[go: up one dir, main page]
More Web Proxy on the site http://driver.im/

CN112379327A - Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation - Google Patents

Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation Download PDF

Info

Publication number
CN112379327A
CN112379327A CN202011381435.7A CN202011381435A CN112379327A CN 112379327 A CN112379327 A CN 112379327A CN 202011381435 A CN202011381435 A CN 202011381435A CN 112379327 A CN112379327 A CN 112379327A
Authority
CN
China
Prior art keywords
matrix
mutual coupling
estimation
array
vector
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.)
Pending
Application number
CN202011381435.7A
Other languages
Chinese (zh)
Inventor
窦慧晶
杨帆
肖子恒
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Beijing University of Technology
Original Assignee
Beijing University of Technology
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Beijing University of Technology filed Critical Beijing University of Technology
Priority to CN202011381435.7A priority Critical patent/CN112379327A/en
Publication of CN112379327A publication Critical patent/CN112379327A/en
Pending legal-status Critical Current

Links

Images

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO 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
    • G01S3/00Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
    • G01S3/02Direction-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
    • G01S3/14Systems 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)
  • Variable-Direction Aerials And Aerial Arrays (AREA)

Abstract

The invention discloses a two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation, and belongs to the technical field of array signal processing. Firstly, constructing a signal receiving model of a uniform planar antenna array under a mutual coupling error by constructing a mutual coupling error matrix; then, separating the information source data from the cross-coupling error vector by using a transform domain relation of parameter mapping, and constructing a corresponding spectral peak search function by using a rank loss estimation criterion to realize the estimation of the two-dimensional orientation parameters; and finally, constructing a decoupling matrix by using the obtained estimated orientation parameters to realize the estimation of the mutual coupling matrix, and further carrying out mutual coupling correction according to the estimation. On the basis, the estimation result of the method is verified by using proper simulation, and compared with the existing estimation algorithm, the DOA estimation result of the method has smaller root mean square error and higher estimation success rate, which indicates that the method has better performance.

Description

一种基于秩损估计的二维DOA估计与互耦校正方法A 2D DOA Estimation and Mutual Coupling Correction Method Based on Rank Loss Estimation

技术领域technical field

本发明涉及阵列信号处理相关领域,可以应用于无线通信、雷达定位等方面,尤其适用于解决天线阵列存在互耦误差条件下的二维DOA估计及互耦校正的问题。The invention relates to the related field of array signal processing, can be applied to wireless communication, radar positioning and the like, and is especially suitable for solving the problems of two-dimensional DOA estimation and mutual coupling correction under the condition of mutual coupling error of antenna array.

背景技术Background technique

阵列信号处理一直以来都是众多学者研究的热点方向之一,由于其在卫星通信、雷达探测、水下定位等方面有着众多的应用,故与此相关的的技术近年来得到了广泛而快速的发展。阵列信号处理的目的是对阵列接收到的数据进行采样,进而通过分析算法进行计算,从而得到期望信号的参数信息。Array signal processing has always been one of the hot research directions of many scholars. Because of its many applications in satellite communication, radar detection, underwater positioning, etc., related technologies have been widely and rapidly developed in recent years. . The purpose of the array signal processing is to sample the data received by the array, and then perform the calculation through the analysis algorithm, so as to obtain the parameter information of the desired signal.

波达方向(DOA)估计是阵列信号处理的一个重要分支。DOA估计的主要目的是为了判断空间内位于某个区域的多个感兴趣的信号的空间位置,也就是各个信号到达阵列参考阵元的方位角和俯仰角。由于二维DOA估计可以在三维空间中的信源位置进行估计,符合实际工程的要求,故而得到了众多学者的广泛研究。二维MUSIC算法是一种典型的二维DOA估计算法,该算法可以实现对二维角度的渐进无偏估计,但其实现过程需要进行二维空间的谱峰搜索,导致计算量过高。后续有学者研究将ESPRIT算法应用到二维DOA估计算法中,这种算法不需要谱峰搜索,所以计算量较小,具有较高的应用价值。Direction of arrival (DOA) estimation is an important branch of array signal processing. The main purpose of DOA estimation is to determine the spatial position of multiple signals of interest located in a certain area in space, that is, the azimuth and elevation angles of each signal reaching the reference array element of the array. Because two-dimensional DOA estimation can estimate the source position in three-dimensional space, which meets the requirements of practical engineering, it has been widely studied by many scholars. The two-dimensional MUSIC algorithm is a typical two-dimensional DOA estimation algorithm. This algorithm can realize asymptotic and unbiased estimation of two-dimensional angles, but its realization process requires spectral peak search in two-dimensional space, resulting in excessive calculation. In the follow-up studies, some scholars applied the ESPRIT algorithm to the two-dimensional DOA estimation algorithm. This algorithm does not require spectral peak search, so the calculation amount is small, and it has high application value.

上述算法都需要已知精确的阵列流型,然而在实际应用的过程中,各天线之间存在着固有的电磁效应,一根天线接收到的信号能量可能会辐射到其他附近的天线上去,尤其在阵元间距较小时,这种电磁辐射效应更加严重,通常将天线之间的这种相互作用成为互耦效应。对于二维平面阵列而言,每个阵元附近的阵元数量较多,这种互耦效应尤其严重,此时理想的阵列流型将会由于这种电磁扰动发生变化,不再能够满足实际工程需求,若不对这种扰动进行处理,现有的很多天线信号处理技术的性能将会恶化,算法实用性也将大大降低。当前对于解决互耦问题的研究,大多是基于一维DOA估计问题展开的。针对平面阵下的二维DOA估计的互耦问题,目前主要是通过在阵列外设置辅助阵元的方式实现的,当处于天线阵列一致耦合的状态下,利用MUSIC算法对二维DOA进行估计。这种算法会对阵列孔径产生损失,而且谱峰搜索的的计算量也比较大。针对此类问题,本发明基于均匀平面阵列提出了一种互耦条件下的二维DOA估计算法,以获得更加准确的信源方位,便于进行互耦误差校正,系统框图如图1所示。The above algorithms all require a known precise array flow pattern. However, in the process of practical application, there is an inherent electromagnetic effect between each antenna. The signal energy received by one antenna may be radiated to other nearby antennas, especially When the distance between the array elements is small, the electromagnetic radiation effect is more serious, and the interaction between the antennas is usually regarded as a mutual coupling effect. For a two-dimensional planar array, the number of array elements near each array element is large, and the mutual coupling effect is particularly serious. At this time, the ideal array flow pattern will change due to this electromagnetic disturbance, which can no longer meet the actual requirements. Engineering requirements, if this disturbance is not processed, the performance of many existing antenna signal processing technologies will deteriorate, and the practicability of the algorithm will also be greatly reduced. Most of the current research on solving the mutual coupling problem is based on the one-dimensional DOA estimation problem. Aiming at the mutual coupling problem of 2D DOA estimation under the planar array, it is mainly realized by setting auxiliary array elements outside the array. When the antenna array is uniformly coupled, the MUSIC algorithm is used to estimate the 2D DOA. This algorithm will cause loss of array aperture, and the amount of calculation of spectral peak search is relatively large. In response to such problems, the present invention proposes a two-dimensional DOA estimation algorithm under mutual coupling conditions based on a uniform planar array to obtain a more accurate source orientation and facilitate mutual coupling error correction. The system block diagram is shown in Figure 1.

发明内容SUMMARY OF THE INVENTION

本发明主要解决的技术问题是,考虑均匀平面天线阵列在接收发射信号的过程中,天线阵列间存在的互耦效应,采用秩损估计准则来设计算法,使得二维DOA估计的降维操作得以实现,从而得到二维DOA参数的估计值,再通过特征值分解的操作得到互耦系数估计值,以实现互耦误差的校正。The main technical problem solved by the present invention is that, considering the mutual coupling effect existing between the antenna arrays in the process of receiving the transmitted signal by the uniform planar antenna array, the rank loss estimation criterion is used to design the algorithm, so that the dimensionality reduction operation of the two-dimensional DOA estimation can be achieved. Then, the estimated value of the two-dimensional DOA parameter is obtained, and then the estimated value of the mutual coupling coefficient is obtained through the operation of eigenvalue decomposition, so as to realize the correction of the mutual coupling error.

为解决上述问题,本发明采用如下的技术方案:In order to solve the above problems, the present invention adopts the following technical scheme:

一种基于秩损估计的二维DOA估计与互耦校正方法,该方法的具体内容如下:A two-dimensional DOA estimation and mutual coupling correction method based on rank loss estimation. The specific contents of the method are as follows:

步骤1:对天线阵列系统进行建模仿真,采用的均匀平面阵列如图2所示。考虑互耦信号模型中,每个阵元不仅会接收到来波信号的入射部分,也会接收到周围其他阵元的辐射信号,故而阵元实际接收到的信号实际上是入射波与耦合分量的叠加。故对理想条件下的阵列流型进行修正,得到阵列输出的响应模型;Step 1: Model and simulate the antenna array system, and the uniform planar array used is shown in Figure 2. Considering the mutual coupling signal model, each array element will not only receive the incident part of the incoming wave signal, but also receive the radiation signal of other surrounding elements, so the signal actually received by the array element is actually the incident wave and the coupled component. superimposed. Therefore, the array flow pattern under ideal conditions is corrected to obtain the response model of the array output;

步骤2:利用修正后的阵列输出响应获得阵列输出的协方差矩阵Rx,并对其进行特征值分解得到噪声子空间Enoise以及信号子空间Esourse。进而基于子空间理论来解决问题。Step 2: Obtain the covariance matrix R x of the array output by using the corrected array output response, and perform eigenvalue decomposition on it to obtain the noise subspace E noise and the signal subspace E source . And then based on the subspace theory to solve the problem.

步骤3:实际中,阵元间的耦合强度也会随着阵元间距的增加而衰减,相距较远的阵元间的作用可以忽略。我们根据均匀平面阵的对称结构以及互易关系,通过对互耦矩阵C进行建模,表示出各阵元间的互耦作用;Step 3: In practice, the coupling strength between the array elements will also attenuate with the increase of the distance between the array elements, and the effect between the farther apart array elements can be ignored. According to the symmetrical structure and reciprocity relationship of the uniform plane array, we model the mutual coupling matrix C to express the mutual coupling effect between the array elements;

步骤4:利用对K个俯仰角和方位角

Figure BDA0002808568900000021
的参数变换可以得到一对映射关系
Figure BDA0002808568900000022
以此实现数据的降维处理,再利用Toeplitz矩阵及Kronecker积的性质,实现阵元信息与互耦系数的独立,根据秩损估计准则构造两次谱峰搜索函数,通过两次一维谱峰搜索代替二维谱峰搜索,从而计算得到方位参数估计值
Figure BDA0002808568900000023
Step 4: Use the pair of K pitch and azimuth angles
Figure BDA0002808568900000021
The parameter transformation of can get a pair of mapping relations
Figure BDA0002808568900000022
In this way, the dimensionality reduction processing of the data is realized, and the properties of the Toeplitz matrix and the Kronecker product are used to realize the independence of the array element information and the mutual coupling coefficient. According to the rank loss estimation criterion, two spectral peak search functions are constructed. The search replaces the two-dimensional spectral peak search, thereby calculating the estimated value of the orientation parameter
Figure BDA0002808568900000023

步骤5:利用映射关系

Figure BDA0002808568900000024
恢复出相对应的方位参数估计值
Figure BDA0002808568900000025
Step 5: Leverage Mapping Relationships
Figure BDA0002808568900000024
The corresponding azimuth parameter estimates are recovered
Figure BDA0002808568900000025

步骤6:对互耦系数进行估计。根据得到的参数估计值

Figure BDA0002808568900000026
构造一个解耦合矩阵T,并利用特征值分解法得到所有的耦合系数,以此重构出互耦矩阵的估计值
Figure BDA0002808568900000031
进而可以据此进行互耦校正。Step 6: Estimate the mutual coupling coefficient. According to the obtained parameter estimates
Figure BDA0002808568900000026
Construct a decoupling matrix T, and use the eigenvalue decomposition method to get all the coupling coefficients, so as to reconstruct the estimated value of the mutual coupling matrix
Figure BDA0002808568900000031
Further, mutual coupling correction can be performed accordingly.

本发明的特征如下:The features of the present invention are as follows:

(1)考虑均匀平面天线阵列中阵元间存在的互耦效应,对互耦矩阵进行建模,建立更符合实际应用中的信号模型。(1) Considering the mutual coupling effect between the array elements in the uniform planar antenna array, the mutual coupling matrix is modeled, and a signal model that is more suitable for practical applications is established.

(2)利用参数映射的变换域关系将信源数据与互耦误差向量分离开,再利用秩损估计准则构造相应的谱峰搜索函数,实现二维方位参数的估计。(2) The source data and the mutual coupling error vector are separated by the transform domain relationship of the parameter mapping, and then the corresponding spectral peak search function is constructed by using the rank loss estimation criterion to realize the estimation of the two-dimensional orientation parameters.

(3)利用得到的估计参数,构造解耦合矩阵,实现对互耦矩阵的估计,进而据此进行互耦校正。(3) Using the obtained estimated parameters, construct the decoupling matrix, realize the estimation of the mutual coupling matrix, and then perform the mutual coupling correction accordingly.

与现有技术相比,本发明具有以下有益效果:Compared with the prior art, the present invention has the following beneficial effects:

本发明提出了一种基于秩损估计的二维DOA估计与互耦校正方法。通过构造互耦误差矩阵构建均匀平面天线阵列在互耦误差下的信号接收模型;利用参数映射的变换域关系将信源数据与互耦误差向量分离开,再利用秩损估计准则构造相应的谱峰搜索函数,实现二维方位参数的估计;最后利用已经得到的估计方位参数,构造解耦合矩阵,实现对互耦矩阵的估计,进而据此可以进行互耦校正。用合适仿真对所提方法的估计结果进行验证。均方根误差对一组测量中的特大或特小误差反映非常敏感,所以,均方根误差能够很好地反映出测量的精密度。该方法与现行估计算法相比,本发明算法DOA估计结果均方根误差更小,估计成功率也更高,即表示本文所提方法效果更佳。The invention proposes a two-dimensional DOA estimation and mutual coupling correction method based on rank loss estimation. The signal receiving model of the uniform planar antenna array under the mutual coupling error is constructed by constructing the mutual coupling error matrix; the source data and the mutual coupling error vector are separated by using the transform domain relationship of parameter mapping, and then the corresponding spectrum is constructed by using the rank loss estimation criterion The peak search function is used to estimate the two-dimensional azimuth parameters; finally, the decoupling matrix is constructed by using the estimated azimuth parameters that have been obtained to realize the estimation of the mutual coupling matrix, and then the mutual coupling can be corrected accordingly. The estimation results of the proposed method are verified by suitable simulations. The root mean square error is very sensitive to very large or small errors in a set of measurements, so the root mean square error can well reflect the precision of the measurement. Compared with the current estimation algorithm, the method of the present invention has smaller root mean square error of the DOA estimation result and higher estimation success rate, which means that the method proposed in this paper has better effect.

附图说明Description of drawings

图1为本发明所涉及方法的流程图;Fig. 1 is the flow chart of the method involved in the present invention;

图2为均匀平面天线阵列模型;Figure 2 is a uniform planar antenna array model;

图3随信噪比变化时均方根误差变化曲线;Fig. 3 Variation curve of root mean square error with the change of signal-to-noise ratio;

图4随信噪比变化时算法成功率变化曲线;Figure 4. The change curve of the algorithm success rate when the signal-to-noise ratio changes;

图5随快拍数变化时均方根误差变化曲线;Fig. 5 Variation curve of root mean square error when the number of snapshots changes;

图6随快拍数变化时算法成功率误差变化曲线。Figure 6. The change curve of the algorithm success rate error when the number of snapshots changes.

具体实施方式Detailed ways

下面结合附图和实施步骤对本发明做进一步说明。The present invention will be further described below in conjunction with the accompanying drawings and implementation steps.

基于秩损估计的二维DOA估计与互耦校正方法流程图如图1所示,包括以下步骤:The flowchart of the two-dimensional DOA estimation and mutual coupling correction method based on rank loss estimation is shown in Figure 1, which includes the following steps:

如图1所示为本发明流程图。Figure 1 is a flow chart of the present invention.

第一步:考虑在存在互耦误差的条件下,对均匀面阵模型进行研究,阵元个数为M×N,阵元间距分别为dx和dy;在某t时刻,考虑K个远场窄带信号以

Figure BDA0002808568900000041
的角度入射到阵列上,
Figure BDA0002808568900000042
表示第k个信号的方位角和俯仰角,则阵列的输出响应被表示为The first step: consider the existence of mutual coupling error, study the uniform area array model, the number of array elements is M×N, and the distances between the array elements are d x and d y respectively; at a certain time t, consider K arrays far-field narrowband signals with
Figure BDA0002808568900000041
incident on the array at an angle,
Figure BDA0002808568900000042
represents the azimuth and elevation angles of the k-th signal, then the output response of the array is expressed as

x(t)=CAs(t)+n(t) (1)x(t)=CAs(t)+n(t) (1)

其中C代表互耦矩阵,

Figure BDA0002808568900000043
表示理想的阵列响应矩阵,其中
Figure BDA0002808568900000044
Figure BDA0002808568900000045
s(t)表示源信号向量,n(t)为不相关的噪声矢量,其均值为零,方差为σ2;其中j表示复数的虚数单位,
Figure BDA0002808568900000046
表示Kronecker积,λ表示信号的波长;where C represents the mutual coupling matrix,
Figure BDA0002808568900000043
represents the ideal array response matrix, where
Figure BDA0002808568900000044
Figure BDA0002808568900000045
s(t) represents the source signal vector, n(t) is the uncorrelated noise vector with zero mean and variance σ 2 ; where j represents the complex imaginary unit,
Figure BDA0002808568900000046
represents the Kronecker product, and λ represents the wavelength of the signal;

第二步:对互耦矩阵C进行建模;由于均匀面阵看作由N个均匀线阵所构成,因此,不同的子阵之间也存在着互耦效应;根据均匀平面天线阵列的对称性和互易性质,互耦矩阵C表示为Step 2: Model the mutual coupling matrix C; since the uniform planar array is considered to be composed of N uniform linear arrays, there is also a mutual coupling effect between different sub-arrays; according to the symmetry of the uniform planar antenna array and reciprocity properties, the mutual coupling matrix C is expressed as

Figure BDA0002808568900000047
Figure BDA0002808568900000047

其中,

Figure BDA0002808568900000048
为由耦合向量
Figure BDA0002808568900000049
所构造的Toeplitz矩阵,
Figure BDA00028085689000000410
表示与x轴平行放置的第n个均匀线阵的第m个阵元的耦合系数;考虑每个阵元与其四周的P个阵元产生互耦效应,得到耦合向量
Figure BDA00028085689000000411
cn中的零元素表示远处的互耦作用忽略不计,则当n>P时,子矩阵Cn为零矩阵;in,
Figure BDA0002808568900000048
coupled vector
Figure BDA0002808568900000049
The constructed Toeplitz matrix,
Figure BDA00028085689000000410
Represents the coupling coefficient of the mth element of the nth uniform linear array placed parallel to the x-axis; considering the mutual coupling effect of each array element and its surrounding P array elements, the coupling vector is obtained
Figure BDA00028085689000000411
The zero element in c n means that the mutual coupling in the distance is negligible, then when n>P, the sub-matrix C n is a zero matrix;

第三步:通过阵列的输出响应得出阵列输出的协方差矩阵响应为Step 3: Through the output response of the array, the covariance matrix response of the array output is obtained as

Rx=E{x(t)xH(t)}=CARsAHCH2I (3)R x =E{x(t) xH (t)}=CAR s A H C H2 I (3)

式中,Rs=E{s(t)sH(t)}为信源协方差矩阵,E{·}表示矩阵的期望运算,(·)H表示共轭转置运算,I表示MN×MN维的单位矩阵;对Rx进行特征值分解则得到噪声子空间Enoise和信号子空间Esourse;当在接收到L次快拍数采样的条件下,协方差矩阵通过

Figure BDA00028085689000000412
等效估计出来,同理得到相应的子空间的估计值
Figure BDA0002808568900000051
Figure BDA0002808568900000052
In the formula, R s =E{s(t)s H (t)} is the source covariance matrix, E{·} is the expected operation of the matrix, (·) H is the conjugate transpose operation, and I is the MN× The identity matrix of MN dimension; the eigenvalue decomposition of R x is performed to obtain the noise subspace E noise and the signal subspace E source ; when the L number of snapshot samples are received, the covariance matrix passes through
Figure BDA00028085689000000412
Equivalent estimation is obtained, and the estimated value of the corresponding subspace is obtained in the same way
Figure BDA0002808568900000051
and
Figure BDA0002808568900000052

第四步:进行参数变换,借助变换域将二维DOA估计与互耦误差分离开来;定义Step 4: Perform parameter transformation, and separate the two-dimensional DOA estimation from the mutual coupling error with the help of the transform domain; define

Figure BDA0002808568900000053
Figure BDA0002808568900000053

则得到一对映射关系

Figure BDA0002808568900000054
Figure BDA0002808568900000055
其中then get a pair of mapping relations
Figure BDA0002808568900000054
but
Figure BDA0002808568900000055
in

Figure BDA0002808568900000056
Figure BDA0002808568900000056

则等效阵列导向矢量写为Then the equivalent array steering vector is written as

Figure BDA0002808568900000057
Figure BDA0002808568900000057

其中,ayn表示ay(vk)的第n个元素;Among them, a yn represents the nth element of a y (v k );

下面引入一个定理,以处理后续步骤;A theorem is introduced below to handle the subsequent steps;

定理1:对于一个带状Toeplitz矩阵A∈CM×M及一个向量x∈CM×1,有如下矩阵运算关系成立Theorem 1: For a banded Toeplitz matrix A∈C M×M and a vector x∈C M×1 , the following matrix operation relations hold

Ax=Q(x)aAx=Q(x)a

其中,a=A1p(p=1,2,..,P)∈CP×1,其中A1p表示矩阵A第一行第p列的元素,P为矩阵A第一行非0元素个数,而Q(x)表示为Among them, a=A 1p (p=1,2,..,P)∈C P×1 , where A 1p represents the element of the first row and the pth column of matrix A, and P is the number of non-zero elements in the first row of matrix A number, and Q(x) is expressed as

Q(x)=Q1(x)+Q2(x)Q(x)=Q 1 (x)+Q 2 (x)

Figure BDA0002808568900000058
Figure BDA0002808568900000058

Figure BDA0002808568900000059
Figure BDA0002808568900000059

[·]ih代表矩阵的第i行h列的元素;[ ] ih represents the element of the i-th row and h-column of the matrix;

定义矢量

Figure BDA00028085689000000510
则运用定理1得出define vector
Figure BDA00028085689000000510
Then, using Theorem 1, we get

Figure BDA00028085689000000511
Figure BDA00028085689000000511

其中n=1,2,...,P;定义矢量

Figure BDA00028085689000000512
则将式(6)整理为where n=1,2,...,P; defines the vector
Figure BDA00028085689000000512
Then formula (6) can be sorted into

Figure BDA0002808568900000061
Figure BDA0002808568900000061

其中Qy(vk)为N×P维矩阵,Qx(uk)为M×P维矩阵,根据定理1,两者具有相同的矩阵结构,根据子空间原理,阵列流型与噪声子空间是相互正交的,因此Among them, Q y (v k ) is an N×P-dimensional matrix, and Q x (u k ) is an M×P-dimensional matrix. According to Theorem 1, the two have the same matrix structure. According to the subspace principle, the array manifold and noise subspace Spaces are mutually orthogonal, so

Figure BDA0002808568900000062
Figure BDA0002808568900000062

利用Kronecker积的性质

Figure BDA0002808568900000063
定义
Figure BDA0002808568900000064
则Using the properties of the Kronecker product
Figure BDA0002808568900000063
definition
Figure BDA0002808568900000064
but

Figure BDA0002808568900000065
Figure BDA0002808568900000065

其中,IM和IP分别表示M阶和P阶的单位矩阵;Among them, IM and IP represent the identity matrix of M order and P order, respectively;

第五步:根据秩损估计原理,由于MN-K≥MP,则G(vk)是满秩的,观察式(10)可知,由于

Figure BDA0002808568900000066
则式(10)仅在G(vk)缺秩的条件下是成立的,则det{G(vk)}=0;根据第二步,在接收到L次快拍数的条件下,G(vk)等效为Step 5: According to the principle of rank loss estimation, since MN-K≥MP, G(v k ) is full rank. From equation (10), it can be seen that due to
Figure BDA0002808568900000066
Then Equation (10) is only valid under the condition that G(v k ) lacks rank, then det{G(v k )}=0; according to the second step, under the condition of receiving L snapshots, G(v k ) is equivalent to

Figure BDA0002808568900000067
Figure BDA0002808568900000067

所以构造如下的谱函数So construct the following spectral function

Figure BDA0002808568900000068
Figure BDA0002808568900000068

式中det{·}表示矩阵的行列式运算,tr{·}表示矩阵的迹运算;基于上式进行谱峰搜索,便获得方位参数vk的估计值

Figure BDA0002808568900000069
将秩损估计扩展到二维情况下使用,定义一个新的P2×P2维的矩阵In the formula, det{·} represents the determinant operation of the matrix, and tr{·} represents the trace operation of the matrix; based on the above formula, the spectral peak search is performed to obtain the estimated value of the orientation parameter v k
Figure BDA0002808568900000069
Extend the rank loss estimation to the two-dimensional case and define a new P 2 ×P 2 -dimensional matrix

Figure BDA00028085689000000610
Figure BDA00028085689000000610

将得到的估计值

Figure BDA00028085689000000611
代入式(13),得到
Figure BDA00028085689000000612
满足秩损原则的条件,即MN-K≥P2,于是构造如下谱函数The estimated value that will be obtained
Figure BDA00028085689000000611
Substituting into equation (13), we get
Figure BDA00028085689000000612
Satisfy the condition of the rank loss principle, that is, MN-K≥P 2 , so the following spectral function is constructed

Figure BDA00028085689000000613
Figure BDA00028085689000000613

同理通过对其进行谱峰搜索,就得到方位参数uk的估计值

Figure BDA00028085689000000614
Similarly, by searching for spectral peaks, the estimated value of the orientation parameter u k is obtained.
Figure BDA00028085689000000614

第六步:根据映射关系

Figure BDA00028085689000000615
恢复出对应的俯仰角和方位角参数
Figure BDA00028085689000000616
Step 6: According to the mapping relationship
Figure BDA00028085689000000615
Recover the corresponding pitch and azimuth parameters
Figure BDA00028085689000000616

Figure BDA00028085689000000617
Figure BDA00028085689000000617

由此可见,(uk,vk)域的谱峰搜索结果与

Figure BDA0002808568900000071
上的谱峰搜索是等价的;It can be seen that the peak search results in the (u k ,v k ) domain are the same as
Figure BDA0002808568900000071
The peak search on is equivalent;

第七步:在得到所有方位参数的估计值后,对互耦系数进行估计;利用已得到估计值构造如下矩阵Step 7: After obtaining the estimated values of all azimuth parameters, estimate the mutual coupling coefficient; construct the following matrix using the obtained estimated values

Figure BDA0002808568900000072
Figure BDA0002808568900000072

对T进行特征值分解操作,由于互耦向量

Figure BDA0002808568900000073
的第一个值为自耦系数,所以取值为1,那么得到互耦系数的估计值The eigenvalue decomposition operation is performed on T, due to the mutual coupling vector
Figure BDA0002808568900000073
The first value of the autocoupling coefficient, so the value is 1, then the estimated value of the mutual coupling coefficient is obtained

Figure BDA0002808568900000074
Figure BDA0002808568900000074

其中emin[·]表示求最小特征值对应的特征向量的算子;进而根据得到的互耦向量的估计值

Figure BDA0002808568900000075
就重构出互耦矩阵
Figure BDA0002808568900000076
从而实现对天线阵列的互耦校正。where e min [ ] represents the operator for finding the eigenvector corresponding to the minimum eigenvalue; and then according to the obtained estimated value of the mutual coupling vector
Figure BDA0002808568900000075
to reconstruct the mutual coupling matrix
Figure BDA0002808568900000076
Thereby, the mutual coupling correction to the antenna array is realized.

以上实施例仅为本发明的示例性实施例,不用于限制本发明,本发明的保护范围由权利要求书限定。本领域技术人员可以在本发明的实质和保护范围内,对本发明做出各种修改或等同替换,这种修改或等同替换也应视为落在本发明的保护范围内。The above embodiments are only exemplary embodiments of the present invention, and are not intended to limit the present invention, and the protection scope of the present invention is defined by the claims. Those skilled in the art can make various modifications or equivalent replacements to the present invention within the spirit and protection scope of the present invention, and such modifications or equivalent replacements should also be regarded as falling within the protection scope of the present invention.

结果分析Result analysis

为了证明本发明算法的有效性,我们选取误差系数已知的MUSIC算法,基于辅助阵元的自校正算法,本发明算法进行对比。In order to prove the effectiveness of the algorithm of the present invention, we select the MUSIC algorithm with a known error coefficient, and compare the algorithm of the present invention based on the self-correction algorithm of the auxiliary array element.

首先对比三种算法在信噪比(SNR)变化时算法的成功率变化和均方根误差(RMSE)变化情况,实验中将快拍数设置为600保持恒定不变,信噪比从-5dB到25dB以3dB为间隔进行变化。为了保证试验的准确性,每个信噪比下做200次独立仿真实验,实验结果如图3,图4。通过结果图可以看出在信噪比增大时三种算法成功率都在增加,均方根误差都有所降低,纵向对比可以看出本发明算法性能在成功率和均方根误差上均优于基于辅助阵元的自校正算法,说明本发明算法得到的估计结果更接近于真实值。First, compare the success rate and root mean square error (RMSE) of the three algorithms when the signal-to-noise ratio (SNR) changes. to 25dB in 3dB steps. In order to ensure the accuracy of the test, 200 independent simulation experiments were performed under each signal-to-noise ratio. The experimental results are shown in Figure 3 and Figure 4. From the result graph, it can be seen that when the signal-to-noise ratio increases, the success rate of the three algorithms increases, and the root mean square error decreases. The longitudinal comparison shows that the performance of the algorithm of the present invention is equal to the success rate and the root mean square error. It is better than the self-correction algorithm based on the auxiliary array element, indicating that the estimation result obtained by the algorithm of the present invention is closer to the real value.

然后再对比三种算法随快拍数(Snapshots)变化时的成功率变化和均方根误差变化(RMSE)情况。实验中将信噪比设置为10dB且保持恒定不变,快拍数从300到900以100为间隔进行变化。为了保证试验的准确性,每个快拍数下做200次独立仿真实验,实验结果如图5,图6。通过结果图可以看出在快拍数增大时三种算法成功率都在增加,均方根误差都有所降低,纵向对比可以看出本发明算法性能在成功率和均方根误差上均优于基于辅助阵元的自校正算法,说明本发明算法得到的估计结果更接近于真实值。Then compare the success rate and root mean square error (RMSE) of the three algorithms when the number of snapshots (Snapshots) changes. In the experiment, the signal-to-noise ratio was set to 10dB and kept constant, and the number of snapshots was changed from 300 to 900 at intervals of 100. In order to ensure the accuracy of the test, 200 independent simulation experiments are performed under each snapshot number, and the experimental results are shown in Figure 5 and Figure 6. From the result graph, it can be seen that when the number of snapshots increases, the success rate of the three algorithms increases, and the root mean square error decreases. The longitudinal comparison shows that the performance of the algorithm of the present invention is equal to the success rate and the root mean square error. It is better than the self-correction algorithm based on the auxiliary array element, indicating that the estimation result obtained by the algorithm of the present invention is closer to the real value.

Claims (2)

1.一种基于秩损估计的二维DOA估计与互耦校正方法,其特征在于:1. a two-dimensional DOA estimation and mutual coupling correction method based on rank loss estimation, is characterized in that: (1)考虑均匀平面天线阵列中阵元间存在的互耦效应,对互耦矩阵进行建模,建立更符合实际应用中的信号模型;(1) Consider the mutual coupling effect between the array elements in the uniform planar antenna array, model the mutual coupling matrix, and establish a signal model that is more in line with practical applications; (2)利用参数映射的变换域关系将信源数据与互耦误差向量分离开,再利用秩损估计准则构造相应的谱峰搜索函数,实现二维方位参数的估计,得到更优的预测结果;(2) Use the transform domain relationship of parameter mapping to separate the source data from the mutual coupling error vector, and then use the rank loss estimation criterion to construct the corresponding spectral peak search function to realize the estimation of the two-dimensional orientation parameters and obtain better prediction results. ; (3)利用得到的估计参数,构造解耦合矩阵,实现对互耦矩阵的估计,进而据此进行互耦误差校正。(3) Using the obtained estimated parameters, construct a decoupling matrix, realize the estimation of the mutual coupling matrix, and then correct the mutual coupling error accordingly. 2.权利要求1所述的方法,其特征在于包括以下步骤:2. the method for claim 1 is characterized in that comprising the following steps: 第一步:考虑在存在互耦误差的条件下,对均匀面阵模型进行研究,阵元个数为M×N,阵元间距分别为dx和dy;在某t时刻,考虑K个远场窄带信号以
Figure FDA0002808568890000011
的角度入射到阵列上,
Figure FDA0002808568890000012
表示第k个信号的方位角和俯仰角,则阵列的输出响应被表示为
The first step: consider the existence of mutual coupling error, study the uniform area array model, the number of array elements is M×N, and the distances between the array elements are d x and d y respectively; at a certain time t, consider K arrays far-field narrowband signals with
Figure FDA0002808568890000011
incident on the array at an angle,
Figure FDA0002808568890000012
represents the azimuth and elevation angles of the k-th signal, then the output response of the array is expressed as
x(t)=CAs(t)+n(t) (1)x(t)=CAs(t)+n(t) (1) 其中C代表互耦矩阵,
Figure FDA0002808568890000013
表示理想的阵列响应矩阵,其中
Figure FDA0002808568890000014
Figure FDA0002808568890000015
s(t)表示源信号向量,n(t)为不相关的噪声矢量,其均值为零,方差为σ2;其中j表示复数的虚数单位,
Figure FDA0002808568890000016
表示Kronecker积,λ表示信号的波长;
where C represents the mutual coupling matrix,
Figure FDA0002808568890000013
represents the ideal array response matrix, where
Figure FDA0002808568890000014
Figure FDA0002808568890000015
s(t) represents the source signal vector, n(t) is the uncorrelated noise vector with zero mean and variance σ 2 ; where j represents the complex imaginary unit,
Figure FDA0002808568890000016
represents the Kronecker product, and λ represents the wavelength of the signal;
第二步:对互耦矩阵C进行建模;由于均匀面阵看作由N个均匀线阵所构成,因此,不同的子阵之间也存在着互耦效应;根据均匀平面天线阵列的对称性和互易性质,互耦矩阵C表示为Step 2: Model the mutual coupling matrix C; since the uniform planar array is considered to be composed of N uniform linear arrays, there is also a mutual coupling effect between different sub-arrays; according to the symmetry of the uniform planar antenna array and reciprocity properties, the mutual coupling matrix C is expressed as
Figure FDA0002808568890000017
Figure FDA0002808568890000017
其中,
Figure FDA0002808568890000018
为由耦合向量
Figure FDA0002808568890000019
所构造的Toeplitz矩阵,
Figure FDA00028085688900000110
表示与x轴平行放置的第n个均匀线阵的第m个阵元的耦合系数;考虑每个阵元与其四周的P个阵元产生互耦效应,得到耦合向量
Figure FDA0002808568890000021
cn中的零元素表示远处的互耦作用忽略不计,则当n>P时,子矩阵Cn为零矩阵;
in,
Figure FDA0002808568890000018
coupled vector
Figure FDA0002808568890000019
The constructed Toeplitz matrix,
Figure FDA00028085688900000110
Represents the coupling coefficient of the mth element of the nth uniform linear array placed parallel to the x-axis; considering the mutual coupling effect of each array element and its surrounding P array elements, the coupling vector is obtained
Figure FDA0002808568890000021
The zero element in c n means that the mutual coupling in the distance is negligible, then when n>P, the sub-matrix C n is a zero matrix;
第三步:通过阵列的输出响应得出阵列输出的协方差矩阵响应为Step 3: Through the output response of the array, the covariance matrix response of the array output is obtained as Rx=E{x(t)xH(t)}=CARsAHCH2I (3)R x =E{x(t) xH (t)}=CAR s A H C H2 I (3) 式中,Rs=E{s(t)sH(t)}为信源协方差矩阵,E{·}表示矩阵的期望运算,(·)H表示共轭转置运算,I表示MN×MN维的单位矩阵;对Rx进行特征值分解则得到噪声子空间Enoise和信号子空间Esourse;当在接收到L次快拍数采样的条件下,协方差矩阵通过
Figure FDA0002808568890000022
等效估计出来,同理得到相应的子空间的估计值
Figure FDA0002808568890000023
Figure FDA0002808568890000024
In the formula, R s =E{s(t)s H (t)} is the source covariance matrix, E{·} is the expected operation of the matrix, (·) H is the conjugate transpose operation, and I is the MN× The identity matrix of MN dimension; the eigenvalue decomposition of R x is performed to obtain the noise subspace E noise and the signal subspace E source ; when the L number of snapshot samples are received, the covariance matrix passes through
Figure FDA0002808568890000022
Equivalent estimation is obtained, and the estimated value of the corresponding subspace is obtained in the same way
Figure FDA0002808568890000023
and
Figure FDA0002808568890000024
第四步:进行参数变换,借助变换域将二维DOA估计与互耦误差分离开来;定义Step 4: Perform parameter transformation, and separate the two-dimensional DOA estimation from the mutual coupling error with the help of the transform domain; define
Figure FDA0002808568890000025
Figure FDA0002808568890000025
则得到一对映射关系
Figure FDA0002808568890000026
Figure FDA0002808568890000027
其中
Then get a pair of mapping relationship
Figure FDA0002808568890000026
but
Figure FDA0002808568890000027
in
Figure FDA0002808568890000028
Figure FDA0002808568890000028
则等效阵列导向矢量写为Then the equivalent array steering vector is written as
Figure FDA0002808568890000029
Figure FDA0002808568890000029
其中,ayn表示ay(vk)的第n个元素;Among them, a yn represents the nth element of a y (v k ); 下面引入一个定理,以处理后续步骤;A theorem is introduced below to handle the subsequent steps; 定理1:对于一个带状Toeplitz矩阵A∈CM×M及一个向量x∈CM×1,有如下矩阵运算关系成立Theorem 1: For a banded Toeplitz matrix A∈C M×M and a vector x∈C M×1 , the following matrix operation relations hold Ax=Q(x)aAx=Q(x)a 其中,a=A1p(p=1,2,..,P)∈CP×1,其中A1p表示矩阵A第一行第p列的元素,P为矩阵A第一行非0元素个数,而Q(x)表示为Among them, a=A 1p (p=1,2,..,P)∈C P×1 , where A 1p represents the element of the first row and the pth column of matrix A, and P is the number of non-zero elements in the first row of matrix A number, and Q(x) is expressed as Q(x)=Q1(x)+Q2(x)Q(x)=Q 1 (x)+Q 2 (x)
Figure FDA0002808568890000031
Figure FDA0002808568890000031
Figure FDA0002808568890000032
Figure FDA0002808568890000032
[·]ih代表矩阵的第i行h列的元素;[ ] ih represents the element of the i-th row and h-column of the matrix; 定义矢量
Figure FDA0002808568890000033
则运用定理1得出
define vector
Figure FDA0002808568890000033
Then, using Theorem 1, we get
Figure FDA0002808568890000034
Figure FDA0002808568890000034
其中n=1,2,...,P;定义矢量
Figure FDA0002808568890000035
则将式(6)整理为
where n=1,2,...,P; defines the vector
Figure FDA0002808568890000035
Then formula (6) can be sorted into
Figure FDA0002808568890000036
Figure FDA0002808568890000036
其中Qy(vk)为N×P维矩阵,Qx(uk)为M×P维矩阵,根据定理1,两者具有相同的矩阵结构,根据子空间原理,阵列流型与噪声子空间是相互正交的,因此Among them, Q y (v k ) is an N×P-dimensional matrix, and Q x (u k ) is an M×P-dimensional matrix. According to Theorem 1, the two have the same matrix structure. According to the subspace principle, the array manifold and noise subspace Spaces are mutually orthogonal, so
Figure FDA0002808568890000037
Figure FDA0002808568890000037
利用Kronecker积的性质
Figure FDA0002808568890000038
定义
Figure FDA0002808568890000039
Using the properties of the Kronecker product
Figure FDA0002808568890000038
definition
Figure FDA0002808568890000039
but
Figure FDA00028085688900000310
Figure FDA00028085688900000310
其中,IM和IP分别表示M阶和P阶的单位矩阵;Among them, IM and IP represent the identity matrix of M order and P order, respectively; 第五步:根据秩损估计原理,由于MN-K≥MP,则G(vk)是满秩的,观察式(10)可知,由于
Figure FDA00028085688900000311
则式(10)仅在G(vk)缺秩的条件下是成立的,则det{G(vk)}=0;根据第二步,在接收到L次快拍数的条件下,G(vk)等效为
Step 5: According to the principle of rank loss estimation, since MN-K≥MP, G(v k ) is full rank. From equation (10), it can be seen that due to
Figure FDA00028085688900000311
Then Equation (10) is only valid under the condition that G(v k ) lacks rank, then det{G(v k )}=0; according to the second step, under the condition of receiving L snapshots, G(v k ) is equivalent to
Figure FDA00028085688900000312
Figure FDA00028085688900000312
所以构造如下的谱函数So construct the following spectral function
Figure FDA00028085688900000313
Figure FDA00028085688900000313
式中det{·}表示矩阵的行列式运算,tr{·}表示矩阵的迹运算;基于上式进行谱峰搜索,便获得方位参数vk的估计值
Figure FDA00028085688900000314
将秩损估计扩展到二维情况下使用,定义一个新的P2×P2维的矩阵
In the formula, det{·} represents the determinant operation of the matrix, and tr{·} represents the trace operation of the matrix; based on the above formula, the spectral peak search is performed to obtain the estimated value of the orientation parameter v k
Figure FDA00028085688900000314
Extend the rank loss estimation to the two-dimensional case and define a new P 2 ×P 2 -dimensional matrix
Figure FDA00028085688900000315
Figure FDA00028085688900000315
将得到的估计值
Figure FDA00028085688900000316
代入式(13),得到
Figure FDA00028085688900000317
满足秩损原则的条件,即MN-K≥P2,于是构造如下谱函数
The estimated value that will be obtained
Figure FDA00028085688900000316
Substituting into equation (13), we get
Figure FDA00028085688900000317
Satisfy the condition of the rank loss principle, that is, MN-K≥P 2 , so the following spectral function is constructed
Figure FDA0002808568890000041
Figure FDA0002808568890000041
同理通过对其进行谱峰搜索,就得到方位参数uk的估计值
Figure FDA0002808568890000042
Similarly, by searching for spectral peaks, the estimated value of the orientation parameter u k is obtained.
Figure FDA0002808568890000042
第六步:根据映射关系
Figure FDA0002808568890000043
恢复出对应的俯仰角和方位角参数
Figure FDA0002808568890000044
Step 6: According to the mapping relationship
Figure FDA0002808568890000043
Recover the corresponding pitch and azimuth parameters
Figure FDA0002808568890000044
Figure FDA0002808568890000045
Figure FDA0002808568890000045
由此可见,(uk,vk)域的谱峰搜索结果与
Figure FDA0002808568890000046
上的谱峰搜索是等价的;
It can be seen that the peak search results in the (u k ,v k ) domain are the same as
Figure FDA0002808568890000046
The peak search on is equivalent;
第七步:在得到所有方位参数的估计值后,对互耦系数进行估计;利用已得到估计值构造如下矩阵Step 7: After obtaining the estimated values of all azimuth parameters, estimate the mutual coupling coefficient; construct the following matrix using the obtained estimated values
Figure FDA0002808568890000047
Figure FDA0002808568890000047
对T进行特征值分解操作,由于互耦向量
Figure FDA0002808568890000048
的第一个值为自耦系数,所以取值为1,那么得到互耦系数的估计值
The eigenvalue decomposition operation is performed on T, due to the mutual coupling vector
Figure FDA0002808568890000048
The first value of the autocoupling coefficient, so the value is 1, then the estimated value of the mutual coupling coefficient is obtained
Figure FDA0002808568890000049
Figure FDA0002808568890000049
其中emin[·]表示求最小特征值对应的特征向量的算子;进而根据得到的互耦向量的估计值
Figure FDA00028085688900000410
就重构出互耦矩阵
Figure FDA00028085688900000411
从而实现对天线阵列的互耦校正。
where e min [ ] represents the operator for finding the eigenvector corresponding to the minimum eigenvalue; and then according to the obtained estimated value of the mutual coupling vector
Figure FDA00028085688900000410
to reconstruct the mutual coupling matrix
Figure FDA00028085688900000411
Thereby, the mutual coupling correction to the antenna array is realized.
CN202011381435.7A 2020-12-01 2020-12-01 Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation Pending CN112379327A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202011381435.7A CN112379327A (en) 2020-12-01 2020-12-01 Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202011381435.7A CN112379327A (en) 2020-12-01 2020-12-01 Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation

Publications (1)

Publication Number Publication Date
CN112379327A true CN112379327A (en) 2021-02-19

Family

ID=74589531

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202011381435.7A Pending CN112379327A (en) 2020-12-01 2020-12-01 Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation

Country Status (1)

Country Link
CN (1) CN112379327A (en)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113296056A (en) * 2021-05-10 2021-08-24 华中科技大学 Sound array configuration and sound source positioning method and system
CN113325376A (en) * 2021-05-27 2021-08-31 重庆邮电大学 Method for correcting electromagnetic cross coupling error of phase control array under color noise
CN113420411A (en) * 2021-05-25 2021-09-21 北京科技大学 High-resolution narrowband DOA estimation algorithm for wireless signals and implementation method
CN113466782A (en) * 2021-06-08 2021-10-01 同济大学 Deep Learning (DL) -based cross-coupling correction D O A estimation method
CN114624665A (en) * 2022-03-24 2022-06-14 电子科技大学 Mutual coupling error DOA self-correction method based on iterative optimization of dynamic parameters
CN115291160A (en) * 2022-08-04 2022-11-04 中国科学院微小卫星创新研究院 Two-dimensional DOA estimation method, system and computer readable medium
CN117031390A (en) * 2023-08-11 2023-11-10 哈尔滨工程大学 Gridless DOA estimation method based on antenna mutual coupling

Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080231505A1 (en) * 2007-03-23 2008-09-25 Weiqing Zhu Method of Source Number Estimation and Its Application in Method of Direction of Arrival Estimation
KR101413229B1 (en) * 2013-05-13 2014-08-06 한국과학기술원 DOA estimation Device and Method
CN106569172A (en) * 2016-10-13 2017-04-19 北京邮电大学 Two-dimensional doa estimation method
CN108226855A (en) * 2017-12-14 2018-06-29 宁波大学 The not rounded joint parameter estimation method in far and near field in the case of mutual coupling
CN108680891A (en) * 2018-01-05 2018-10-19 大连大学 The DOA estimation method of mutual coupling effect is considered under the conditions of non-uniform noise
CN110749857A (en) * 2019-09-12 2020-02-04 宁波大学 DOA estimation method for two-dimensional non-circular signal of uniform rectangular array based on rank loss method

Patent Citations (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080231505A1 (en) * 2007-03-23 2008-09-25 Weiqing Zhu Method of Source Number Estimation and Its Application in Method of Direction of Arrival Estimation
KR101413229B1 (en) * 2013-05-13 2014-08-06 한국과학기술원 DOA estimation Device and Method
CN106569172A (en) * 2016-10-13 2017-04-19 北京邮电大学 Two-dimensional doa estimation method
CN108226855A (en) * 2017-12-14 2018-06-29 宁波大学 The not rounded joint parameter estimation method in far and near field in the case of mutual coupling
CN108680891A (en) * 2018-01-05 2018-10-19 大连大学 The DOA estimation method of mutual coupling effect is considered under the conditions of non-uniform noise
CN110749857A (en) * 2019-09-12 2020-02-04 宁波大学 DOA estimation method for two-dimensional non-circular signal of uniform rectangular array based on rank loss method

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
刘江等: "均匀平面阵下的二维DOA估计与互耦自校正", 《电讯技术》, pages 377 - 382 *

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113296056A (en) * 2021-05-10 2021-08-24 华中科技大学 Sound array configuration and sound source positioning method and system
CN113420411A (en) * 2021-05-25 2021-09-21 北京科技大学 High-resolution narrowband DOA estimation algorithm for wireless signals and implementation method
CN113420411B (en) * 2021-05-25 2024-02-20 北京科技大学 High-resolution narrowband DOA estimation algorithm for wireless signals and implementation method
CN113325376A (en) * 2021-05-27 2021-08-31 重庆邮电大学 Method for correcting electromagnetic cross coupling error of phase control array under color noise
CN113466782A (en) * 2021-06-08 2021-10-01 同济大学 Deep Learning (DL) -based cross-coupling correction D O A estimation method
CN113466782B (en) * 2021-06-08 2022-09-13 同济大学 A Deep Learning (DL)-Based Mutual Coupling Correction DOA Estimation Method
CN114624665A (en) * 2022-03-24 2022-06-14 电子科技大学 Mutual coupling error DOA self-correction method based on iterative optimization of dynamic parameters
CN114624665B (en) * 2022-03-24 2023-11-07 电子科技大学 Mutual coupling error DOA self-correction method based on dynamic parameter iterative optimization
CN115291160A (en) * 2022-08-04 2022-11-04 中国科学院微小卫星创新研究院 Two-dimensional DOA estimation method, system and computer readable medium
CN117031390A (en) * 2023-08-11 2023-11-10 哈尔滨工程大学 Gridless DOA estimation method based on antenna mutual coupling

Similar Documents

Publication Publication Date Title
CN112379327A (en) Two-dimensional DOA estimation and cross coupling correction method based on rank loss estimation
Roy et al. ESPRIT-estimation of signal parameters via rotational invariance techniques
CN108375751B (en) Multi-source direction-of-arrival estimation method
Hu et al. DOA estimation for sparse array via sparse signal reconstruction
CN112881972B (en) Direction-of-arrival estimation method based on neural network under array model error
CN106707257B (en) Direction of Arrival Estimation Method for MIMO Radar Based on Nested Array
CN110109050B (en) Unknown mutual coupling DOA estimation method based on sparse Bayes under nested array
CN107340512B (en) A passive localization method for near-far-field hybrid sources based on sub-array division
Chen et al. A DOA estimation algorithm based on eigenvalues ranking problem
CN106980106A (en) Sparse DOA estimation method under array element mutual coupling
CN105068041A (en) Single-base MIMO radar angle estimation method based on covariance vector sparse representation under cross coupling condition
CN106646376A (en) P-norm noise source positioning identification method based on weight correction parameter
CN107092007A (en) A kind of Wave arrival direction estimating method of virtual second order array extension
CN106501765B (en) A kind of Maximum Likelihood DOA Estimation based on quadratic sum and Semidefinite Programming
CN104181499A (en) Ranging passive location method under azimuth angle prior condition based on linear sparse arrays
CN107121665B (en) A kind of passive location method of the near field coherent source based on Sparse Array
CN104407335A (en) DOA estimation method of 3-axis cross array
CN105403871A (en) Bistatic MIMO radar array target angle estimation and mutual coupling error calibration method
CN106526529A (en) Sparse representation-based direction-of-arrival estimation method in mismatched condition of steering vectors
CN107656239B (en) A coherent source direction finding method based on polarization sensitive array
CN102662158A (en) Quick processing method for sensor antenna array received signals
CN111308416A (en) Near-field non-circular information source parameter estimation method based on fourth-order cumulant
CN110895325A (en) Angle of Arrival Estimation Method Based on Enhanced Quaternion Multiple Signal Classification
CN116699511A (en) Multi-frequency point signal direction of arrival estimation method, system, equipment and medium
CN107450046A (en) Direction of arrival estimation method under low elevation angle multi-path environment

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
WD01 Invention patent application deemed withdrawn after publication

Application publication date: 20210219