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CN103954942A - Method for partial combination clutter suppression in airborne MIMO radar three-dimensional beam space - Google Patents

Method for partial combination clutter suppression in airborne MIMO radar three-dimensional beam space Download PDF

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CN103954942A
CN103954942A CN201410171717.2A CN201410171717A CN103954942A CN 103954942 A CN103954942 A CN 103954942A CN 201410171717 A CN201410171717 A CN 201410171717A CN 103954942 A CN103954942 A CN 103954942A
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dimensionality reduction
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冯大政
向平叶
吕晖
周延
解虎
肖春宝
白登潘
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Xidian University
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    • 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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/023Interference mitigation, e.g. reducing or avoiding non-intentional interference with other HF-transmitters, base station transmitters for mobile communication or other radar systems, e.g. using electro-magnetic interference [EMI] reduction techniques
    • 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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/28Details of pulse systems
    • G01S7/285Receivers
    • G01S7/292Extracting wanted echo-signals
    • G01S7/2923Extracting wanted echo-signals based on data belonging to a number of consecutive radar periods
    • 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
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/42Diversity systems specially adapted for radar

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  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Computer Networks & Wireless Communication (AREA)
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  • General Physics & Mathematics (AREA)
  • Radar Systems Or Details Thereof (AREA)

Abstract

本发明属于雷达信号处理技术领域,涉及雷达杂波的局域化抑制处理,公开了一种机载MIMO雷达三维波束空间的部分联合杂波抑制方法。该方法包括:步骤1.得到空时数据矢量x表达式并且构建目标的空时二维导向矢量;步骤2.利用三维离散傅里叶变换将空时数据矢量x由阵元-脉冲域变换到三维波束域;步骤3.得到降维后的空时数据矢量z和降维后的目标空时二维导向矢量;步骤4.根据降维空时自适应处理的代价函数计算降维处理器的权矢量;步骤5.利用降维处理器的权矢量得到经过杂波抑制的空时数据。本发明能够解决运算量大与样本需求量大的问题,应用于雷达杂波处理的情景。

The invention belongs to the technical field of radar signal processing, relates to localized suppression processing of radar clutter, and discloses a partly combined clutter suppression method in three-dimensional beam space of an airborne MIMO radar. The method includes: Step 1. Obtain the space-time data vector x expression and construct the space-time two-dimensional steering vector of the target; Step 2. Use the three-dimensional discrete Fourier transform to transform the space-time data vector x from the array element-pulse domain to Three-dimensional beam domain; Step 3. Obtain the space-time data vector z after dimensionality reduction and the target space-time two-dimensional steering vector after dimensionality reduction; Step 4. Calculate the dimensionality reduction processor according to the cost function of dimensionality reduction space-time adaptive processing Weight vector; Step 5. Using the weight vector of the dimensionality reduction processor to obtain space-time data that has undergone clutter suppression. The invention can solve the problems of large calculation amount and large sample demand, and is applied to the scenario of radar clutter processing.

Description

机载MIMO雷达三维波束空间的部分联合杂波抑制方法Partial Joint Clutter Suppression Method in Three-Dimensional Beam Space of Airborne MIMO Radar

技术领域technical field

本发明属于雷达信号处理技术领域,涉及雷达杂波的局域化抑制处理,特别涉及一种机载MIMO雷达三维波束空间的部分联合杂波抑制方法。The invention belongs to the technical field of radar signal processing, and relates to localized suppression processing of radar clutter, in particular to a partial combined clutter suppression method in three-dimensional beam space of an airborne MIMO radar.

背景技术Background technique

自从MIMO雷达成为下一代雷达的发展方向以来,MIMO雷达也成为当前研究的热点。MIMO雷达在发射端和接收端同时采用数字阵技术,发射多个正交或非相干信号,并在接收端利用匹配滤波分离各发射信号分量,MIMO雷达利用较小的天线规模就可以获得很大的虚拟阵列孔径和系统自由度,从而大幅度提高雷达的参数估计精度、角度分辨率和杂波抑制能力。由于MIMO雷达在发射端和接收端同时采用了数字阵技术,MIMO雷达在抗杂波、抗干扰、低截获等性能方面,与传统雷达相比具有明显的优势。Since MIMO radar has become the development direction of the next-generation radar, MIMO radar has also become a current research hotspot. MIMO radar uses digital array technology at the transmitter and receiver at the same time, transmits multiple orthogonal or incoherent signals, and uses matched filtering to separate the transmitted signal components at the receiver. MIMO radar can obtain a large The virtual array aperture and system degrees of freedom can greatly improve the radar parameter estimation accuracy, angular resolution and clutter suppression ability. Since MIMO radar adopts digital array technology at both the transmitting end and receiving end, MIMO radar has obvious advantages compared with traditional radar in terms of anti-clutter, anti-interference, low interception and other performance.

空时自适应处理(Space Time Adaptive Processing,STAP)是机载预警雷达检测慢速运动目标的关键技术,但受到高维数据协方差矩阵求逆导致的运算量大和要求的独立分布样本庞大等影响,使得其在实际应用中难以实现。在相控阵雷达体制下,人们已经提出许多旨在降低样本数目需求和运算量的降维STAP方法,如主分量方法(Principle Component,PC)、因子化方法(Factored Approach,FA)以及扩展因子方法(Extended Factored Approach,EFA)等。PC法的基本思想是利用杂波子空间的特征基向量对消主支路的杂波;FA法是先采用一组具有高带外衰减的多普勒滤波器对MIMO雷达各接收阵元的输出进行滤波,然后使用空域Capon波束形成对相同多普勒通道的输出进行自适应处理;EFA法是在主杂波区附近联合m(m通常取奇数3、5等)个多普勒通道进行自适应处理。虽然这些方法同样适用于机载MIMO雷达,但由于发射波形分集的缘故,MIMO-STAP将传统的空—时二维处理扩展到空—时—码(波形)三维空间,数据维数的急剧增加导致运算量和协方差矩阵估计等问题变得更加突出,简单地运用这些方法仍难以满足实时性的要求,急剧增加的数据维数使得样本需求量(即独立同分布参考单元数)庞大以及协方差矩阵估计和求逆时运算量也会很大,也就是现有技术中受到运算量大与样本需求量大的制约。因此,迫切需要针对机载MIMO雷达研究更高效的降维STAP方法。Space Time Adaptive Processing (STAP) is a key technology for airborne early warning radars to detect slow-moving targets, but it is affected by the large amount of calculations caused by the inversion of the high-dimensional data covariance matrix and the large number of independent distribution samples required. , making it difficult to realize in practical applications. Under the system of phased array radar, people have proposed many dimensionality reduction STAP methods aimed at reducing the number of samples and the amount of computation, such as the principal component method (Principle Component, PC), the factorization method (Factored Approach, FA) and the expansion factor Method (Extended Factored Approach, EFA), etc. The basic idea of the PC method is to use the eigenvectors of the clutter subspace to cancel the clutter of the main branch; the FA method first uses a set of Doppler filters with high out-of-band attenuation to output the output of each receiving element of the MIMO radar. Filter, and then use the spatial domain Capon beamforming to adaptively process the output of the same Doppler channel; the EFA method combines m (m usually takes an odd number of 3, 5, etc.) Doppler channels for self-adaptive processing near the main clutter area. Adapt to handling. Although these methods are also applicable to airborne MIMO radar, due to the transmit waveform diversity, MIMO-STAP extends the traditional space-time two-dimensional processing to the space-time-code (waveform) three-dimensional space, and the data dimension increases sharply. As a result, problems such as computation load and covariance matrix estimation have become more prominent. Simply using these methods is still difficult to meet the real-time requirements. The amount of computation for estimating and inverting the variance matrix will also be very large, that is, the prior art is restricted by a large amount of computation and a large demand for samples. Therefore, there is an urgent need to study more efficient dimensionality-reduced STAP methods for airborne MIMO radars.

发明内容Contents of the invention

针对现有方法应用于机载MIMO雷达杂波抑制时,本发明提出一种机载MIMO雷达三维波束空间的部分联合杂波抑制方法,用于解决运算量大与样本需求量大的问题。When the existing method is applied to airborne MIMO radar clutter suppression, the present invention proposes a partly combined clutter suppression method in the three-dimensional beam space of airborne MIMO radar, which is used to solve the problems of large calculation amount and large sample demand.

为达到上述目的,本发明采用以下技术方案预以实现。In order to achieve the above object, the present invention adopts the following technical solutions to realize.

一种机载MIMO雷达三维波束空间的部分联合杂波抑制方法,其特征在于,包括以下步骤:A partial joint clutter suppression method in three-dimensional beam space of airborne MIMO radar, is characterized in that, comprises the following steps:

步骤1.利用机载MIMO雷达天线接收空时数据,得到空时数据矢量x表达式并且构建目标的空时二维导向矢量b(fs,0,fd,0);Step 1. Use the airborne MIMO radar antenna to receive space-time data, obtain the space-time data vector x expression and construct the space-time two-dimensional steering vector b(f s,0 ,f d,0 );

步骤2.利用三维离散傅里叶变换将空时数据矢量x由阵元-脉冲域变换到三维波束域;空时数据矢量x在三维波束域中称为三维波束;Step 2. Utilize the three-dimensional discrete Fourier transform to transform the space-time data vector x from the array element-pulse domain to the three-dimensional beam domain; the space-time data vector x is called a three-dimensional beam in the three-dimensional beam domain;

步骤3.构造降维矩阵P,利用降维矩阵P对三维波束域中的三维波束进行部分联合自适应处理,得到降维后的空时数据矢量z和降维后的目标空时二维导向矢量c(fs,0,fd,0);Step 3. Construct the dimensionality reduction matrix P, and use the dimensionality reduction matrix P to perform partial joint adaptive processing on the 3D beams in the 3D beam domain to obtain the space-time data vector z after dimensionality reduction and the target space-time two-dimensional guidance after dimensionality reduction vector c(f s,0 ,f d,0 );

步骤4.根据线性约束最小方差准则,即在保证目标信号增益一定的前提下最小化输出的杂波和噪声功率,利用降维后的空时数据矢量z和降维后的目标空时二维导向矢量c(fs,0,fd,0)构建降维空时自适应处理的代价函数;根据降维空时自适应处理的代价函数计算降维处理器的权矢量w;Step 4. According to the linear constraint minimum variance criterion, that is, to minimize the output clutter and noise power under the premise of ensuring a certain target signal gain, use the dimensionally reduced space-time data vector z and the dimensionally reduced target space-time two-dimensional Steering vector c(f s,0 ,f d,0 ) constructs the cost function of dimensionality reduction space-time adaptive processing; calculates the weight vector w of dimensionality reduction processor according to the cost function of dimensionality reduction space-time adaptive processing;

步骤5.利用降维处理器的权矢量w对机载MIMO雷达天线接收的空时数据矢量x进行加权求和,得到经过杂波抑制的空时数据。Step 5. Use the weight vector w of the dimensionality reduction processor to weight and sum the space-time data vector x received by the airborne MIMO radar antenna to obtain the space-time data after clutter suppression.

上述技术方案的特点和进一步改进在于:The characteristics and further improvement of the above-mentioned technical scheme are:

(1)步骤1包括以下子步骤:(1) Step 1 includes the following sub-steps:

1a)设定在一个相干处理间隔内,机载MIMO雷达天线的M个发射阵元同时辐射由K个脉冲组成的脉冲串波形,并且M个发射阵元发射的M个发射波形相互正交,在N个接收阵元的每一个接收阵元处,用M个参考发射信号对K个脉冲周期的回波数据进行匹配滤波,将所有匹配滤波器的输出排列成如下MNK×1维空时数据矢量,得到空时数据矢量x表达式为下式:1a) It is set that within a coherent processing interval, the M transmitting elements of the airborne MIMO radar antenna simultaneously radiate a burst waveform composed of K pulses, and the M transmitting waveforms emitted by the M transmitting elements are orthogonal to each other, At each of the N receiving array elements, M reference transmitting signals are used to perform matched filtering on the echo data of K pulse periods, and the outputs of all matched filters are arranged into the following MNK×1-dimensional space-time data Vector, the expression of the space-time data vector x is obtained as the following formula:

xx == ∫∫ 00 ππ ρρ (( θθ )) bb (( ff sthe s ,, ff dd )) dθdθ ++ xx ww

其中,空时数据矢量x的维数为MNK×1维,是服从零均值复高斯分布的杂波散射系数;表示归一化杂波多普勒频率,Tr为脉冲重复周期,λ为雷达天线工作波长,v为载机速度,θ表示观测地面的方位角,为俯仰角;表示归一化杂波空间频率; b ( f s , f d ) = a d ( f d ) ⊗ a t ( f s ) ⊗ a r ( f s ) 为空时数据x中的杂波的空时二维导向矢量,其中at(fs)=[1 exp(j2πfsα)…exp(j2πfsα(M-1))]T为M×1维发射阵列导向矢量,α=dT/dR,M为发射阵元数,N为接收阵元数,K为发射脉冲数,dT为发射阵元间距,dR为接收阵元间距;ar(fs)=[1 exp(j2πfs)…exp(j2πfs(N-1))]T为N×1维接收阵列导向矢量,ad(fd)=[1 exp(j2πfd)…exp(j2πfd(K-1))]T为K×1维多普勒导向矢量;表示Kronecker积;是服从0均值,方差为的MNK×1维高斯白噪声向量,IMNK代表MNK×MNK单位矩阵,分别表示输入杂波功率和噪声功率,(·)T表示向量转置;Among them, the dimension of space-time data vector x is MNK×1 dimension, is the clutter scattering coefficient that obeys the zero-mean complex Gaussian distribution; Indicates the normalized clutter Doppler frequency, T r is the pulse repetition period, λ is the working wavelength of the radar antenna, v is the speed of the carrier aircraft, θ is the azimuth angle of the observed ground, is the pitch angle; Indicates the normalized clutter spatial frequency; b ( f the s , f d ) = a d ( f d ) ⊗ a t ( f the s ) ⊗ a r ( f the s ) is the space-time two-dimensional steering vector of the clutter in the space-time data x, where a t (f s )=[1 exp(j2πf s α)…exp(j2πf s α(M-1))] T is M× 1-dimensional transmitting array steering vector, α=d T /d R , M is the number of transmitting array elements, N is the number of receiving array elements, K is the number of transmitting pulses, d T is the distance between transmitting array elements, and d R is the distance between receiving array elements ; a r (f s )=[1 exp(j2πf s )…exp(j2πf s (N-1))] T is N×1-dimensional receiving array steering vector, a d (f d )=[1 exp(j2πf d )...exp(j2πf d (K-1))] T is the K×1 dimensional Doppler steering vector; Indicates the Kronecker product; is subject to 0 mean, variance is The MNK×1-dimensional Gaussian white noise vector, I MNK represents the MNK×MNK identity matrix, and Respectively represent the input clutter power and noise power, ( ) T represents the vector transpose;

1b)构建目标的空时二维导向矢量 b ( f s , 0 , f d , 0 ) = a d ( f d , 0 ) ⊗ a t ( f s , 0 ) ⊗ a r ( f s , 0 ) ; 1b) Construct the space-time two-dimensional guidance vector of the target b ( f the s , 0 , f d , 0 ) = a d ( f d , 0 ) ⊗ a t ( f the s , 0 ) ⊗ a r ( f the s , 0 ) ;

其中,ad(fd,0)为目标多普勒导向矢量,at(fs,0)为发射阵列导向矢量,ar(fs,0)为接收阵列导向矢量,fd,0为目标的多普勒频率,fs,0为目标的归一化空间频率,表示Kronecker积。Among them, a d (f d,0 ) is the target Doppler steering vector, at (f s,0 ) is the transmitting array steering vector, a r ( f s,0 ) is the receiving array steering vector, f d,0 is the Doppler frequency of the target, f s,0 is the normalized spatial frequency of the target, Represents the Kronecker product.

(2)步骤3包括以下子步骤:(2) Step 3 includes the following sub-steps:

3a)构造降维矩阵P,降维矩阵P表示为3a) Construct a dimensionality reduction matrix P, and the dimensionality reduction matrix P is expressed as

PP == GG dd ⊗⊗ GG tt ⊗⊗ GG rr

其中,Gd=[ad(fd,-1),ad(fd,0),ad(fd,1)]为三个邻近的多普勒导向矢量组成的多普勒滤波器组,Gt=[at(fs,-1),at(fs,0),at(fs,1)]为三个邻近的发射阵列导向矢量组成的发射波束形成器组,Gr=[ar(fs,-1),ar(fs,0),ar(fs,1)]为三个邻近的接收阵列导向矢量组成的接收波束形成器组,表示Kronecker积;Among them, G d =[a d (f d,-1 ), a d (f d,0 ), a d (f d,1 )] is the Doppler filter composed of three adjacent Doppler steering vectors G t =[a t (f s,-1 ), at (f s,0 ), at (f s,1 )] is the transmit beamformer composed of three adjacent transmit array steering vectors group, G r =[a r (f s,-1 ), a r (f s,0 ), a r (f s,1 )] is the receiving beamformer group composed of three adjacent receiving array steering vectors , Indicates the Kronecker product;

3b)从三维波束域中选择3个或5个三维波束;3b) Select 3 or 5 3D beams from the 3D beam field;

3c)利用降维矩阵P对选择的三维波束根据下式进行部分联合自适应处理,得到空时数据矢量x降维后的空时数据矢量z;得到下式:3c) Using the dimensionality reduction matrix P to perform partial joint adaptive processing on the selected three-dimensional beams according to the following formula, to obtain the space-time data vector z after dimensionality reduction of the space-time data vector x; obtain the following formula:

z=PHxz = P H x

其中,P为降维矩阵,z为空时数据矢量x降维后的空时数据矢量,(·)H表示矩阵或向量的复共轭转置;Among them, P is the dimensionality reduction matrix, z is the space-time data vector after dimensionality reduction of the space-time data vector x, ( ) H represents the complex conjugate transposition of the matrix or vector;

3d)根据降维矩阵P和目标空时二维导向矢量b(fs,0,fd,0)求取降维后的目标空时二维导向矢量c(fs,0,fd,0),得到下式:3d) Calculate the dimensionality-reduced target space-time two-dimensional steering vector c(f s ,0 ,f d , 0 ), get the following formula:

c(fs,0,fd,0)=PHb(fs,0,fd,0)c(f s,0 ,f d,0 )=P H b(f s,0 ,f d,0 )

其中,c(fs,0,fd,0)为目标空时二维导向矢量b(fs,0,fd,0)降维后的目标空时二维导向矢量;降维矩阵P维数为MNK×rMrNrK,rM表示选取的发射波束的数目,rN表示选取的接收波束的数目,rK表示选取的多普勒通道数目;其中rM为大于或等于3并且小于M的整数,rN为大于或等于3并且小于N的整数,rK为大于或等于3并且小于K的整数,fd,0为目标的多普勒频率,fs,0为目标的归一化空间频率,(·)H表示矩阵或向量的复共轭转置,M为发射阵元数,N为接收阵元数,K为发射脉冲数。Among them, c(f s,0 ,f d,0 ) is the target space-time two-dimensional steering vector after dimension reduction of the target space-time two-dimensional steering vector b(f s,0 ,f d,0 ); the dimensionality reduction matrix P The dimension is MNK×r M r N r K , where r M represents the number of selected transmit beams, r N represents the number of selected receive beams, and r K represents the number of selected Doppler channels; where r M is greater than or equal to r N is an integer greater than or equal to 3 and less than N, r K is an integer greater than or equal to 3 and less than K, f d,0 is the Doppler frequency of the target, f s,0 is The normalized spatial frequency of the target, (·) H represents the complex conjugate transpose of a matrix or vector, M is the number of transmitting array elements, N is the number of receiving array elements, and K is the number of transmitting pulses.

(3)步骤4包括以下子步骤:(3) Step 4 includes the following sub-steps:

4a)利用降维后的空时数据矢量z求取降维后的空时数据矢量z的协方差矩阵Rz,Rz表达式为:4a) Use the space-time data vector z after dimension reduction to obtain the covariance matrix R z of the space-time data vector z after dimension reduction, and the expression of R z is :

Rz=E{zzH}=PHRPR z =E{zz H }=P H RP

其中,z表示降维后的空时数据矢量,P为降维矩阵,R为空时数据x的协方差矩阵,(·)H表示矩阵或向量的复共轭转置,E{·}表示进行期望操作;Among them, z represents the space-time data vector after dimensionality reduction, P is the dimensionality reduction matrix, R is the covariance matrix of space-time data x, ( ) H represents the complex conjugate transpose of matrix or vector, E{ } represents perform the desired operation;

4b)根据线性约束最小方差准则,将降维空时自适应处理的代价函数表示为:4b) According to the linearly constrained minimum variance criterion, the cost function of dimensionality reduction space-time adaptive processing is expressed as:

minmin ww Hh RR zz ww sthe s .. tt .. ww Hh cc (( ff sthe s ,, 00 ,, ff dd ,, 00 )) == 11

其中,Rz为降维后的空时数据矢量z的协方差矩阵,维数为rMrNrK;rM表示选取的发射波束的数目,rN表示选取的接收波束的数目,rK表示选取的多普勒通道数目;其中rM为大于或等于3并且小于M的整数,rN为大于或等于3并且小于N的整数,rK为大于或等于3并且小于K的整数,M为发射阵元数,N为接收阵元数,K为发射脉冲数,(·)H表示矩阵或向量的复共轭转置;Among them, R z is the covariance matrix of the space-time data vector z after dimensionality reduction, and the dimension is r M r N r K ; r M represents the number of selected transmit beams, r N represents the number of selected receive beams, r K represents the number of Doppler channels selected; where r M is an integer greater than or equal to 3 and less than M, r N is an integer greater than or equal to 3 and less than N, and r K is an integer greater than or equal to 3 and less than K, M is the number of transmitting array elements, N is the number of receiving array elements, K is the number of transmitting pulses, (·) H represents the complex conjugate transposition of matrix or vector;

4c)求解降维空时自适应处理的代价函数,得到降维处理器的权矢量w:4c) Solve the cost function of dimensionality reduction space-time adaptive processing, and obtain the weight vector w of dimensionality reduction processor:

ww == RR zz -- 11 cc (( ff sthe s ,, 00 ,, ff dd ,, 00 )) cc Hh (( ff sthe s ,, 00 ,, ff dd ,, 00 )) RR zz -- 11 cc (( ff sthe s ,, 00 ,, ff dd ,, 00 ))

其中,c(fs,0,fd,0)为降维后的目标空时二维导向矢量,(·)H表示矩阵或向量的复共轭转置,[·]-1表示对矩阵求逆,fd,0为目标的多普勒频率,fs,0为目标的归一化空间频率,Rz为降维后的空时数据矢量z的协方差矩阵。Among them, c(f s,0 ,f d,0 ) is the target space-time two-dimensional steering vector after dimensionality reduction, (·) H represents the complex conjugate transpose of matrix or vector, [·] -1 represents the pair matrix Inverse, f d,0 is the Doppler frequency of the target, f s,0 is the normalized spatial frequency of the target, R z is the covariance matrix of the space-time data vector z after dimensionality reduction.

与现有技术相比,本发明具有突出的实质性特点和显著的进步。本发明与现有方法相比,具有以下优点:Compared with the prior art, the present invention has outstanding substantive features and remarkable progress. Compared with existing methods, the present invention has the following advantages:

(1)相对于现有方法,本发明局域化方法的目标检测性能更优。如图4所示,图4比较了4种方法的改善因子曲线。当目标多普勒频率fd,0接近零时,FA方法的性能急剧下降,这是因为杂波已从多普勒滤波器的主瓣渗入,这时仅在检测多普勒通道内进行空域自适应处理,显然不能有效滤除杂波。与之不同的是,EFA方法和本发明局域化方法除了检测多普勒通道fd,0外,再取fd,-1和fd,1两组辅助通道参与自适应,所以相比FA方法,此两种方法在主杂波区的性能明显提高,而在其它区域也有一定的改善。此外,本发明局域化通过空域和时域同时降维处理,降低了对训练样本的要求,因此,在样本数仅为300的条件下本发明局域化目标检测性能优于EFA方法,而且与最优STAP相比,仅有约2.7dB的性能损益。(1) Compared with the existing methods, the target detection performance of the localization method of the present invention is better. As shown in Figure 4, Figure 4 compares the improvement factor curves of the four methods. The performance of the FA method drops sharply when the target Doppler frequency f d,0 is close to zero, because the clutter has penetrated from the main lobe of the Doppler filter, and the spatial domain Adaptive processing obviously cannot effectively filter out clutter. The difference is that, in addition to detecting the Doppler channel f d,0 in the EFA method and the localization method of the present invention, two groups of auxiliary channels f d,-1 and f d,1 are used to participate in self-adaptation, so compared FA method, the performance of these two methods is obviously improved in the main clutter area, and there are certain improvements in other areas. In addition, the localization of the present invention reduces the requirement for training samples through simultaneous dimensionality reduction in the space domain and the time domain. Therefore, the localized target detection performance of the present invention is better than that of the EFA method under the condition that the number of samples is only 300, and Compared with the optimal STAP, there is only about 2.7dB performance loss.

(2)本发明利用局域化方法比现有方法的目标功率高出残余杂波峰值功率的值大,使得本发明的杂波抑制性能更优。在235号和260号距离单元分别注入信噪比为0dB和-15dB的动目标信号,目标均位于载机正侧视方向,归一化多普勒频率为fd,0=0.125。如图5所示,图5为4种方法在200~300号距离单元的归一化输出功率。由图5(a)和5(b)明显看出,PC和FA方法的残余杂波功率较大,导致位于260号距离门的弱目标被湮没。图5(c)为EFA方法的输出结果,235和260号距离门目标功率分别高出残余杂波峰值功率21.68dB和6.72dB,235和260号距离门目标功率分别高出残余杂波平均功率31.28dB和16.60dB。图5(d)中,利用局域化方法,所得235和260号距离门目标功率分别高出残余杂波峰值功率23.26dB和6.98dB,所得235和260号距离门目标功率分别高出残余杂波平均功率33.55dB和17.27dB。可见,本发明方法比PC方法、FA方法及EFA方法的残余杂波功率要低,以上结果表明,本发明局域化方法的杂波抑制性能优于其他方法。(2) The target power of the present invention is larger than the value of the residual clutter peak power in the localization method compared with the existing method, so that the clutter suppression performance of the present invention is better. Moving target signals with signal-to-noise ratios of 0dB and -15dB are respectively injected into range cells No. 235 and No. 260. The targets are all located in the side-looking direction of the carrier aircraft, and the normalized Doppler frequency is f d,0 =0.125. As shown in Figure 5, Figure 5 shows the normalized output power of the four methods at distance units 200 to 300. It can be clearly seen from Fig. 5(a) and 5(b) that the residual clutter power of the PC and FA methods is relatively large, which leads to the obliteration of the weak target located at the No. 260 range gate. Figure 5(c) shows the output results of the EFA method. The target powers of No. 235 and No. 260 range gates are 21.68dB and 6.72dB higher than the peak power of residual clutter, respectively, and the target powers of No. 235 and No. 260 range gates are higher than the average power of residual clutter. 31.28dB and 16.60dB. In Fig. 5(d), using the localization method, the target powers of range gates 235 and 260 are 23.26dB and 6.98dB higher than the residual clutter peak power respectively, and the target powers of range gates 235 and 260 are higher than the residual clutter peak power respectively. Wave average power 33.55dB and 17.27dB. It can be seen that the residual clutter power of the method of the present invention is lower than that of the PC method, FA method and EFA method. The above results show that the clutter suppression performance of the localization method of the present invention is better than other methods.

(3)相对于现有方法,本发明局域化方法的收敛速度更快,降低了运算量和对样本的需求。图6为四种方法在目标多普勒通道的改善因子随样本数的变化曲线。通过比较可以看出,局域化方法具有较快的收敛速度,尤其是在小样本条件下,性能显著优于其它方法。由此可见,在难以获得大量独立同分布参考单元的真实杂波环境中,局域化方法具有较大的优势。本发明通过空域和时域同时降维处理,降低了对训练样本的要求。在运算量方面,本发明局域化的运算量为O[(rM×rN×rK)3],而EFA方法的运算量高达O[(rK×M×N)3],其中,M为发射阵元数,N为接收阵元数,rM表示选取的发射波束的数目,rN表示选取的接收波束的数目,rK表示选取的多普勒通道数目;当rM=3、rN=5、rK=3,M=5、N=10时,EFA方法的运算量大约是本发明的37倍,可见,本发明局域化方法的运算量比现有方法的运算量要低。(3) Compared with the existing method, the localization method of the present invention has a faster convergence speed, which reduces the amount of computation and the demand for samples. Fig. 6 is the change curve of the improvement factors of the four methods in the target Doppler channel with the number of samples. It can be seen from the comparison that the localization method has a faster convergence speed, especially under the condition of small samples, and its performance is significantly better than other methods. It can be seen that in the real clutter environment where it is difficult to obtain a large number of independent and identically distributed reference units, the localization method has great advantages. The present invention reduces the requirement on training samples through simultaneous dimensionality reduction processing in space domain and time domain. In terms of calculation amount, the calculation amount of the localization of the present invention is O[(r M ×r N ×r K ) 3 ], while the calculation amount of the EFA method is as high as O[(r K ×M×N) 3 ], where , M is the number of transmitting array elements, N is the number of receiving array elements, r M represents the number of selected transmitting beams, r N represents the number of selected receiving beams, r K represents the number of selected Doppler channels; when r M = 3. When r N =5, r K =3, M=5, N=10, the amount of calculation of the EFA method is about 37 times that of the present invention. It can be seen that the amount of calculation of the localization method of the present invention is higher than that of the existing method The amount of computation is low.

本发明具体是一种新的机载多输入多输出(Multiple-Input-Multiple-Output,MIMO)雷达三维波束空间的部分联合杂波抑制方法,大大降低了运算量和对参考单元数目的要求,有利于工程实现。The present invention is specifically a new airborne multiple-input multiple-output (Multiple-Input-Multiple-Output, MIMO) radar three-dimensional beam space partial joint clutter suppression method, which greatly reduces the amount of computation and the requirements for the number of reference units. Conducive to project realization.

附图说明Description of drawings

下面结合附图和具体实施方式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 specific embodiments.

图1为机载MIMO雷达系统模型示意图;Figure 1 is a schematic diagram of an airborne MIMO radar system model;

图2为本发明局域化方法数据处理流程图;Fig. 2 is the data processing flowchart of the localization method of the present invention;

图3为本发明局域化方法原理图;Fig. 3 is a schematic diagram of the localization method of the present invention;

图4为PC法、FA法、EFA法和本发明局域化方法的改善因子曲线图;Fig. 4 is the improvement factor graph of PC method, FA method, EFA method and localization method of the present invention;

图5为PC法、FA法、EFA法和本发明局域化方法在200~300号距离单元的归一化输出功率图,其中图5(a)为PC法的归一化输出功率图;图5(b)为FA法;图5(c)为EFA法的归一化输出功率图;图5(d)为本发明局域化方法的归一化输出功率图;Fig. 5 is the normalized output power figure of PC method, FA method, EFA method and the localization method of the present invention at No. 200~300 distance units, wherein Fig. 5 (a) is the normalized output power figure of PC method; Fig. 5 (b) is the FA method; Fig. 5 (c) is the normalized output power diagram of the EFA method; Fig. 5 (d) is the normalized output power diagram of the localization method of the present invention;

图6为PC法、FA法、EFA法和本发明局域化方法在目标多普勒通道的改善因子随样本数的变化曲线图。Fig. 6 is a graph showing the variation of the improvement factor of the PC method, the FA method, the EFA method and the localization method of the present invention in the target Doppler channel with the number of samples.

具体实施方式Detailed ways

参照图1和图2,说明本发明的一种机载MIMO雷达三维波束空间的部分联合杂波抑制方法,其具体步骤如下:With reference to Fig. 1 and Fig. 2, the partial joint clutter suppression method of a kind of airborne MIMO radar three-dimensional beam space of the present invention is illustrated, and its specific steps are as follows:

步骤1.利用机载MIMO雷达天线接收空时数据,并且构建目标的空时二维导向矢量b(fs,0,fd,0);Step 1. Use the airborne MIMO radar antenna to receive space-time data, and construct the space-time two-dimensional steering vector b(f s,0 ,f d,0 ) of the target;

1a)设定在一个相干处理间隔内,机载MIMO雷达天线的M个发射阵元同时辐射由K个脉冲组成的脉冲串波形,并且M个发射阵元发射的M个发射波形相互正交,在N个接收阵元的每一个接收阵元处,用M个参考发射信号对K个脉冲周期的回波数据进行匹配滤波,将所有匹配滤波器的输出排列成如下MNK×1维空时数据矢量,得到空时数据矢量x表达式为下式:1a) It is set that within a coherent processing interval, the M transmitting elements of the airborne MIMO radar antenna simultaneously radiate a burst waveform composed of K pulses, and the M transmitting waveforms emitted by the M transmitting elements are orthogonal to each other, At each of the N receiving array elements, M reference transmitting signals are used to perform matched filtering on the echo data of K pulse periods, and the outputs of all matched filters are arranged into the following MNK×1-dimensional space-time data Vector, the expression of the space-time data vector x is obtained as the following formula:

xx == ∫∫ 00 ππ ρρ (( θθ )) bb (( ff sthe s ,, ff dd )) dθdθ ++ xx ww

其中,空时数据x的维数为MNK×1维,是服从零均值复高斯分布的杂波散射系数;表示归一化杂波多普勒频率,Tr为脉冲重复周期,λ为雷达天线工作波长,v为载机速度,θ表示观测地面的方位角,为俯仰角;表示归一化杂波空间频率; b ( f s , f d ) = a d ( f d ) ⊗ a t ( f s ) ⊗ a r ( f s ) 为空时数据x中的杂波的空时二维导向矢量,其中,at(fs)=[1 exp(j2πfsα)…exp(j2πfsα(M-1))]T为M×1维发射阵列导向矢量,α=dT/dR,M为发射阵元数,N为接收阵元数,K为发射脉冲数,dT为发射阵元间距,dR为接收阵元间距;ar(fs)=[1 exp(j2πfs)…exp(j2πfs(N-1))]T为N×1维接收阵列导向矢量,ad(fd)=[1 exp(j2πfd)…exp(j2πfd(K-1))]T为K×1维多普勒导向矢量;表示Kronecker积;是服从0均值,方差为的MNK×1维高斯白噪声向量,IMNK代表MNK×MNK单位矩阵,分别表示输入杂波功率和噪声功率,(·)T表示向量转置;Among them, the dimension of space-time data x is MNK×1 dimension, is the clutter scattering coefficient that obeys the zero-mean complex Gaussian distribution; Indicates the normalized clutter Doppler frequency, T r is the pulse repetition period, λ is the working wavelength of the radar antenna, v is the speed of the carrier aircraft, θ is the azimuth angle of the observed ground, is the pitch angle; Indicates the normalized clutter spatial frequency; b ( f the s , f d ) = a d ( f d ) ⊗ a t ( f the s ) ⊗ a r ( f the s ) is the space-time two-dimensional steering vector of the clutter in the space-time data x, where a t (f s )=[1 exp(j2πf s α)…exp(j2πf s α(M-1))] T is M ×1-dimensional transmitting array steering vector, α=d T /d R , M is the number of transmitting array elements, N is the number of receiving array elements, K is the number of transmitting pulses, d T is the distance between transmitting array elements, and d R is the receiving array element spacing; a r (f s )=[1 exp(j2πf s )…exp(j2πf s (N-1))] T is the N×1-dimensional receiving array steering vector, a d (f d )=[1 exp( j2πf d )…exp(j2πf d (K-1))] T is the K×1 dimensional Doppler steering vector; Indicates the Kronecker product; is subject to 0 mean, variance is The MNK×1-dimensional Gaussian white noise vector, I MNK represents the MNK×MNK identity matrix, and Respectively represent the input clutter power and noise power, ( ) T represents the vector transpose;

1b)构建目标的空时二维导向矢量 b ( f s , 0 , f d , 0 ) = a d ( f d , 0 ) ⊗ a t ( f s , 0 ) ⊗ a r ( f s , 0 ) ; 1b) Construct the space-time two-dimensional guidance vector of the target b ( f the s , 0 , f d , 0 ) = a d ( f d , 0 ) ⊗ a t ( f the s , 0 ) ⊗ a r ( f the s , 0 ) ;

其中,ad(fd,0)为目标多普勒导向矢量,at(fs,0)为发射阵列导向矢量,ar(fs,0)为接收阵列导向矢量,fd,0为目标的多普勒频率,fs,0为目标的归一化空间频率,表示Kronecker积。Among them, a d (f d,0 ) is the target Doppler steering vector, at (f s,0 ) is the transmitting array steering vector, a r ( f s,0 ) is the receiving array steering vector, f d,0 is the Doppler frequency of the target, f s,0 is the normalized spatial frequency of the target, Represents the Kronecker product.

在现有技术中,机载MIMO雷达的空时二维最优处理器的权矢量wopt表示为:In the prior art, the weight vector wopt of the space-time two-dimensional optimal processor of the airborne MIMO radar is expressed as:

wopt=μR-1b(fs,0,fd,0)w opt =μR -1 b(f s,0 ,f d,0 )

其中,μ=1/[bH(fs,0,fd,0)R-1b(fs,0,fd,0)]为归一化复常数,R=E{xxH}为空时数据矢量x的协方差矩阵,维数为MNK,M为发射阵元数,N为接收阵元数,K为发射脉冲数;(·)H表示矩阵或向量的复共轭转置,[·]-1表示对矩阵求逆,E(·)表示数学期望。Among them, μ=1/[b H (f s,0 ,f d,0 )R -1 b(f s,0 ,f d,0 )] is a normalized complex constant, R=E{xx H } is the covariance matrix of the space-time data vector x, the dimension is MNK, M is the number of transmitting array elements, N is the number of receiving array elements, K is the number of transmitting pulses; ( ) H represents the complex conjugate transposition of the matrix or vector , [ ] -1 means to invert the matrix, and E( ) means mathematical expectation.

然而,在现有技术中求解空时二维最优处理器的权矢量wopt时,实际的MIMO雷达涉及的M,N,K通常为几十甚至上百,因此,直接对MNK维数据进行自适应处理存在两个缺陷:一是协方差矩阵R求逆的计算量O(M3N3K3)太大,处理器硬件难以实现;二是估计协方差矩阵所需的独立同分布参考单元数要求不低于2MNK,实际中尤其是非均匀杂波背景下很难满足。因此,STAP的应用必须采用降维处理方案,从而进行以下步骤2:However, when solving the weight vector w opt of the space-time two-dimensional optimal processor in the prior art, the M, N, and K involved in the actual MIMO radar are usually dozens or even hundreds, so the MNK dimensional data is directly There are two defects in adaptive processing: one is that the calculation amount O(M 3 N 3 K 3 ) for the inversion of the covariance matrix R is too large, and the processor hardware is difficult to realize; the other is that the independent and identical distribution reference The number of units is required to be no less than 2MNK, which is difficult to meet in practice, especially in the background of non-uniform clutter. Therefore, the application of STAP must adopt the dimension reduction processing scheme, so as to carry out the following steps 2:

步骤2.利用三维离散傅里叶变换将空时数据矢量x由阵元-脉冲域变换到三维波束域;空时数据矢量x在三维波束域中称为三维波束;Step 2. Utilize the three-dimensional discrete Fourier transform to transform the space-time data vector x from the array element-pulse domain to the three-dimensional beam domain; the space-time data vector x is called a three-dimensional beam in the three-dimensional beam domain;

如图3所示,将空时数据矢量x的发射阵元坐标变换到发射波束坐标、接收阵元坐标变换到接收波束坐标、时域脉冲坐标变换到多普勒通道坐标。As shown in Fig. 3, the transmit element coordinates of the space-time data vector x are transformed into transmit beam coordinates, the receive array element coordinates are transformed into receive beam coordinates, and the time-domain pulse coordinates are transformed into Doppler channel coordinates.

步骤3.构造降维矩阵P,利用降维矩阵P对三维波束域中的三维波束进行部分联合自适应处理,得到降维后的空时数据矢量z和降维后的目标空时二维导向矢量c(fs,0,fd,0);Step 3. Construct the dimensionality reduction matrix P, and use the dimensionality reduction matrix P to perform partial joint adaptive processing on the 3D beams in the 3D beam domain to obtain the space-time data vector z after dimensionality reduction and the target space-time two-dimensional guidance after dimensionality reduction vector c(f s,0 ,f d,0 );

3a)构造降维矩阵P,降维矩阵P表示为:3a) Construct a dimensionality reduction matrix P, and the dimensionality reduction matrix P is expressed as:

PP == GG dd ⊗⊗ GG tt ⊗⊗ GG rr

其中,Gd=[ad(fd,-1),ad(fd,0),ad(fd,1)]为三个邻近的多普勒导向矢量组成的多普勒滤波器组,Gt=[at(fs,-1),at(fs,0),at(fs,1)]为三个邻近的发射阵列导向矢量组成的发射波束形成器组,Gr=[ar(fs,-1),ar(fs,0),ar(fs,1)]为三个邻近的接收阵列导向矢量组成的接收波束形成器组,表示Kronecker积。Among them, G d =[a d (f d,-1 ), a d (f d,0 ), a d (f d,1 )] is the Doppler filter composed of three adjacent Doppler steering vectors G t =[a t (f s,-1 ), at (f s,0 ), at (f s,1 )] is the transmit beamformer composed of three adjacent transmit array steering vectors group, G r =[a r (f s,-1 ), a r (f s,0 ), a r (f s,1 )] is the receiving beamformer group composed of three adjacent receiving array steering vectors , Represents the Kronecker product.

3b)从三维波束域中选择3个或5个三维波束。3b) Select 3 or 5 3D beams from the 3D beam field.

3c)利用降维矩阵P对选择的三维波束根据下式进行部分联合自适应处理,得到空时数据矢量x降维后的空时数据矢量z;得到下式:3c) Using the dimensionality reduction matrix P to perform partial joint adaptive processing on the selected three-dimensional beams according to the following formula, to obtain the space-time data vector z after dimensionality reduction of the space-time data vector x; obtain the following formula:

z=PHxz = P H x

其中,P为降维矩阵,z为空时数据矢量x降维后的空时数据矢量,(·)H表示矩阵或向量的复共轭转置。Among them, P is the dimensionality reduction matrix, z is the space-time data vector after dimensionality reduction of space-time data vector x, (·) H represents the complex conjugate transpose of matrix or vector.

3d)根据降维矩阵P和目标空时二维导向矢量b(fs,0,fd,0)求取降维后的目标空时二维导向矢量c(fs,0,fd,0),得到下式:3d) Calculate the dimensionality-reduced target space-time two-dimensional steering vector c(f s ,0 ,f d , 0 ), get the following formula:

c(fs,0,fd,0)=PHb(fs,0,fd,0)c(f s,0 ,f d,0 )=P H b(f s,0 ,f d,0 )

其中,c(fs,0,fd,0)为目标空时二维导向矢量b(fs,0,fd,0)降维后的目标空时二维导向矢量;降维矩阵P维数为MNK×rMrNrK,rM表示选取的发射波束的数目,rN表示选取的接收波束的数目,rK表示选取的多普勒通道数目;其中rM为大于或等于3并且小于M的整数,rN为大于或等于3并且小于N的整数,rK为大于或等于3并且小于K的整数,fd,0为目标的多普勒频率,fs,0为目标的归一化空间频率,(·)H表示矩阵或向量的复共轭转置,M为发射阵元数,N为接收阵元数,K为发射脉冲数。Among them, c(f s,0 ,f d,0 ) is the target space-time two-dimensional steering vector after dimension reduction of the target space-time two-dimensional steering vector b(f s,0 ,f d,0 ); the dimensionality reduction matrix P The dimension is MNK×r M r N r K , where r M represents the number of selected transmit beams, r N represents the number of selected receive beams, and r K represents the number of selected Doppler channels; where r M is greater than or equal to r N is an integer greater than or equal to 3 and less than N, r K is an integer greater than or equal to 3 and less than K, f d,0 is the Doppler frequency of the target, f s,0 is The normalized spatial frequency of the target, (·) H represents the complex conjugate transpose of a matrix or vector, M is the number of transmitting array elements, N is the number of receiving array elements, and K is the number of transmitting pulses.

由于本发明局域化方法的处理器维数为rMrNrK,故要求独立同分布参考单元数不小于2rMrNrK,在本发明中独立同分布参考单元数就是样本数。Rz=E{zzH}=PHRP为降维后的空时数据矢量z的协方差矩阵,该矩阵Rz求逆的运算量为通常情况下rM、rN和rK取3或5;有rMrNrK<<MNK,实际雷达中,M,N,K通常为几十甚至上百,现有技术中,一是协方差矩阵R求逆的计算量O(M3N3K3)太大,处理器硬件难以实现;二是估计协方差矩阵所需的独立同分布参考单元数要求不低于2MNK,所需独立同分布参考单元数远大于本发明所需的独立同分布参考单元数目,因此采用本发明局域化方法可以大幅降低运算量和对参考单元数目的要求。事实上,选取的局域范围越大,对杂波的抑制效果越好,但同时涉及的计算量也会随之增加,所以应综合考虑性能和计算量两方面因素,选择合理的局域尺寸。在本发明的仿真中,采用了3×5×3的局域尺寸,在不考虑误差的情况下获得了接近最优的杂波抑制性能。然而实际中由于阵列误差的影响,杂波谱将展宽,此时应多取几个空域通道以增加空域自由度,而时域精度较高,可以少选几个多普勒单元。Since the processor dimension of the localization method of the present invention is r M r N r K , it is required that the number of independent and identically distributed reference units is not less than 2r M r N r K , and the number of independent and identically distributed reference units in the present invention is the number of samples . R z =E{zz H }=P H RP is the covariance matrix of the space-time data vector z after dimensionality reduction, and the calculation amount of inversion of this matrix R z is Usually r M , r N and r K take 3 or 5; r M r N r K << MNK, in actual radar, M, N, K are usually dozens or even hundreds, in the prior art, a The reason is that the amount of calculation O(M 3 N 3 K 3 ) for the inversion of the covariance matrix R is too large to be realized by the processor hardware; the second is that the number of independent and identically distributed reference units required for estimating the covariance matrix is not less than 2MNK, so The number of IID reference units required is far greater than the number of IID reference units required by the present invention, so the localization method of the present invention can greatly reduce the amount of computation and the requirement for the number of reference units. In fact, the larger the selected local area, the better the clutter suppression effect, but at the same time the amount of calculation involved will increase accordingly, so the performance and calculation amount should be considered comprehensively to choose a reasonable local area size . In the simulation of the present invention, a local area size of 3×5×3 is adopted, and near optimal clutter suppression performance is obtained without considering errors. However, in practice, due to the influence of array errors, the clutter spectrum will broaden. At this time, several more airspace channels should be selected to increase the degree of freedom in the airspace, and the time domain accuracy is higher, so a few Doppler units can be selected less.

步骤4.根据线性约束最小方差准则,即在保证目标信号增益一定的前提下最小化输出的杂波和噪声功率,利用降维后的空时数据矢量z和降维后的目标空时二维导向矢量c(fs,0,fd,0)构建降维空时自适应处理的代价函数;根据降维空时自适应处理的代价函数计算降维处理器的权矢量w;Step 4. According to the linear constraint minimum variance criterion, that is, to minimize the output clutter and noise power under the premise of ensuring a certain target signal gain, use the dimensionally reduced space-time data vector z and the dimensionally reduced target space-time two-dimensional Steering vector c(f s,0 ,f d,0 ) constructs the cost function of dimensionality reduction space-time adaptive processing; calculates the weight vector w of dimensionality reduction processor according to the cost function of dimensionality reduction space-time adaptive processing;

4a)利用降维后的空时数据矢量z求取降维后的空时数据矢量z的协方差矩阵Rz,Rz表达式为:4a) Use the space-time data vector z after dimension reduction to obtain the covariance matrix R z of the space-time data vector z after dimension reduction, and the expression of R z is :

Rz=E{zzH}=PHRPR z =E{zz H }=P H RP

其中,z表示降维后的空时数据矢量,P为降维矩阵,R为空时数据x的协方差矩阵,(·)H表示矩阵或向量的复共轭转置,E{·}表示进行期望操作。Among them, z represents the space-time data vector after dimensionality reduction, P is the dimensionality reduction matrix, R is the covariance matrix of space-time data x, ( ) H represents the complex conjugate transpose of matrix or vector, E{ } represents Perform the desired operation.

4b)根据线性约束最小方差准则,将降维空时自适应处理的代价函数表示为:4b) According to the linearly constrained minimum variance criterion, the cost function of dimensionality reduction space-time adaptive processing is expressed as:

minmin ww Hh RR zz ww sthe s .. tt .. ww Hh cc (( ff sthe s ,, 00 ,, ff dd ,, 00 )) == 11

其中,Rz为降维后的空时数据矢量z的协方差矩阵,维数为rMrNrK;rM表示选取的发射波束的数目,rN表示选取的接收波束的数目,rK表示选取的多普勒通道数目;其中rM为大于或等于3并且小于M的整数,rN为大于或等于3并且小于N的整数,rK为大于或等于3并且小于K的整数,M为发射阵元数,N为接收阵元数,K为发射脉冲数,(·)H表示矩阵或向量的复共轭转置;Among them, R z is the covariance matrix of the space-time data vector z after dimensionality reduction, and the dimension is r M r N r K ; r M represents the number of selected transmit beams, r N represents the number of selected receive beams, r K represents the number of Doppler channels selected; where r M is an integer greater than or equal to 3 and less than M, r N is an integer greater than or equal to 3 and less than N, and r K is an integer greater than or equal to 3 and less than K, M is the number of transmitting array elements, N is the number of receiving array elements, K is the number of transmitting pulses, (·) H represents the complex conjugate transposition of matrix or vector;

4c)求解降维空时自适应处理的代价函数,得到降维处理器的权矢量w:4c) Solve the cost function of dimensionality reduction space-time adaptive processing, and obtain the weight vector w of dimensionality reduction processor:

ww == RR zz -- 11 cc (( ff sthe s ,, 00 ,, ff dd ,, 00 )) cc Hh (( ff sthe s ,, 00 ,, ff dd ,, 00 )) RR zz -- 11 cc (( ff sthe s ,, 00 ,, ff dd ,, 00 ))

其中,c(fs,0,fd,0)为降维后的目标空时二维导向矢量,(·)H表示矩阵或向量的复共轭转置,[·]-1表示对矩阵求逆,fd,0为目标的多普勒频率,fs,0为目标的归一化空间频率,Rz为降维后的空时数据矢量z的协方差矩阵。Among them, c(f s,0 ,f d,0 ) is the target space-time two-dimensional steering vector after dimensionality reduction, (·) H represents the complex conjugate transpose of matrix or vector, [·] -1 represents the pair matrix Inverse, f d,0 is the Doppler frequency of the target, f s,0 is the normalized spatial frequency of the target, R z is the covariance matrix of the space-time data vector z after dimensionality reduction.

步骤5.利用降维处理器的权矢量w对机载MIMO雷达天线接收的空时数据矢量x进行加权求和,得到经过杂波抑制的空时数据。Step 5. Use the weight vector w of the dimensionality reduction processor to weight and sum the space-time data vector x received by the airborne MIMO radar antenna to obtain the space-time data after clutter suppression.

因为本发明中根据线性约束最小方差准则获取降维处理器的权矢量w,则经过杂波抑制的空时数据中杂波输出功率最小,而使目标信号的能量保持恒定,从而完成杂波的抑制。Because in the present invention, the weight vector w of the dimensionality reduction processor is obtained according to the linear constraint minimum variance criterion, the clutter output power in the space-time data after clutter suppression is the smallest, and the energy of the target signal is kept constant, thereby completing the clutter inhibition.

由于本发明的部分联合杂波抑制方法的处理器维数为rMrNrK,故要求独立同分布参考单元数不小于2rMrNrK;矩阵Rz求逆时只需对局域杂波的协方差矩阵进行估计和求逆,其运算量为通常情况下rM、rN和rK取3或5,有rMrNrK<<MNK,实际雷达中,M,N,K通常为几十甚至上百,现有技术中,一是协方差矩阵R求逆的计算量O(M3N3K3)远大于本发明中降维协方差矩阵的求逆运算量,处理器硬件难以实现;二是估计协方差矩阵所需的独立同分布参考单元数要求不低于2MNK,现有技术中所需独立同分布参考单元数远大于本发明所需的独立同分布参考单元数目,因此采用本发明局域化方法可以大幅降低运算量和对参考单元数目的要求,有利于工程实现。Since the processor dimension of the partial joint clutter suppression method of the present invention is r M r N r K , it is required that the number of independent and identically distributed reference units is not less than 2r M r N r K ; matrix R z only needs to match the The covariance matrix of domain clutter is estimated and inverted, and the calculation amount is Usually r M , r N and r K take 3 or 5, and r M r N r K <<MNK. In actual radar, M, N, and K are usually dozens or even hundreds. In the prior art, one It is that the amount of computation O(M 3 N 3 K 3 ) for the inversion of the covariance matrix R is far greater than the amount of computation for the inversion of the dimension-reduced covariance matrix in the present invention, which is difficult for the processor hardware to realize; The number of i.d. reference units is required to be no less than 2MNK. The number of i.d. reference units required in the prior art is far greater than the number of i.d. The quantity and the requirement for the number of reference units are beneficial to the realization of the project.

为了进一步说明本发明的机载MIMO雷达三维波束空间的部分联合杂波抑制方法,也可以称为局域化方法,相对于现有的方法(如PC法、FA法以及EFA法)的优越性,通过以下仿真体现。In order to further illustrate the partial joint clutter suppression method of airborne MIMO radar three-dimensional beam space of the present invention, also can be referred to as localization method, with respect to the superiority of existing method (such as PC method, FA method and EFA method) , through the following simulation.

下面结合仿真实验对本发明的效果做进一步说明。The effects of the present invention will be further described below in combination with simulation experiments.

(1)实验条件:(1) Experimental conditions:

本发明选取的局域尺寸为rM×rN×rK=3×5×3,FA方法时域滤波采用-60dB切比雪夫加权。实验参数设置为:载机速度v=150m/s,高度h=9km,雷达天线工作波长λ=0.3m,脉冲数K=16,脉冲周期Tr=5×10-4s,雷达距离分辨率为150m,发射阵元数M=5,接收阵元数为N=10,发射阵元间距dt=1.5m,接收阵元间距dr=0.15m,即接收阵阵元间距为半波长而发射阵稀布。计算机模拟中没有考虑地杂波起伏,并且认为各距离单元杂波相互独立,噪声功率杂噪比为40dB;杂波协方差矩阵由100~399号300个距离门的数据获得;假设雷达检测方向始终为正侧视方向,即归一化空间频率fs,0=0。The local area size selected in the present invention is r M ×r N ×r K =3×5×3, and the time domain filtering of the FA method adopts -60dB Chebyshev weighting. The experimental parameters are set as follows: aircraft speed v=150m/s, height h=9km, radar antenna operating wavelength λ=0.3m, pulse number K=16, pulse period T r =5×10 -4 s, radar range resolution is 150m, the number of transmitting array elements M=5, the number of receiving array elements is N=10, the spacing between transmitting array elements d t =1.5m, and the spacing between receiving array elements d r =0.15m, that is, the spacing between receiving array elements is half a wavelength and The emission array is sparse. The ground clutter fluctuation is not considered in the computer simulation, and it is considered that the clutter of each distance unit is independent of each other, and the noise power The clutter-to-noise ratio is 40dB; the clutter covariance matrix is obtained from the data of 300 range gates from 100 to 399; it is assumed that the radar detection direction is always the side-looking direction, that is, the normalized spatial frequency f s,0 =0.

在本发明中,将一个距离单元接收到的空时数据矢量x作为一个样本,雷达在不同距离单元接收的空时数据样本之间相互独立,独立样本数即为距离单元个数。In the present invention, the space-time data vector x received by one range unit is taken as a sample, and the space-time data samples received by the radar at different range units are independent of each other, and the number of independent samples is the number of range units.

(2)实验结果分析(2) Analysis of experimental results

实验一:如图4所示,横坐标是归一化多普勒频率,纵坐标是改善因子,图4比较了PC法、FA法、EFA法和本发明局域化方法4种方法随归一化多普勒频率变化的改善因子曲线。当目标多普勒频率fd,0接近零时,FA方法的性能急剧下降,这是因为杂波已从多普勒滤波器的主瓣渗入,这时仅在检测多普勒通道内进行空域自适应处理,显然不能有效滤除杂波。与之不同的是,EFA方法和本发明局域化方法除了检测多普勒通道fd,0外,再取fd,-1和fd,1两组辅助通道参与自适应,所以相比FA方法此两种方法在主杂波区的性能明显提高,而在其它区域也有一定的改善。此外,本发明局域化方法通过空域和时域同时降维处理,降低了对训练样本的要求,因此,在样本数仅为300的条件下性能优于EFA方法,而且与最优STAP相比,仅有约2.7dB的性能损益。在运算量方面,本发明局域化方法的运算量为O[(3×5×3)3],而EFA方法的运算量高达O[(3×5×10)3],大约是本发明局域化方法的37倍。PC方法虽然利用了杂波的低秩特性降低了对样本数的要求,但性能较差。Experiment 1: As shown in Figure 4, the abscissa is the normalized Doppler frequency, and the ordinate is the improvement factor. Figure 4 compares the regression of the PC method, the FA method, the EFA method and the localization method of the present invention. Improvement factor curve for normalized Doppler frequency change. The performance of the FA method drops sharply when the target Doppler frequency f d,0 is close to zero, because the clutter has penetrated from the main lobe of the Doppler filter, and the spatial domain is only performed in the detection Doppler channel. Adaptive processing obviously cannot effectively filter out clutter. The difference is that, in addition to detecting the Doppler channel f d,0 in the EFA method and the localization method of the present invention, two groups of auxiliary channels f d,-1 and f d,1 are used to participate in self-adaptation, so compared FA method The performance of these two methods is obviously improved in the main clutter area, and there are certain improvements in other areas. In addition, the localization method of the present invention reduces the requirements for training samples through simultaneous dimensionality reduction in the space and time domains. Therefore, the performance of the localization method is better than that of the EFA method when the number of samples is only 300, and compared with the optimal STAP , only about 2.7dB performance loss. In terms of calculation volume, the calculation volume of the localization method of the present invention is O[(3×5×3) 3 ], while the calculation volume of the EFA method is as high as O[(3×5×10) 3 ], which is about 37 times that of localized methods. Although the PC method takes advantage of the low-rank characteristics of clutter to reduce the requirement on the number of samples, its performance is poor.

实验二:在235号和260号距离单元分别注入信噪比为0dB和-15dB的动目标信号,目标均位于载机正侧视方向,归一化多普勒频率为fd,0=0.125。如图5所示,横坐标是距离单元,纵坐标是输出功率,在本发明仿真中具体指归一化输出功率,图5为PC法、FA法、EFA法和本发明4种方法在200~300号距离单元的归一化输出功率。需要说明的是,本发明中的FA法也就是1DT法,EFA法也就是3DT。由图5(a)和5(b)明显看出,PC和FA方法的残余杂波功率较大,导致位于260号距离门的弱目标被湮没。图5(c)为EFA方法的输出结果,235和260号距离门目标功率分别高出残余杂波峰值功率21.68dB和6.72dB,235和260号距离门目标功率分别高出残余杂波平均功率31.28dB和16.60dB。图5(d)中,利用本发明局域化方法,所得235和260号距离门目标功率分别高出残余杂波峰值功率23.26dB和6.98dB,所得235和260号距离门目标功率分别高出残余杂波平均功率33.55dB和17.27dB。可见,本发明局域化方法的目标功率高出残余杂波功率的值要大于其他方法的目标功率高于残余杂波功率的值,即体现了本发明方法的残余杂波功率比PC方法、FA方法及EFA方法的残余杂波功率都要低,以上结果表明,本发明局域化方法的杂波抑制性能优于其他方法。需要说明的是,在本发明所研究的部分联合杂波抑制方法为图4、图5和图6中示出的局域化方法。Experiment 2: Inject moving target signals with signal-to-noise ratios of 0dB and -15dB into range cells No. 235 and No. 260 respectively. The targets are located in the side-looking direction of the carrier aircraft, and the normalized Doppler frequency is f d,0 = 0.125 . As shown in Figure 5, the abscissa is the distance unit, and the ordinate is the output power, which specifically refers to the normalized output power in the simulation of the present invention. Normalized output power for ~300 range cells. It should be noted that the FA method in the present invention is also the 1DT method, and the EFA method is also the 3DT method. It can be clearly seen from Fig. 5(a) and 5(b) that the residual clutter power of the PC and FA methods is relatively large, which leads to the obliteration of the weak target located at the No. 260 range gate. Figure 5(c) shows the output results of the EFA method. The target powers of No. 235 and No. 260 range gates are 21.68dB and 6.72dB higher than the peak power of residual clutter, respectively, and the target powers of No. 235 and No. 260 range gates are higher than the average power of residual clutter. 31.28dB and 16.60dB. Among Fig. 5 (d), utilize the localization method of the present invention, gained No. 235 and No. 260 range gate target powers are respectively higher than residual clutter peak power 23.26dB and 6.98dB, gained No. 235 and No. 260 range gate target powers are respectively higher than The average power of residual clutter is 33.55dB and 17.27dB. It can be seen that the target power of the localization method of the present invention is higher than the value of the residual clutter power than the target power of other methods is higher than the value of the residual clutter power, that is, the residual clutter power of the method of the present invention is higher than that of the PC method, Both the FA method and the EFA method have low residual clutter power, and the above results show that the clutter suppression performance of the localization method of the present invention is better than other methods. It should be noted that the partial joint clutter suppression method studied in the present invention is the localization method shown in FIG. 4 , FIG. 5 and FIG. 6 .

实验三:如图6所示,横坐标是独立样本数,纵坐标是改善因子,图6为PC法、FA法、EFA法和本发明局域化方法四种方法在目标多普勒通道的改善因子随独立样本数的变化曲线。通过比较可以看出,本发明局域化方法具有较快的收敛速度,尤其是在小样本条件下,目标检测性能显著优于其它方法。在本发明中,将一个距离单元接收到的空时数据矢量x作为一个样本,雷达在不同距离单元接收的空时数据样本之间相互独立,独立样本数即为距离单元个数。由此可见,在难以获得大量独立同分布参考单元的真实杂波环境中,本发明局域化方法具有较大的优势。Experiment three: as shown in Figure 6, the abscissa is the number of independent samples, and the ordinate is the improvement factor. Figure 6 shows the results of the PC method, the FA method, the EFA method and the localization method of the present invention in the target Doppler channel. The change curve of the improvement factor with the number of independent samples. It can be seen from the comparison that the localization method of the present invention has a faster convergence speed, especially under the condition of small samples, and the target detection performance is significantly better than other methods. In the present invention, the space-time data vector x received by one range unit is taken as a sample, and the space-time data samples received by the radar at different range units are independent of each other, and the number of independent samples is the number of range units. It can be seen that in the real clutter environment where it is difficult to obtain a large number of IID reference units, the localization method of the present invention has great advantages.

Claims (4)

1. the part of an airborne MIMO radar three-dimensional beam space associating clutter suppression method, is characterized in that, comprises the following steps:
Data when step 1. utilizes airborne MIMO radar antenna to receive sky, the space-time two-dimensional steering vector b (f of data vector x expression formula and establishing target while obtaining sky s, 0, f d, 0);
When step 2. is utilized 3 d-dem Fourier transform by sky, data vector x transforms to three-dimensional Beam Domain by array element-pulse domain; When empty, data vector x is called three-dimensional wave beam in three-dimensional Beam Domain;
Step 3. structure dimensionality reduction matrix P, utilizes dimensionality reduction matrix P to carry out part associating self-adaptive processing to the three-dimensional wave beam in three-dimensional Beam Domain, two-dimensional guide vector C (f during target empty while obtaining empty after dimensionality reduction after data vector z and dimensionality reduction s, 0, f d, 0);
Step 4. is according to linearly constrained minimum variance, in the clutter and the noise power that guarantee to minimize under the prerequisite that targeted signal gain is certain output, and two-dimensional guide vector C (f during target empty while utilizing empty after dimensionality reduction after data vector z and dimensionality reduction s, 0, f d, 0) build the cost function that dimensionality reduction space-time adaptive is processed; The weight vector w of the cost function calculation dimension-reduction treatment device of processing according to dimensionality reduction space-time adaptive;
The weight vector w that step 5. is utilized dimension-reduction treatment device receives airborne MIMO radar antenna when empty, and data vector x is weighted summation, obtain suppressing through clutter empty time data.
2. the part of a kind of airborne MIMO radar three-dimensional beam space according to claim 1 associating clutter suppression method, is characterized in that, step 1 comprises following sub-step:
1a) be set in relevant a processing in interval, the train of impulses waveform that the radiation simultaneously of the M of airborne MIMO radar antenna transmitting array element is comprised of K pulse, and M transmitted waveform of M transmitting array element transmitting is mutually orthogonal, at N each reception array element place that receives array element, by M reference transmitted signal, the echo data of K recurrence interval is carried out to matched filtering, the data vector when output of all matched filters is arranged in to following MNK * 1 dimension sky, while obtaining sky, data vector x expression formula is following formula:
x = &Integral; 0 &pi; &rho; ( &theta; ) b ( f s , f d ) d&theta; + x w
Wherein, when empty, the dimension of data vector x is MNK * 1 dimension, it is the clutter scattering coefficient of obeying the multiple Gaussian distribution of zero-mean; represent normalization clutter Doppler frequency, T rfor the pulse repetition time, λ is radar antenna operation wavelength, and v is carrier aircraft speed, and θ represents to observe the position angle on ground, for the angle of pitch; represent normalization clutter spatial frequency; b ( f s , f d ) = a d ( f d ) &CircleTimes; a t ( f s ) &CircleTimes; a r ( f s ) The space-time two-dimensional steering vector of the clutter during for sky in data x, wherein a t(f s)=[1 exp (j2 π f sα) ... exp (j2 π f sα (M-1))] tfor M * 1 dimension emission array steering vector, α=d t/ d r, M is transmitting array number, and N is for receiving array number, and K is transponder pulse number, d tfor transmitting array element distance, d rfor receiving array element distance; a r(f s)=[1 exp (j2 π f s) ... exp (j2 π f s(N-1))] tfor N * 1 dimension receiving array steering vector, a d(f d)=[1 exp (j2 π f d) ... exp (j2 π f d(K-1))] tfor K * 1 dimension Doppler steering vector; represent that Kronecker is long-pending; be to obey 0 average, variance is mNK * 1 dimension white Gaussian noise vector, I mNKrepresent MNK * MNK unit matrix, with represent respectively input clutter power and noise power, () trepresent vectorial transposition;
1b) the space-time two-dimensional steering vector of establishing target b ( f s , 0 , f d , 0 ) = a d ( f d , 0 ) &CircleTimes; a t ( f s , 0 ) &CircleTimes; a r ( f s , 0 ) ;
Wherein, a d(f d, 0) be target Doppler steering vector, a t(f s, 0) be emission array steering vector, a r(f s, 0) be receiving array steering vector, f d, 0for the Doppler frequency of target, f s, 0for the normalization spatial frequency of target, represent that Kronecker is long-pending.
3. the part of a kind of airborne MIMO radar three-dimensional beam space according to claim 1 associating clutter suppression method, is characterized in that, step 3 comprises following sub-step:
3a) structure dimensionality reduction matrix P, dimensionality reduction matrix P is expressed as
P = G d &CircleTimes; G t &CircleTimes; G r
Wherein, G d=[a d(f d ,-1), a d(f d, 0), a d(f d, 1)] be the Doppler filter group of Doppler's steering vector composition of three vicinities, G t=[a t(f s ,-1), a t(f s, 0), a t(f s, 1)] be the launching beam shaper group of the emission array steering vector composition of three vicinities, G r=[a r(f s ,-1), a r(f s, 0), a r(f s, 1)] be the receive beamformer group of the receiving array steering vector composition of three vicinities, represent that Kronecker is long-pending;
3b) from three-dimensional Beam Domain, select 3 or 5 three-dimensional wave beams;
3c) utilize dimensionality reduction matrix P according to following formula, to carry out part associating self-adaptive processing to the three-dimensional wave beam of selecting, data vector z during empty while obtaining sky after data vector x dimensionality reduction; Obtain following formula:
z=P Hx
Wherein, P is dimensionality reduction matrix, data vector during empty when z is empty after data vector x dimensionality reduction, () hthe complex-conjugate transpose of representing matrix or vector;
Two-dimensional guide vector b (f during 3d) according to dimensionality reduction matrix P and target empty s, 0, f d, 0) two-dimensional guide vector C (f while asking for the target empty after dimensionality reduction s, 0, f d, 0), obtain following formula:
c(f s,0,f d,0)=P Hb(f s,0,f d,0)
Wherein, c (f s, 0, f d, 0) two-dimensional guide vector b (f while being target empty s, 0, f d, 0) two-dimensional guide vector during target empty after dimensionality reduction; Dimensionality reduction matrix P dimension is MNK * r mr nr k, r mthe number of the launching beam that expression is chosen, r nthe number of the received beam that expression is chosen, r krepresent Doppler's number of active lanes of choosing; R wherein mfor being more than or equal to 3 and be less than the integer of M, r nfor being more than or equal to 3 and be less than the integer of N, r kfor being more than or equal to 3 and be less than the integer of K, f d, 0for the Doppler frequency of target, f s, 0for the normalization spatial frequency of target, () hthe complex-conjugate transpose of representing matrix or vector, M is transmitting array number, and N is for receiving array number, and K is transponder pulse number.
4. the part of a kind of airborne MIMO radar three-dimensional beam space according to claim 1 associating clutter suppression method, is characterized in that, step 4 comprises following sub-step:
The covariance matrix R of data vector z when data vector z asks for empty after dimensionality reduction while 4a) utilizing empty after dimensionality reduction z, R zexpression formula is:
R z=E{zz H}=P HRP
Wherein, data vector when z represents empty after dimensionality reduction, P is dimensionality reduction matrix, the covariance matrix of data x when R is empty, () hthe complex-conjugate transpose of representing matrix or vector, E{} represents to carry out desired operation;
4b) according to linearly constrained minimum variance, the cost function that dimensionality reduction space-time adaptive is processed is expressed as:
min w H R z w s . t . w H c ( f s , 0 , f d , 0 ) = 1
Wherein, R zthe covariance matrix of data vector z during for empty after dimensionality reduction, dimension is r mr nr k; r mthe number of the launching beam that expression is chosen, r nthe number of the received beam that expression is chosen, r krepresent Doppler's number of active lanes of choosing; R wherein mfor being more than or equal to 3 and be less than the integer of M, r nfor being more than or equal to 3 and be less than the integer of N, r kfor being more than or equal to 3 and be less than the integer of K, M is transmitting array number, and N is for receiving array number, and K is transponder pulse number, () hthe complex-conjugate transpose of representing matrix or vector;
4c) solve the cost function that dimensionality reduction space-time adaptive is processed, obtain the weight vector w of dimension-reduction treatment device:
w = R z - 1 c ( f s , 0 , f d , 0 ) c H ( f s , 0 , f d , 0 ) R z - 1 c ( f s , 0 , f d , 0 )
Wherein, c (f s, 0, f d, 0) two-dimensional guide vector while being the target empty after dimensionality reduction, () hthe complex-conjugate transpose of representing matrix or vector, [] -1expression is to matrix inversion, f d, 0for the Doppler frequency of target, f s, 0for the normalization spatial frequency of target, R zthe covariance matrix of data vector z during for empty after dimensionality reduction.
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