CN114325626A - Bistatic MIMO target positioning method based on one-bit sampling - Google Patents
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Abstract
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技术领域technical field
本发明涉及阵列信号处理技术领域,尤其涉及一种基于一比特采样的双基地MIMO目标定位方法。The invention relates to the technical field of array signal processing, in particular to a bistatic MIMO target positioning method based on one-bit sampling.
背景技术Background technique
MIMO(Multiple-Input Multiple-Output)是指在无线通信领域使用多天线发送和接收信号的技术,MIMO雷达采用多个天线同时发射相互正交的波形,并用多个天线接收来自目标的反射回波,MIMO雷达目标定位是指根据接收到的反射回波数据,利用阵列信号处理技术进行DOD和DOA的估计。在过去的十年中,由于在目标检测和定位方面的优势,MIMO雷达已引起广泛关注。MIMO (Multiple-Input Multiple-Output) refers to the technology of using multiple antennas to send and receive signals in the field of wireless communication. MIMO radar uses multiple antennas to transmit mutually orthogonal waveforms at the same time, and uses multiple antennas to receive reflected echoes from the target. , MIMO radar target positioning refers to the estimation of DOD and DOA by using array signal processing technology according to the received reflected echo data. In the past decade, MIMO radar has attracted extensive attention due to its advantages in object detection and localization.
为解决MIMO雷达目标定位参量估计问题,人们使用了众多算法,例如基于特征值分解的子空间类算法和基于信号稀疏性的压缩感知类算法,上述的两类算法均使用多比特量化数据,但存在系统的硬件成本和数据存储量要求高的问题,因此一比特量化被引入到MIMO雷达目标定位研究中,然而现有的方法只针对单基地MIMO雷达,且需要多个脉冲的数据,而对于快速移动的目标采集多个脉冲回波数据是不现实的。In order to solve the problem of MIMO radar target positioning parameter estimation, many algorithms have been used, such as the subspace algorithm based on eigenvalue decomposition and the compressed sensing algorithm based on signal sparsity. The above two types of algorithms both use multi-bit quantized data, but There are problems of high hardware cost and high data storage requirements of the system, so one-bit quantization is introduced into the research of MIMO radar target positioning. However, the existing methods are only for monostatic MIMO radar and require multiple pulse data, while for It is impractical to acquire multiple pulse echo data from a fast moving target.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供一种基于一比特采样的双基地MIMO目标定位方法,旨在克服现有技术中的针对快速移动目标很难采集多个脉冲回波数据的问题,仅需要单个脉冲的回波数据,同时使用一比特ADC对接收数据进行量化,降低系统成本和功耗。The purpose of the present invention is to provide a bistatic MIMO target locating method based on one-bit sampling, which aims to overcome the problem that it is difficult to collect multiple pulse echo data for fast moving targets in the prior art, and only needs the echo data of a single pulse. wave data, and use a one-bit ADC to quantify the received data, reducing system cost and power consumption.
为实现上述目的,本发明提供了一种基于一比特采样的双基地MIMO目标定位方法,包括下列步骤:To achieve the above object, the present invention provides a bistatic MIMO target positioning method based on one-bit sampling, comprising the following steps:
布置双基地MIMO雷达阵列;Arrange bistatic MIMO radar arrays;
使用多比特接收数据的结构构建约束,获得多比特原子范数最小化问题;Use the structure of multi-bit received data to construct constraints to obtain a multi-bit atomic norm minimization problem;
提出一比特原子范数最小化优化问题;A one-bit atomic norm minimization optimization problem is proposed;
利用MUSIC技术分别求解信号的DOA和DOD;Use MUSIC technology to solve the DOA and DOD of the signal respectively;
针对DOA和DOD进行角度配对。Angle pairing for DOA and DOD.
其中,所述双基地MIMO雷达阵列为设置在平面上的两个均匀线型阵列,对于每个接收阵元,使用一比特ADC对接收数据进行量化。Wherein, the bistatic MIMO radar array is two uniform linear arrays arranged on a plane, and for each receiving array element, a one-bit ADC is used to quantize the received data.
其中,使用多比特接收数据的结构构建约束,获得多比特原子范数最小化问题的过程,包括下列步骤:Among them, using the structure of multi-bit received data to construct constraints, the process of obtaining the multi-bit atomic norm minimization problem includes the following steps:
根据接收数据的表示式,定义一个无噪声协方差矩阵;Define a noise-free covariance matrix according to the representation of the received data;
基于无噪声协方差矩阵的结构构建原子集;Build atomic sets based on the structure of noise-free covariance matrices;
据原子范数的性质提出相应的秩最小化问题;According to the properties of atomic norm, the corresponding rank minimization problem is proposed;
将秩最小化问题凸松弛为迹的最小化,修正目标函数;The convex relaxation of the rank minimization problem is the minimization of the trace, and the objective function is modified;
引入多比特观测数据对优化问题进行约束,得到最终的多比特原子范数最小化问题。The multi-bit observation data is introduced to constrain the optimization problem, and the final multi-bit atomic norm minimization problem is obtained.
其中,在提出一比特原子范数最小化优化问题的过程中,根据一比特采样不改变原数据符号的特点,构建新的约束,再根据扰动矢量的稀疏性修正目标函数。Among them, in the process of proposing the optimization problem of one-bit atomic norm minimization, new constraints are constructed according to the characteristics that one-bit sampling does not change the original data symbol, and then the objective function is modified according to the sparsity of the disturbance vector.
其中,利用MUSIC技术分别求解信号的DOA和DOD的过程,具体为使用MUSIC谱峰搜索得到目标DOA和DOD的估计值的过程。Among them, the process of using the MUSIC technology to solve the DOA and DOD of the signal respectively is the process of using the MUSIC spectral peak search to obtain the estimated values of the target DOA and DOD.
其中,在针对DOA和DOD进行角度配对的过程中,首先分别根据DOA和DOD构造相应的阵列流型,再使用排序矩阵辅助进行配对操作。Among them, in the process of performing angle pairing for DOA and DOD, first construct corresponding array flow patterns according to DOA and DOD respectively, and then use sorting matrix to assist in pairing operation.
本发明的提供了一种基于一比特采样的双基地MIMO目标定位方法,首先布置双基地MIMO雷达阵列,再根据多比特接收数据的结构,构建优化问题的约束,同时对目标函数凸松弛,得到多比特原子范数最小化问题,然后根据一比特量化不改变数值正负的特点构建理论数据与一比特观测数据之间的约束,引入稀疏扰动向量以便求解优化问题,接着对求解优化问题得到的两个无噪声协方差矩阵分别使用MUSIC谱峰搜索得到目标DOA和DOD的估计值,最后,应用所提出的角度配对算法进行两组角度估计值的配对,发明仅需要单个脉冲的回波数据就可以实现角度估计,因此也适用于快速移动的目标,同时使用一比特数据,降低了系统成本和功耗。The present invention provides a bistatic MIMO target positioning method based on one-bit sampling. First, the bistatic MIMO radar array is arranged, and then the constraints of the optimization problem are constructed according to the structure of the multi-bit received data, and the objective function is convexly relaxed to obtain The multi-bit atomic norm minimization problem, and then construct the constraints between the theoretical data and the one-bit observation data according to the characteristic that one-bit quantization does not change the positive and negative values, and introduce sparse perturbation vectors to solve the optimization problem. The two noise-free covariance matrices use the MUSIC spectral peak search to obtain the estimated values of the target DOA and DOD. Finally, the proposed angle pairing algorithm is used to pair the two sets of angle estimates. The invention only needs the echo data of a single pulse. Angle estimation can be achieved, so it is also suitable for fast moving targets, while using one bit of data, reducing system cost and power consumption.
附图说明Description of drawings
为了更清楚地说明本发明实施例或现有技术中的技术方案,下面将对实施例或现有技术描述中所需要使用的附图作简单地介绍,显而易见地,下面描述中的附图仅仅是本发明的一些实施例,对于本领域普通技术人员来讲,在不付出创造性劳动的前提下,还可以根据这些附图获得其他的附图。In order to illustrate the embodiments of the present invention or the technical solutions in the prior art more clearly, the following briefly introduces the accompanying drawings that are used in the description of the embodiments or the prior art. Obviously, the drawings in the following description are only These are some embodiments of the present invention. For those of ordinary skill in the art, other drawings can also be obtained from these drawings without creative efforts.
图1是本发明的一种基于一比特采样的双基地MIMO目标定位方法的流程示意图。FIG. 1 is a schematic flowchart of a bistatic MIMO target positioning method based on one-bit sampling according to the present invention.
图2是本发明的双基地MIMO雷达阵列设置示意图。FIG. 2 is a schematic diagram of the arrangement of the bistatic MIMO radar array of the present invention.
图3是本发明的具体实施例的仿真实验DOA和DOD的均方根误差随SNR变化关系示意图。FIG. 3 is a schematic diagram of the variation relationship between the root mean square error of DOA and DOD in a simulation experiment with SNR according to a specific embodiment of the present invention.
图4是本发明的具体实施例的仿真实验DOA和DOD的均方根误差随采样数变化关系示意图。FIG. 4 is a schematic diagram showing the variation relationship between the root mean square error of DOA and DOD in a simulation experiment according to a specific embodiment of the present invention and the number of samples.
图5是本发明的具体实施例的仿真实验估计角度的分布示意图。FIG. 5 is a schematic diagram of distribution of estimated angles in a simulation experiment according to a specific embodiment of the present invention.
具体实施方式Detailed ways
下面详细描述本发明的实施例,所述实施例的示例在附图中示出,其中自始至终相同或类似的标号表示相同或类似的元件或具有相同或类似功能的元件。下面通过参考附图描述的实施例是示例性的,旨在用于解释本发明,而不能理解为对本发明的限制。The following describes in detail the embodiments of the present invention, examples of which are illustrated in the accompanying drawings, wherein the same or similar reference numerals refer to the same or similar elements or elements having the same or similar functions throughout. The embodiments described below with reference to the accompanying drawings are exemplary, and are intended to explain the present invention and should not be construed as limiting the present invention.
本发明涉及的相关英文术语如下,后续仅仅使用英文进行描述:The relevant English terms involved in the present invention are as follows, and follow-up only uses English to describe:
模数转换器(analog-to-digital convert,ADC);Analog-to-digital converter (analog-to-digital convert, ADC);
离去角(direction-of-departure,DOD);Departure angle (direction-of-departure, DOD);
到达角(direction-of-arrival,DOA)。Arrival angle (direction-of-arrival, DOA).
请参阅图1,本发明提出了一种基于一比特采样的双基地MIMO目标定位方法,包括下列步骤:Referring to FIG. 1, the present invention proposes a bistatic MIMO target positioning method based on one-bit sampling, including the following steps:
S1:布置双基地MIMO雷达阵列;S1: Arrange bistatic MIMO radar array;
S2:使用多比特接收数据的结构构建约束,获得多比特原子范数最小化问题;S2: Use the structure of multi-bit received data to construct constraints to obtain the multi-bit atomic norm minimization problem;
S3:提出一比特原子范数最小化优化问题;S3: Propose a one-bit atomic norm minimization optimization problem;
S4:利用MUSIC技术分别求解信号的DOA和DOD;S4: Use MUSIC technology to solve the DOA and DOD of the signal respectively;
S5:针对DOA和DOD进行角度配对。S5: Angle pairing for DOA and DOD.
所述双基地MIMO雷达阵列为设置在平面上的两个均匀线型阵列,对于每个接收阵元,使用一比特ADC对接收数据进行量化。The bistatic MIMO radar array is two uniform linear arrays arranged on a plane. For each receiving array element, a one-bit ADC is used to quantize the received data.
使用多比特接收数据的结构构建约束,获得多比特原子范数最小化问题的过程,包括下列步骤:The process of obtaining a multi-bit atomic norm minimization problem using the structure construction constraints of the multi-bit received data includes the following steps:
根据接收数据的表示式,定义一个无噪声协方差矩阵;Define a noise-free covariance matrix according to the representation of the received data;
基于无噪声协方差矩阵的结构构建原子集;Build atomic sets based on the structure of noise-free covariance matrices;
据原子范数的性质提出相应的秩最小化问题;According to the properties of atomic norm, the corresponding rank minimization problem is proposed;
将秩最小化问题凸松弛为迹的最小化,修正目标函数;The convex relaxation of the rank minimization problem is the minimization of the trace, and the objective function is modified;
引入多比特观测数据对优化问题进行约束,得到最终的多比特原子范数最小化问题。The multi-bit observation data is introduced to constrain the optimization problem, and the final multi-bit atomic norm minimization problem is obtained.
在提出一比特原子范数最小化优化问题的过程中,根据一比特采样不改变原数据符号的特点,构建新的约束,并修正目标函数。In the process of proposing the one-bit atomic norm minimization optimization problem, new constraints are constructed and the objective function is modified according to the characteristic that one-bit sampling does not change the original data symbol.
利用MUSIC技术分别求解信号的DOA和DOD的过程,具体为使用MUSIC谱峰搜索得到目标DOA和DOD的估计值的过程。The process of using MUSIC technology to solve the DOA and DOD of the signal respectively, specifically the process of using the MUSIC spectral peak search to obtain the estimated values of the target DOA and DOD.
在针对DOA和DOD进行角度配对的过程中,首先分别根据DOA和DOD构造相应的阵列流型,再使用排序矩阵辅助进行配对操作。In the process of angle pairing for DOA and DOD, the corresponding array flow pattern is first constructed according to DOA and DOD respectively, and then the pairing operation is performed with the assistance of sorting matrix.
具体地,下面结合实施方式和附图,对本发明的算法作进一步地详细描述:Specifically, below in conjunction with embodiment and accompanying drawing, the algorithm of the present invention is described in further detail:
步骤1:设置天线阵列:Step 1: Set up the antenna array:
设置一个如图1所示的双基地MIMO雷达系统,每个接收阵元均使用一比特ADC对接收数据进行量化。发射阵列的阵元数为M,阵列间距d。接收阵列的阵元数为N,阵列间距也为d。λ是信号波长。本实施方式有K个目标,信号被建模为窄带不相关正交编码信号。接收阵列阵元上的噪声为零均值加性高斯白噪声,且噪声独立于信号。A bistatic MIMO radar system as shown in Figure 1 is set up, and each receiving array element uses a one-bit ADC to quantize the received data. The number of elements of the transmitting array is M, and the array spacing is d. The number of elements of the receiving array is N, and the array spacing is also d. λ is the signal wavelength. This embodiment has K targets and the signal is modeled as a narrowband uncorrelated quadrature coded signal. The noise on the receiving array elements is zero-mean additive white Gaussian noise, and the noise is independent of the signal.
因此,进行一比特量化操作之前,接收阵列在t时刻接收到的数据可以表示为:Therefore, before the one-bit quantization operation, the data received by the receiving array at time t can be expressed as:
其中,Q是全部的脉冲个数,βk表示第k个目标的反射系数,ωk=(2πvkTp)/λ是相应的多普勒频率,vk代表目标移动速度,Tp代表脉冲持续时间,s(t)=[s1(t),...,sM(t)]T表示发射波形向量,(·)T表示转置,zq(t)∈CN表示加性高斯噪声向量,a(φ)和b(θ)代表发射和接收阵列流型,有下列形式:Among them, Q is the total number of pulses, β k is the reflection coefficient of the k-th target, ω k =(2πv k T p )/λ is the corresponding Doppler frequency, v k is the moving speed of the target, and T p is the Pulse duration, s(t)=[s 1 (t),...,s M (t)] T represents the transmitted waveform vector, ( ) T represents the transpose, z q (t)∈C N represents the addition The Gaussian noise vector, a(φ) and b(θ) represent the transmit and receive array flow patterns, and have the following forms:
a(φ)=[1,ej(2πdsinφλ),...,ej(2π(M-1)dsinφ/λ)]T a(φ)=[1,e j(2πdsinφλ) ,...,e j(2π(M-1)dsinφ/λ) ] T
b(θ)=[1,ej(2πdsinθλ),...,ej(2π(N-1)dsinθ/λ)]T b(θ)=[1,e j(2πdsinθλ) ,...,e j(2π(N-1)dsinθ/λ) ] T
其中,θ和φ是信号的DOA和DOD参数。where θ and φ are the DOA and DOD parameters of the signal.
将一比特量化前的阵列观测数据表示成矩阵形式为:The array observation data before one-bit quantization is expressed in matrix form as:
Xq=BΣΔqATS+Zq X q =BΣΔ q A T S+Z q
其中,S=[s(0),s(Ts),...,s((L-1)Ts)]∈CM×L为发射数据矩阵,Ts表示采样间隔,L表示一个脉冲内的采样数,Zq∈CN×L代表包含噪声和量化误差的复矩阵,A=[a(φ1),...,a(φK)]∈CM×K和B=[b(θ1),...,b(θK)]∈CN×K分别代表发射和接收阵列流型矩阵,Σ和Δq是两个对角矩阵,有如下结构:Among them, S=[s(0),s(T s ),...,s((L-1)T s )]∈C M×L is the transmit data matrix, T s represents the sampling interval, and L represents a The number of samples within a pulse, Z q ∈ C N×L represents the complex matrix containing noise and quantization error, A=[a(φ 1 ),...,a(φ K )]∈C M×K and B= [b(θ 1 ),...,b(θ K )]∈C N×K represent the transmit and receive array flow pattern matrices, respectively, Σ and Δ q are two diagonal matrices with the following structure:
Σ=diag([β1,...,βK])Σ=diag([β 1 ,...,β K ])
当考虑一比特量化时,观测数据矩阵为:When considering one-bit quantization, the observed data matrix is:
Yq=Q1(Xq-Hq)Y q =Q 1 (X q -H q )
其中,Hq为已知的量化阈值,表示复值量化函数,sign(·)表示符号函数,和分别表示复矩阵的实部和虚部。Among them, H q is the known quantization threshold, represents a complex-valued quantization function, sign( ) represents a sign function, and represent the real and imaginary parts of a complex matrix, respectively.
步骤2:提出多比特原子范数最小化优化问题:Step 2: Formulate the multi-bit atomic norm minimization optimization problem:
本发明采用原子范数最小化技术,需要根据观测数据确定一个原子集。为此,首先观察观测数据中的无噪声部分,并定义无噪声协方差矩阵:The invention adopts the atomic norm minimization technology, and needs to determine an atomic set according to the observation data. To do this, first look at the noise-free part of the observed data and define the noise-free covariance matrix:
此时,多比特观测矩阵可写成:At this point, the multi-bit observation matrix can be written as:
Xq=RqS+Zq X q =R q S+Z q
相应的原子集可以被定义为:The corresponding set of atoms can be defined as:
而Rq的原子l0范数就是指可以表示Rq的G中最少的原子的个数,即The atomic l 0 norm of R q refers to the minimum number of atoms in G that can represent R q , namely
根据原子范数的性质,上式可以通过如下一个半正定最优化问题计算:According to the properties of the atomic norm, the above formula can be calculated by a positive semi-definite optimization problem as follows:
其中,Tu1和Tu2分别为以u1和u2为第一列,构建的Hermitian Toeplitz矩阵。Among them, Tu 1 and Tu 2 are Hermitian Toeplitz matrices constructed with u 1 and u 2 as the first column, respectively.
将上式的NP-hard的矩阵H的秩最小化问题凸松弛为迹的最小化,也就是说将目标函数变为tr(Tu1)+tr(Tu2),并引入有噪声的多比特观测数据对Rq进行约束,得到最终的多比特原子范数最小化问题:Convex relaxation of the rank minimization problem of the NP-hard matrix H of the above formula to minimize the trace, that is to say, change the objective function to tr(Tu 1 )+tr(Tu 2 ), and introduce noisy multi-bit The observation data constrains R q to obtain the final multi-bit atomic norm minimization problem:
||Xq-RqS||F≤ε||X q -R q S|| F ≤ε
其中,ε为一个受噪声和量化误差影响的自定义参数,||·||F为Frobenius范数。where ε is a custom parameter affected by noise and quantization error, and ||·|| F is the Frobenius norm.
步骤3:提出一比特原子范数最小化优化问题:Step 3: Propose a one-bit atomic norm minimization optimization problem:
首先有Yq=Q1(Xq-Hq)=Q1(RqS+Zq-Hq),列向量化后得到vec(Yq)=vec(Q1(RqS+Zq-Hq))。First, Y q =Q 1 (X q -H q )=Q 1 (R q S+Z q -H q ), after column vectorization, vec(Y q )=vec(Q 1 (R q S+Z q -H q )).
在多比特原子范数最小化问题的基础上,根据一比特采样不改变原数据符号的特点,构建新的约束Based on the multi-bit atomic norm minimization problem, a new constraint is constructed according to the characteristic that one-bit sampling does not change the original data symbol
再引入稀疏扰动矢量pq,用于消除zq中未知的随机噪声和量化误差的影响,然后一比特约束可以被更新为:A sparse perturbation vector p q is then introduced to remove the effects of unknown random noise and quantization errors in z q , and then the one-bit constraint can be updated as:
这里,pq是一个与zq同维度的稀疏矢量参量,为了加强扰动向量pq的稀疏性,需要对目标函数作出修改,最终得到如下一比特原子范数最小化问题,求解出u1,u2和Rq Here, p q is a sparse vector parameter with the same dimension as z q . In order to enhance the sparsity of the perturbation vector p q , the objective function needs to be modified. Finally, the following one-bit atomic norm minimization problem is obtained, and u 1 is solved, u 2 and R q
其中,||·||1代表向量一范数。Among them, ||·|| 1 represents the vector one norm.
步骤4:利用MUSIC技术分别求解信号的DOA和DOD:Step 4: Use the MUSIC technique to solve the DOA and DOD of the signal separately:
将T(u1)和T(u2)特征分解,有Decomposing T(u 1 ) and T(u 2 ) features, we have
其中,(·)H表示共轭转置,Usr是N×K维的接收信号子空间,由Tu1的K个最大特征值对应的特征向量张成。Σsr是K×K维的对角矩阵,包含了Tu1的K个最大特征值。Unr是N×(N-K)维的接收噪声子空间,由Tu1的(N-K)个最小特征值对应的特征向量张成。Σnr是(N-K)×(N-K)维的对角矩阵,包含了Tu1的(N-K)个最小特征值。Ust是M×K维的发射信号子空间,由Tu2的K个最大特征值对应的特征向量张成。Σst是K×K维的对角矩阵,包含了Tu2的K个最大特征值。Unt是M×(M-K)维的发射噪声子空间,由Tu2的(M-K)个最小特征值对应的特征向量张成。Σnt是(M-K)×(M-K)维的对角矩阵,包含了Tu2的(M-K)个最小特征值。Among them, (·) H represents the conjugate transpose, and U sr is the N×K-dimensional received signal subspace, which is stretched by the eigenvectors corresponding to the K largest eigenvalues of Tu 1 . Σ sr is a K × K dimensional diagonal matrix that contains the K largest eigenvalues of Tu 1 . Unr is an N×(NK) dimensional received noise subspace, which is stretched by the eigenvectors corresponding to the (NK) smallest eigenvalues of Tu 1 . Σ nr is a (NK)×(NK) dimensional diagonal matrix that contains the (NK) smallest eigenvalues of Tu 1 . U st is an M×K dimensional transmitted signal subspace, stretched by the eigenvectors corresponding to the K largest eigenvalues of Tu 2 . Σ st is a K × K dimensional diagonal matrix that contains the K largest eigenvalues of Tu 2 . U nt is an M×(MK) dimensional emission noise subspace, stretched by the eigenvectors corresponding to the (MK) smallest eigenvalues of Tu 2 . Σ nt is a (MK) × (MK) dimensional diagonal matrix containing the (MK) smallest eigenvalues of Tu 2 .
然后,利用MUSIC谱峰搜索可以分别得到DOA和DOD估计:Then, DOA and DOD estimates can be obtained, respectively, using MUSIC peak search:
其中,(·)*表示共轭。where (·) * represents conjugation.
步骤5:角度配对:Step 5: Angle Pairing:
因为步骤2和步骤3估计出的无噪声协方差矩阵可以被近似表示为:Because the noise-free covariance matrix estimated in
即当两组角度是配对成功时,排序矩阵Λ是对角矩阵。且根据上式可得到排序矩阵的近似估计值That is, when the two sets of angles are paired successfully, the sorting matrix Λ is a diagonal matrix. And according to the above formula, the approximate estimated value of the sorting matrix can be obtained
可以以此为依据进行角度配对,其中表示伪逆。Angle pairing can be performed based on this, where represents the pseudo-inverse.
具体方法是以接受阵列流型B为基准,用估计出的DOA角度以任意的角度顺序构造接收阵列流型然后用估计出的DOD角度以全部的排列组合形式构造所有可能的阵列流型(共K!种结果,其中(·)!表示阶乘)。再将通过求解步骤2或步骤3的优化问题估计出的无噪声协方差矩阵构造出的和全部的K!个代入上面Λ的估计式中,求出K!个排序矩阵Λ的估计值,找到其中K个最大的元素位于对角线上的Λ。求出这个Λ的和为配对好的发射和接收阵列流型,这两个阵列流型相同列序号包含的角度就对应于同一目标。分别找到这K组列向量对应的K对角度,即完成配对操作。The specific method is to accept the array flow pattern B as the benchmark, and use the estimated DOA angle Construct receive array manifolds in arbitrary angular order Then use the estimated DOD angle Construct all possible array manifolds in all permutations and combinations (A total of K! kinds of results, where (·)! represents factorial). Then the noise-free covariance matrix estimated by solving the optimization problem of
进一步地,本发明还设计了三组仿真实验,实验结果请参阅图3、图4和图5。第一组实验为所提出的一比特原子范数最小化算法(实验中简称为1b-ANM算法)、所提出的多比特原子范数最小化算法(实验中简称为mb-ANM算法)、有效阵列孔径扩展技术(实验中简称为EAET算法)[8]在单个脉冲内的采样数为128的情况下,DOA与DOD估计均方根误差随信噪比的变化关系。第二组实验是信噪比为10dB的条件下将mb-ANM算法和EAET算法单个脉冲内的采样数固定为32,而1b-ANM算法的采样数逐渐增大,此时的DOA与DOD估计均方根误差随采样数的变化关系。第三组实验给出了信噪比为10dB时,1b-ANM算法角度估计值的分布图,用于验证所提出角度配对步骤的有效性。Further, three groups of simulation experiments are also designed in the present invention. Please refer to FIG. 3 , FIG. 4 and FIG. 5 for the experimental results. The first set of experiments are the proposed one-bit atomic norm minimization algorithm (referred to as 1b-ANM algorithm in the experiment), the proposed multi-bit atomic norm minimization algorithm (abbreviated as mb-ANM algorithm in the experiment), effective Array aperture expansion technology (referred to as EAET algorithm in the experiment) [8] shows the relationship between the root mean square error of DOA and DOD estimation with the signal-to-noise ratio when the number of samples in a single pulse is 128. The second set of experiments is that the number of samples in a single pulse of the mb-ANM algorithm and the EAET algorithm is fixed to 32 under the condition of a signal-to-noise ratio of 10dB, while the number of samples of the 1b-ANM algorithm gradually increases. At this time, the DOA and DOD estimates Root mean square error as a function of the number of samples. The third group of experiments gives the distribution of the angle estimates of the 1b-ANM algorithm when the signal-to-noise ratio is 10dB, which is used to verify the effectiveness of the proposed angle pairing step.
三组实验的随机实验次数均为100,所用阵列相同,接收和发射阵列阵元数同为18,阵列间距为d=λ/2,Hq的实部和虚部服从同一均匀分布。前两组实验入射的目标个数为K=2,目标角度分别为(0°,30°)和(20°,40°)。第三组实验入射的目标个数为K=8,目标角度分别为(-60°,-20°),(-40°,50°),(-30°,-50°),(-10°,0°),(10°,-10°),(20°,40°),(40°,-40°)和(50°,20°)。第k个目标的多普勒频率被设置为ωk=0.1k,反射系数βk的幅度被设置为1,相位在[0,2π]内均匀分布。The number of random experiments in the three groups of experiments are all 100, the arrays used are the same, the number of receiving and transmitting array elements is 18, the array spacing is d=λ/2, and the real and imaginary parts of H q obey the same uniform distribution. The number of incident targets in the first two groups of experiments is K=2, and the target angles are (0°, 30°) and (20°, 40°) respectively. The number of incident targets in the third group of experiments is K=8, and the target angles are (-60°, -20°), (-40°, 50°), (-30°, -50°), (-10 °, 0°), (10°, -10°), (20°, 40°), (40°, -40°) and (50°, 20°). The Doppler frequency of the k-th target is set to ω k =0.1k, the magnitude of the reflection coefficient β k is set to 1, and the phase is uniformly distributed in [0, 2π].
以上所揭露的仅为本发明一种较佳实施例而已,当然不能以此来限定本发明之权利范围,本领域普通技术人员可以理解实现上述实施例的全部或部分流程,并依本发明权利要求所作的等同变化,仍属于发明所涵盖的范围。The above disclosure is only a preferred embodiment of the present invention, and of course, it cannot limit the scope of rights of the present invention. Those of ordinary skill in the art can understand that all or part of the process of implementing the above embodiment can be realized according to the rights of the present invention. The equivalent changes required by the invention still belong to the scope covered by the invention.
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