CN114460531A - Uniform linear array MUSIC spatial spectrum estimation method - Google Patents
Uniform linear array MUSIC spatial spectrum estimation method Download PDFInfo
- Publication number
- CN114460531A CN114460531A CN202011245176.5A CN202011245176A CN114460531A CN 114460531 A CN114460531 A CN 114460531A CN 202011245176 A CN202011245176 A CN 202011245176A CN 114460531 A CN114460531 A CN 114460531A
- Authority
- CN
- China
- Prior art keywords
- array
- matrix
- subspace
- signal
- 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
Links
- 238000000034 method Methods 0.000 title claims abstract description 34
- 238000001228 spectrum Methods 0.000 title claims abstract description 25
- 239000011159 matrix material Substances 0.000 claims abstract description 64
- 239000013598 vector Substances 0.000 claims abstract description 39
- 238000012937 correction Methods 0.000 claims abstract description 16
- 238000000354 decomposition reaction Methods 0.000 claims abstract description 14
- 238000007781 pre-processing Methods 0.000 claims abstract description 11
- 238000005457 optimization Methods 0.000 claims abstract description 6
- 230000003595 spectral effect Effects 0.000 claims description 5
- 238000012935 Averaging Methods 0.000 claims description 3
- 238000003491 array Methods 0.000 claims description 3
- 238000004364 calculation method Methods 0.000 claims description 3
- 238000004891 communication Methods 0.000 abstract description 3
- 238000005259 measurement Methods 0.000 abstract description 3
- 238000004422 calculation algorithm Methods 0.000 description 10
- 238000005516 engineering process Methods 0.000 description 5
- 238000012545 processing Methods 0.000 description 4
- 238000006880 cross-coupling reaction Methods 0.000 description 2
- 238000004088 simulation Methods 0.000 description 2
- 238000004458 analytical method Methods 0.000 description 1
- 230000001427 coherent effect Effects 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 230000007812 deficiency Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 238000011161 development Methods 0.000 description 1
- 238000003672 processing method Methods 0.000 description 1
- 238000011160 research Methods 0.000 description 1
- 238000005070 sampling Methods 0.000 description 1
- 238000012163 sequencing technique Methods 0.000 description 1
- 238000006467 substitution reaction Methods 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/02—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
- G01S3/14—Systems for determining direction or deviation from predetermined direction
- G01S3/143—Systems for determining direction or deviation from predetermined direction by vectorial combination of signals derived from differently oriented antennae
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S3/00—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
- G01S3/02—Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received using radio waves
- G01S3/04—Details
- G01S3/10—Means for reducing or compensating for quadrantal, site, or like errors
Landscapes
- Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Radar Systems Or Details Thereof (AREA)
Abstract
The invention provides a uniform linear array MUSIC spatial spectrum estimation method, which is applied to target angle measurement of radar communication and navigation, and comprises the following steps: acquiring a covariance matrix of array received signals; performing Topriz preprocessing on the covariance matrix; performing characteristic decomposition on the matrix subjected to Topriz pretreatment; estimating the number of information sources by using the characteristic value after the characteristic decomposition; constructing an error correction matrix by using the steering vectors of the array received signals; and constructing a spectrum estimation formula by using the approximate orthogonality of the guide vector in the signal subspace and the noise subspace and the error correction matrix, and performing optimization search. When various non-ideal factors exist simultaneously, the method can still stably and accurately estimate the direction of arrival of the echo signal.
Description
Technical Field
The invention belongs to the field of signal processing, and particularly relates to a uniform array MUSIC spatial spectrum estimation method.
Background
Direction of Arrival (DOA) estimation is an important research Direction for array signal processing, and is gradually developed on the basis of a beam forming technology, a null technology and a time domain spectrum estimation technology. The spatial sampling of the spatial information source is completed through antenna units at different spatial positions, and then the high-precision and high-resolution azimuth estimation of the spatial information source is realized through the analysis and processing of snapshot data. Since the orientation information in the airspace corresponds to the spectral information in the time domain, the DOA estimate is also commonly referred to as a Spatial Spectrum (Spatial Spectrum) estimate.
In conventional array direction finding, the angular resolution of the target depends on the physical aperture size of the array, i.e. is subject to Rayleigh limit (Rayleigh Limitation). In practical applications, the physical aperture of the array is always limited by practical conditions and cannot be infinitely increased, which makes it difficult to obtain a high precision target direction using conventional processing methods. The high-resolution DOA estimation technology breaks through the Rayleigh limit constraint, and can greatly improve the angle estimation precision, the angle resolution and other related parameter estimation precision of spatial signals in system processing bandwidth, so that the method has a very wide application prospect in the fields of radar, communication, sonar and the like. In particular, it has recently become a key technology in the hotspot field, such as array radar passive detection, smart antenna Spatial Division Multiple Access (SDMA) vehicle-mounted millimeter wave radar, and the like.
The multiple signal classification (MUSIC) algorithm was proposed by r.o.schmidt doctor, et al, in 1979, and the proposed algorithm initiated a new era of spatial spectrum estimation algorithm, promoted the rise and development of feature structure class algorithm, and became an algorithm with spatial spectrum estimation notability. The MUSIC algorithm can obtain high angle measurement precision under ideal conditions. However, in practical application, various non-ideal factors often exist: array errors, unknown clutter, different noise, channel inconsistency, array cross-coupling, signal source coherence, and the like. In recent years, many researchers have proposed some solutions around the non-ideal factors in practice, but often the single non-ideal factor is not good or even fails when multiple non-ideal factors exist.
Disclosure of Invention
In view of the above, the present invention provides a method for estimating a uniform array MUSIC spatial spectrum, which is used to solve the deficiencies of the prior art.
In order to achieve the purpose, the invention adopts the following technical scheme:
the embodiment of the invention provides a method for estimating a uniform array MUSIC spatial spectrum, which comprises the following steps:
acquiring a covariance matrix of array received signals;
performing Topriz preprocessing on the covariance matrix;
performing characteristic decomposition on the matrix subjected to Topriz pretreatment;
estimating the number of information sources by using the characteristic value after the characteristic decomposition;
constructing an error correction matrix by using the steering vectors of the array received signals;
and constructing a spectrum estimation formula by using the approximate orthogonality of the guide vector in the signal subspace and the noise subspace and the error correction matrix, and performing optimization search.
Further, the specific process of obtaining the covariance matrix of the array received signals is as follows:
the N narrow-band far-field signals received by the M arrays are:
X(t)=A(θ)s(t)+N(t) (1)
wherein X (t) is M × 1 dimension snapshot data vector of array, N (t) is M × 1 dimension noise data vector of array, S (t) is N × 1 dimension vector of space signal, A is M × N dimension flow pattern matrix (guide vector matrix) of space array
A=[a1(ω),a2(ω),…,aN(ω)] (2)
Wherein the guide vector
Wherein,c is the speed of light, lambda is the wavelength, tau is the wave path difference, for a uniform linear array, the wave path difference of adjacent array elements is
Wherein d is the array element spacing, and theta is the signal incidence angle.
At this time, the covariance matrix of the array data can be obtained as
R=E[XXH]=AE[SSH]AH+σ2I=ARSAH+σ2I (5)
Wherein R isSBeing a covariance matrix of the signal, ARSAHAs signal part, σ2Variance of noise, σ2I is the noise portion.
Further, the specific process of performing Topriz preprocessing on the covariance matrix is as follows:
the NxN array covariance matrix R is
Matrix R after Topritz preprocessingTIs composed of
The following relationships apply: rTElement on diagonal: rt is an integer of1,1=rt2,2=rti,i=rtN,N;RTElement above diagonal: rt is an integer of1,2=rt2,3=rti,i+1=rtN-1,N;RTElements below the diagonal: rt is an integer of2,1=rt3,2=rti+1,i=rtN,N-1And so on; all RTThe elements with the same size on the matrix diagonal are obtained by averaging the corresponding elements of the array covariance matrix R, that is:and so on.
Further, the specific process of performing characteristic decomposition on the matrix after the Topriz preprocessing comprises the following steps:
matrix R after pretreatment of TopritzTIs subjected to characteristic decomposition of
Wherein, USIs a subspace spanned by the eigenvectors corresponding to the large eigenvalues, i.e. the signal subspace, and UNIs a subspace spanned by the feature vectors corresponding to the small feature values, namely a noise subspace;
ideally, the signal subspace and the noise subspace in the data space are orthogonal to each other, i.e. the steering vector in the signal subspace is also orthogonal to the noise subspace
aH(θ)UN=0 (9)。
Further, the specific process of constructing the error correction matrix by using the steering vector of the array received signal comprises the following steps:
assuming that the signal steering vector in the ideal case is a (θ), the error correction matrix T consists of two parts:
T=T1+T2 (10)
wherein, T1 and T2 are respectively calculated by the following formulas:
further, a spectrum estimation formula is constructed by using the approximate orthogonality of the steering vector in the signal subspace and the noise subspace and the error correction matrix, and the specific process of optimizing and searching is as follows:
the spectral calculation formula constructed is as follows:
where det () denotes a determinant.
And setting a proper threshold, searching in a preset angle range, and determining that the angle has the target when the angle passes the threshold.
The invention provides a robust MUSIC spatial spectrum estimation method suitable for a uniform linear array, which can still obtain stable and accurate target angle estimation under the condition of simultaneously having various non-ideal factors. The method is particularly suitable for engineering implementation.
Drawings
In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings used in the description of the embodiments or the prior art will be briefly described below, it is obvious that the drawings in the following description are only some embodiments of the present invention, and for those skilled in the art, other drawings can be obtained according to the drawings without creative efforts.
Fig. 1 is a flowchart of a method for estimating a spatial spectrum of a uniform array MUSIC according to an embodiment of the present invention;
FIG. 2 is the spectral estimation result of the classical MUSIC algorithm;
fig. 3 is a spectrum estimation result of the uniform array MUSIC spatial spectrum estimation method provided by the present application.
Detailed Description
The technical solutions in the embodiments of the present invention will be clearly and completely described below with reference to the drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
Fig. 1 is a schematic flowchart illustrating a method for estimating a uniform array MUSIC spatial spectrum according to an embodiment of the present invention. The method is applied to target angle measurement of radar communication and navigation. The method comprises the following steps:
s101, acquiring a covariance matrix of array received signals.
The main method steps for forming the covariance matrix by the array received signals are as follows:
assume that the N narrow-band far-field signals received by the M arrays are:
X(t)=A(θ)s(t)+N(t) (1)
wherein X (t) is M × 1 dimension snapshot data vector of array, N (t) is M × 1 dimension noise data vector of array, S (t) is N × 1 dimension vector of space signal, A is M × N dimension flow pattern matrix (guide vector matrix) of space array
A=[a1(ω),a2(ω),…,aN(ω)] (2)
Wherein the guide vector
Wherein,c is the speed of light, lambda is the wavelength, tau is the wave path difference, for a uniform linear array, the wave path difference of adjacent array elements is
Wherein d is the array element spacing, and theta is the signal incidence angle.
At this time, the covariance matrix of the array data can be obtained as
R=E[XXH]=AE[SSH]AH+σ2I=ARSAH+σ2I (5)
Wherein R isSBeing a covariance matrix of the signal, ARSAHAs signal part, σ2Variance of noise, σ2I is the noise portion.
S102, Topriz preprocessing is carried out on the covariance matrix.
The main method steps for preprocessing the covariance matrix of the array data by Toeplitz pre (Toeplitz) are as follows:
assume that the array covariance matrix R of NxN obtained in S101 is
Matrix R after Toeplitz pretreatmentTIs composed of
The following relationships apply: rTElement on diagonal: rt is an integer of1,1=rt2,2=rti,i=rtN,N;RTElement above diagonal: rt is an integer of1,2=rt2,3=rti,i+1=rtN-1,N;RTElements below the diagonal: rt is an integer of2,1=rt3,2=rti+1,i=rtN,N-1And so on. All RTThe elements with the same size on the matrix diagonal are obtained by averaging the corresponding elements of the array covariance matrix R, that is:and so on.
S103, performing characteristic decomposition on the matrix subjected to Topritz preprocessing.
Matrix R after pretreatment of ToeplitzTThe main method steps for performing characteristic decomposition are as follows:
matrix R after pretreatment of TopritzTIs subjected to characteristic decomposition of
Wherein, USIs a subspace spanned by the eigenvectors corresponding to the large eigenvalues, i.e. the signal subspace, and UNIs a subspace spanned by the feature vectors corresponding to the small feature values, i.e. the noise subspace.
Ideally, the signal subspace and the noise subspace in the data space are orthogonal to each other, i.e. the steering vector in the signal subspace is also orthogonal to the noise subspace
aH(θ)UN=0 (9)
And S104, estimating the number of the information sources by using the characteristic values after the characteristic decomposition.
And sequencing the characteristic values from large to small, and setting a threshold so as to determine the number of the information sources.
And S105, constructing an error correction matrix by using the guide vectors of the array received signals.
An error correction matrix T is constructed using the steering vectors. The method comprises the following steps:
assuming that the signal steering vector in the ideal case is a (θ), T consists of two parts:
T=T1+T2 (10)
wherein, T1 and T2 are respectively calculated by the following formulas:
and S106, constructing a spectrum estimation formula by using the approximate orthogonality of the guide vector and the noise subspace in the signal subspace and the error correction matrix, and performing optimization search.
And (4) constructing a spectrum estimation formula by using the approximate orthogonality of the guide vector in the signal subspace and the noise subspace and the error correction matrix T obtained in the step S105, and performing optimization search. The method mainly comprises the following steps:
the spectral calculation formula constructed is as follows:
where det () denotes a determinant.
An appropriate threshold is set, a search is performed over the range of angles of interest (e.g., -90 °,90 °), and the angle is considered to have a target when the threshold is exceeded.
The following simulations compare the estimated performance of the classical MUSIC algorithm and the proposed method in the presence of various errors.
Simulation conditions are as follows: the ground clutter noise ratio is 15dB, the array element number is 8, the two coherent targets are respectively positioned at-5 degrees and 5 degrees, and the amplitude phase error: -1dB, -10 °,10 °) randomly distributed; array element cross coupling degree of freedom: 2, mutual coupling coefficient: c1 ═ 0.1+0.1 × i.
Fig. 2 and fig. 3 show the spectrum estimation results of the classical MUSIC algorithm and the method of the present invention, respectively, and it can be seen from the graphs that the classical MUSIC algorithm has failed when there are many non-ideal factors, but the method of the present invention can still obtain stable and accurate angle estimation.
The above description is only for the specific embodiments of the present invention, but the scope of the present invention is not limited thereto, and any person skilled in the art can easily think of the changes or substitutions within the technical scope of the present invention, and shall cover the scope of the present invention. Therefore, the protection scope of the present invention shall be subject to the protection scope of the appended claims.
Claims (6)
1. A method for estimating a uniform array MUSIC spatial spectrum is characterized by comprising the following steps:
acquiring a covariance matrix of array received signals;
performing Topriz preprocessing on the covariance matrix;
performing characteristic decomposition on the matrix subjected to Topriz pretreatment;
estimating the number of information sources by using the characteristic value after the characteristic decomposition;
constructing an error correction matrix by using the steering vectors of the array received signals;
and constructing a spectrum estimation formula by using the approximate orthogonality of the guide vector in the signal subspace and the noise subspace and the error correction matrix, and performing optimization search.
2. The method of claim 1, wherein the obtaining the covariance matrix of the array received signals comprises:
the N narrow-band far-field signals received by the M arrays are:
X(t)=A(θ)s(t)+N(t) (1)
wherein X (t) is M × 1 dimension snapshot data vector of array, N (t) is M × 1 dimension noise data vector of array, S (t) is N × 1 dimension vector of space signal, A is M × N dimension flow pattern matrix (guide vector matrix) of space array
A=[a1(ω),a2(ω),…,aN(ω)] (2)
Wherein the guide vector
Wherein,c is the speed of light, lambda is the wavelength, tau is the wave path difference, for a uniform linear array, the wave path difference of adjacent array elements is
Wherein d is the array element spacing, and theta is the signal incidence angle.
At this time, the covariance matrix of the array data can be obtained as
R=E[XXH]=AE[SSH]AH+σ2I=ARSAH+σ2I (5)
Wherein R isSBeing a covariance matrix of the signal, ARSAHAs signal part, σ2Variance of noise, σ2I is the noise portion.
3. The method according to claim 1, wherein the Topritz preprocessing of the covariance matrix comprises:
the NxN array covariance matrix R is
Matrix R after Topritz preprocessingTIs composed of
The following relationships apply: rTElement on diagonal: rt is an integer of1,1=rt2,2=rti,i=rtN,N;RTElements above the diagonal: rt is an integer of1,2=rt2,3=rti,i+1=rtN-1,N;RTElements below the diagonal: rt is an integer of2,1=rt3,2=rti+1,i=rtN,N-1And so on; all RTThe elements with the same size on the matrix diagonal are obtained by averaging the corresponding elements of the array covariance matrix R, that is:and so on.
4. The method according to claim 1, wherein the characteristic decomposition of the Topritz-preprocessed matrix comprises the following specific steps:
matrix R after pretreatment of TopritzTIs subjected to characteristic decomposition of
Wherein, USIs a feature vector sheet corresponding to a large feature valueA subspace of, i.e., a signal subspace, and UNIs a subspace spanned by the feature vectors corresponding to the small feature values, namely a noise subspace;
ideally, the signal subspace and the noise subspace in the data space are orthogonal to each other, i.e. the steering vector in the signal subspace is also orthogonal to the noise subspace
aH(θ)UN=0 (9)。
5. The method of claim 1, wherein constructing the error correction matrix using the steering vectors of the array received signals comprises:
assuming that the signal steering vector in the ideal case is a (θ), the error correction matrix T consists of two parts:
T=T1+T2 (10)
wherein, T1 and T2 are respectively calculated by the following formulas:
6. the method of claim 1, wherein the spectral estimation formula is constructed by using the approximate orthogonality of the steering vector in the signal subspace and the noise subspace and the error correction matrix, and the optimization search is performed by:
the constructed spectrum calculation formula is as follows:
where det () denotes a determinant.
And setting a proper threshold, searching in a preset angle range, and determining that the angle has the target when the angle passes the threshold.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202011245176.5A CN114460531A (en) | 2020-11-10 | 2020-11-10 | Uniform linear array MUSIC spatial spectrum estimation method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN202011245176.5A CN114460531A (en) | 2020-11-10 | 2020-11-10 | Uniform linear array MUSIC spatial spectrum estimation method |
Publications (1)
Publication Number | Publication Date |
---|---|
CN114460531A true CN114460531A (en) | 2022-05-10 |
Family
ID=81404436
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN202011245176.5A Pending CN114460531A (en) | 2020-11-10 | 2020-11-10 | Uniform linear array MUSIC spatial spectrum estimation method |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN114460531A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117331027A (en) * | 2023-09-27 | 2024-01-02 | 青岛哈尔滨工程大学创新发展中心 | Sound source number estimation method and system based on subspace matching measurement |
CN117970227A (en) * | 2024-02-04 | 2024-05-03 | 哈尔滨工程大学 | Amplitude-phase error and angle parameter joint estimation method and system based on coherent distribution source under strong impulse noise |
-
2020
- 2020-11-10 CN CN202011245176.5A patent/CN114460531A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN117331027A (en) * | 2023-09-27 | 2024-01-02 | 青岛哈尔滨工程大学创新发展中心 | Sound source number estimation method and system based on subspace matching measurement |
CN117331027B (en) * | 2023-09-27 | 2024-06-04 | 青岛哈尔滨工程大学创新发展中心 | Sound source number estimation method and system based on subspace matching measurement |
CN117970227A (en) * | 2024-02-04 | 2024-05-03 | 哈尔滨工程大学 | Amplitude-phase error and angle parameter joint estimation method and system based on coherent distribution source under strong impulse noise |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
WO2021139208A1 (en) | One-dimensional doa estimation method based on combined signals at specific frequencies | |
CN109061554B (en) | Target arrival angle estimation method based on dynamic update of spatial discrete grid | |
CN109490820B (en) | Two-dimensional DOA estimation method based on parallel nested array | |
CN112130111B (en) | Single-snapshot two-dimensional DOA estimation method in large-scale uniform cross array | |
CN106501765B (en) | A kind of Maximum Likelihood DOA Estimation based on quadratic sum and Semidefinite Programming | |
CN107037398B (en) | Parallel computing method for estimating direction of arrival by two-dimensional MUSIC algorithm | |
CN113835063B (en) | Unmanned aerial vehicle array amplitude and phase error and signal DOA joint estimation method | |
CN112666513B (en) | Improved MUSIC (multiple input multiple output) direction-of-arrival estimation method | |
CN101252382B (en) | Wide frequency range signal polarizing and DOA estimating method and apparatus | |
CN114460531A (en) | Uniform linear array MUSIC spatial spectrum estimation method | |
CN111983554A (en) | High-precision two-dimensional DOA estimation under non-uniform L array | |
CN109696651B (en) | M estimation-based direction-of-arrival estimation method under low snapshot number | |
CN113759303B (en) | Gridless angle of arrival estimation method based on particle swarm optimization | |
CN105572629B (en) | A kind of two-dimentional direction-finding method of low computational complexity suitable for General Cell structure | |
CN112763972B (en) | Sparse representation-based double parallel line array two-dimensional DOA estimation method and computing equipment | |
CN112363108B (en) | Signal subspace weighting super-resolution direction-of-arrival detection method and system | |
CN111368256B (en) | Single snapshot direction finding method based on uniform circular array | |
CN108594165B (en) | Narrow-band signal direction-of-arrival estimation method based on expectation maximization algorithm | |
CN112946615B (en) | Phased array system amplitude and phase error correction method | |
CN114609580A (en) | Non-hole co-prime array design method based on non-circular signals | |
CN114265005A (en) | Polarization phase interferometer direction finding method and device | |
CN111366891B (en) | Pseudo covariance matrix-based uniform circular array single snapshot direction finding method | |
CN113791379A (en) | Orthogonal matching pursuit DOA estimation method under nested array non-Gaussian environment | |
CN112579972A (en) | Spatial domain information joint estimation method under directional electromagnetic coupling effect | |
CN112363106A (en) | Signal subspace direction of arrival detection method and system based on quantum particle swarm |
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 |