondingly reduced, which reflects economy and high efficiency.
Claims (6)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710302902.4A CN107102291B (en) | 2017-05-03 | 2017-05-03 | The relatively prime array Wave arrival direction estimating method of mesh freeization based on virtual array interpolation |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710302902.4A CN107102291B (en) | 2017-05-03 | 2017-05-03 | The relatively prime array Wave arrival direction estimating method of mesh freeization based on virtual array interpolation |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107102291A CN107102291A (en) | 2017-08-29 |
CN107102291B true CN107102291B (en) | 2019-07-23 |
Family
ID=59657497
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201710302902.4A Active CN107102291B (en) | 2017-05-03 | 2017-05-03 | The relatively prime array Wave arrival direction estimating method of mesh freeization based on virtual array interpolation |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107102291B (en) |
Families Citing this family (30)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP7023565B2 (en) * | 2017-10-06 | 2022-02-22 | 日本無線株式会社 | Array antenna device |
CN107907852B (en) * | 2017-10-27 | 2021-08-03 | 大连大学 | Covariance Matrix Rank Minimization DOA Estimation Method Based on Spatial Smoothing |
CN107870315B (en) * | 2017-11-06 | 2021-07-30 | 重庆邮电大学 | A Method for Estimating Direction of Arrival Arbitrary Array Using Iterative Phase Compensation Technique |
CN109239649B (en) * | 2018-04-04 | 2023-02-10 | 中国人民解放军空军预警学院 | Novel co-prime array DOA estimation method under array error condition |
CN108872929B (en) * | 2018-04-12 | 2021-03-23 | 浙江大学 | Estimation method for direction of arrival of co-prime array based on rotation invariance of covariance matrix subspace of interpolated virtual array |
CN108922553B (en) * | 2018-07-19 | 2020-10-09 | 苏州思必驰信息科技有限公司 | Direction-of-arrival estimation method and system for sound box equipment |
CN109061555B (en) * | 2018-08-27 | 2022-10-11 | 电子科技大学 | Mixed coherent DOA estimation method under nested array |
CN109375152B (en) * | 2018-09-05 | 2020-08-07 | 南京航空航天大学 | Low-complexity DOA and Polarization Joint Estimation Method for Electromagnetic Vector Nested L-Arrays |
CN109471086B (en) * | 2018-10-18 | 2020-11-24 | 浙江大学 | Coprime MIMO Radar Direction of Arrival Estimation Method Based on Multi-Sampling Snapshots and Discrete Fourier Transform of Set Array Signals |
CN109507636B (en) * | 2018-11-16 | 2022-08-16 | 南京邮电大学 | Direction-of-arrival estimation method based on virtual domain signal reconstruction |
CN109557503B (en) * | 2018-12-19 | 2023-03-14 | 成都理工大学 | MIMO (multiple input multiple output) co-prime array DOA (direction of arrival) estimation method based on correlation matrix reconstruction decorrelation |
CN109444810B (en) * | 2018-12-24 | 2022-11-01 | 哈尔滨工程大学 | Mutual-prime array non-grid DOA estimation method under nonnegative sparse Bayesian learning framework |
CN109901101A (en) * | 2019-02-25 | 2019-06-18 | 西安电子科技大学 | Method of Arrival Angle Estimation of Coherent Signals Based on Coprime Array of Electromagnetic Vector Sensors |
CN110412535B (en) * | 2019-08-10 | 2021-08-03 | 浙江大学 | A Sequential Space-Time Adaptive Processing Parameter Estimation Method |
JP7044290B2 (en) | 2020-05-03 | 2022-03-30 | 浙江大学 | A method for estimating the two-dimensional arrival direction of disjoint area arrays based on the processing of tensor signals in a structured virtual domain. |
CN111665468B (en) | 2020-06-08 | 2022-12-02 | 浙江大学 | Estimation method of direction of arrival of co-prime array based on single-bit quantized signal virtual domain statistic reconstruction |
CN111983553B (en) * | 2020-08-20 | 2024-02-20 | 上海无线电设备研究所 | Gridless DOA estimation method based on cross-prime multi-carrier-frequency sparse array |
CN112285642B (en) * | 2020-09-22 | 2023-09-29 | 华南理工大学 | Signal arrival direction estimation method for non-overlapping optimized mutual mass array |
CN112305495B (en) * | 2020-10-22 | 2023-10-13 | 南昌工程学院 | Method for reconstructing covariance matrix of cross matrix based on atomic norm minimum |
CN112505675B (en) * | 2021-02-08 | 2021-06-08 | 网络通信与安全紫金山实验室 | Target angle and distance positioning method and device, radar and storage medium |
CN113093093B (en) * | 2021-04-07 | 2023-08-18 | 南京邮电大学 | Vehicle positioning method based on linear array direction of arrival estimation |
CN113820655A (en) * | 2021-09-18 | 2021-12-21 | 宜宾电子科技大学研究院 | A DOA Estimation Method of Coprime Array Coherent Signal Based on Toeplitz Matrix Reconstruction and Matrix Filling |
CN114019446B (en) * | 2021-10-19 | 2024-04-12 | 南京航空航天大学 | Inter-quality coherent information source estimation method based on denoising kernel norm minimization |
CN114371440B (en) * | 2022-01-14 | 2025-01-03 | 天津大学 | DOA estimation method for coprime arrays based on information geometry |
CN114444298B (en) * | 2022-01-21 | 2024-12-17 | 浙江大学 | Virtual domain tensor filling-based mutual mass array two-dimensional direction-of-arrival estimation method |
CN114624647B (en) * | 2022-03-18 | 2024-06-07 | 北京航空航天大学 | A virtual array DOA estimation method based on backward selection |
CN114879131B (en) * | 2022-03-24 | 2024-07-16 | 西安电子科技大学 | Gridless DOA estimation method combining sparse linear array with interpolation virtual transformation technology |
CN115236586B (en) * | 2022-06-30 | 2023-04-18 | 哈尔滨工程大学 | Polar region under-ice DOA estimation method based on data preprocessing |
CN115236588B (en) * | 2022-07-27 | 2024-10-01 | 电子科技大学 | Mixed resolution quantization-based method for estimating arrival direction of reciprocal array |
CN115438604B (en) * | 2022-11-08 | 2023-03-24 | 中国空气动力研究与发展中心计算空气动力研究所 | Grid identification method based on prime number system |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105182293A (en) * | 2015-08-25 | 2015-12-23 | 西安电子科技大学 | Method for estimating DOA and DOD of MIMO radar based on co-prime array |
CN106324558A (en) * | 2016-08-30 | 2017-01-11 | 东北大学秦皇岛分校 | Broadband signal DOA estimation method based on co-prime array |
CN106569171A (en) * | 2016-11-08 | 2017-04-19 | 西安电子科技大学 | Dual-layer-hybrid-array-based estimation method for direction angle of arrival |
Family Cites Families (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US10054666B2 (en) * | 2014-09-26 | 2018-08-21 | The United States Of America, As Represented By The Secretary Of The Navy | Sparse space-time adaptive array architecture |
-
2017
- 2017-05-03 CN CN201710302902.4A patent/CN107102291B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN105182293A (en) * | 2015-08-25 | 2015-12-23 | 西安电子科技大学 | Method for estimating DOA and DOD of MIMO radar based on co-prime array |
CN106324558A (en) * | 2016-08-30 | 2017-01-11 | 东北大学秦皇岛分校 | Broadband signal DOA estimation method based on co-prime array |
CN106569171A (en) * | 2016-11-08 | 2017-04-19 | 西安电子科技大学 | Dual-layer-hybrid-array-based estimation method for direction angle of arrival |
Non-Patent Citations (2)
Title |
---|
A Grid-Less Approach to Underdetermined Direction of Arrival Estimation Via Low Rank Matrix Denoising;Piya Pal,et al;《IEEE SIGNAL PROCESSING LETTERS》;20140630;第21卷(第6期);p737-741 |
Coprime Coarray Interpolation for DOA Estimation via Nuclear Norm Minimization;Chun-Lin Liu,et al;《IEEE》;20161231;p2639-2642 |
Also Published As
Publication number | Publication date |
---|---|
CN107102291A (en) | 2017-08-29 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN107102291B (en) | The relatively prime array Wave arrival direction estimating method of mesh freeization based on virtual array interpolation | |
CN107315160B (en) | Estimation method of coprime array direction of arrival based on minimization of atomic norm of interpolated virtual array signal | |
CN107329108B (en) | The relatively prime array Wave arrival direction estimating method rebuild based on interpolation virtual array covariance matrix Toeplitzization | |
CN108872929B (en) | Estimation method for direction of arrival of co-prime array based on rotation invariance of covariance matrix subspace of interpolated virtual array | |
CN107092004B (en) | Direction of Arrival Estimation Method for Coprime Array Based on Rotation Invariance of Signal Subspace | |
CN106324558B (en) | DOA Estimation Method for Wideband Signal Based on Coprime Array | |
CN107290709B (en) | Direction of Arrival Estimation Method for Coprime Array Based on Vandermonde Decomposition | |
CN107329110B (en) | Direction of Arrival Estimation Method Based on Sparse Array Direct Interpolation | |
CN107037392B (en) | Degree-of-freedom increased type co-prime array direction-of-arrival estimation method based on compressed sensing | |
CN107015190A (en) | Relatively prime array Wave arrival direction estimating method based on the sparse reconstruction of virtual array covariance matrix | |
CN108896954B (en) | Estimation method of angle of arrival based on joint real-value subspace in co-prime matrix | |
CN110850359B (en) | An Underdetermined Direction Finding Method for Coprime Matrix Based on Atomic Norm | |
CN107589399B (en) | A method for estimation of direction of arrival of coprime array based on singular value decomposition of multi-sampled virtual signal | |
CN107561484B (en) | Direction-of-arrival estimation method based on interpolation co-prime array covariance matrix reconstruction | |
CN106972882B (en) | Coprime Array Adaptive Beamforming Method Based on Virtual Domain Spatial Power Spectrum Estimation | |
CN110082708B (en) | Non-Uniform Array Design and Direction of Arrival Estimation Method | |
CN111610486B (en) | High-resolution accurate two-dimensional direction of arrival estimation method based on planar co-prime array virtual domain tensor spatial spectrum search | |
CN107104720B (en) | Mutual-prime array self-adaptive beam forming method based on covariance matrix virtual domain discretization reconstruction | |
CN105974358A (en) | Compression-sensing-based DOA estimation method for intelligent antenna | |
CN110297209B (en) | A Two-Dimensional Direction of Arrival Estimation Method Based on Spatiotemporal Expansion of Parallel Coprime Arrays | |
WO2021068496A1 (en) | Co-prime array two-dimensional direction of arrival estimation method based on structured virtual domain tensor signal processing | |
CN113567913B (en) | Two-dimensional planar DOA estimation method based on iterative reweighting for dimensionality reduction | |
CN115236589B (en) | Polar region under-ice DOA estimation method based on covariance matrix correction | |
CN108614234B (en) | Direction of Arrival Estimation Method Based on Inverse Fast Fourier Transform of Received Signals from Multi-Sampling Snapshot Coprime Arrays | |
CN109471087B (en) | Direction-of-arrival estimation method based on co-prime MIMO radar difference set and signal collection fast Fourier transform |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant |