CN107193002B - A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise - Google Patents
A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise Download PDFInfo
- Publication number
- CN107193002B CN107193002B CN201710364405.7A CN201710364405A CN107193002B CN 107193002 B CN107193002 B CN 107193002B CN 201710364405 A CN201710364405 A CN 201710364405A CN 107193002 B CN107193002 B CN 107193002B
- Authority
- CN
- China
- Prior art keywords
- auto
- vector
- formula
- range profile
- dimensional range
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
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
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/88—Radar or analogous systems specially adapted for specific applications
- G01S13/89—Radar or analogous systems specially adapted for specific applications for mapping or imaging
-
- 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
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/02—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
- G01S7/41—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section
Landscapes
- Engineering & Computer Science (AREA)
- Remote Sensing (AREA)
- Radar, Positioning & Navigation (AREA)
- Physics & Mathematics (AREA)
- Computer Networks & Wireless Communication (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Radar Systems Or Details Thereof (AREA)
Abstract
The invention belongs to Radar Technology fields, are related to a kind of one-dimensional range profile high-resolution imaging method that can inhibit wideband phase noise.Method of the invention is main are as follows: firstly, carrying out oversampled discrete processing in the bandwidth of wideband radar transmitting signal to radar echo signal, constructing the one-dimensional range profile imaging model based on phase recovery;Secondly, non-convex problem is imaged in the one-dimensional range profile based on phase recovery and is converted to the convex problem restored based on auto-correlation using Fourier's base characteristic of observing matrix;Augmented Lagrangian Functions are constructed, the function is calculated relative to the derivative of auto-correlation vector and to enable it is zero, obtain the iterative equation about auto-correlation vector;Iterative processing is executed, stops when residual error is less than reservation threshold or the number of iterations is greater than maximum number of iterations, obtains optimal auto-correlation vector;Finally, solving corresponding scattering coefficient vector to the method for the auto-correlation vector Ke Ermoge love spectral factorization found out under minimum phase criterion.
Description
Technical field
The invention belongs to Radar Technology field, be related to a kind of one-dimensional range profile high-resolution that can inhibit wideband phase noise at
Image space method.
Background technique
Radar High Range Resolution (High Resolution Range Profiles, HRRP) is that target reflectivity characteristics exist
One Dimensional Projection on radar line of sight contains the features such as number, distribution and the radical length of target scattering point, and it is vertical to reflect target
To fine structure, have great importance to target detection, tracking and identification, have in practice in engineering and important apply valence
Value.
According to electromagnetic theory, when the electric size of target scattering body is much larger than wavelength, the high-frequency electromagnetic scattering properties of target
It can be indicated by the synthesis of local scattering properties, locally scattering is commonly known as equivalent scattering center for these.It is theoretical herein
On the basis of, with the continuous development of Radar Technology, lot of documents proposes to obtain by pulse compression technique using big bandwidth signal
The target scattering center high-resolution upward in distance by radar is obtained, to realize the one-dimensional range profile high-resolution of target scattering center
Imaging.The present invention emits broadband signal using wideband radar, emits delay and amplitude modulating action of the signal Jing Guo observed object
Afterwards, the reflection echo of target is obtained, and then carries out one-dimensional range profile high-resolution imaging.However, due to radio wave propagation, systematic error
It can be by the serious shadow of random phase noise in broadband signal with factors, the target echo that wideband radar receives such as atmospheric interference
It rings, and then one-dimensional range profile generation is caused seriously to defocus, it is difficult to obtain high-resolution performance.
Summary of the invention
It is to be solved by this invention, aiming at the above problem, propose it is a kind of can inhibit wideband phase noise it is one-dimensional away from
From image height resolution imaging method, target scene is observed using the broadband signal that wideband radar emits, utilizes observing matrix
Fourier's base characteristic and phase retrieval problem architectural characteristic, to returning while establishing one-dimensional range profile imaging problem hidden convexity
Phase noise of the wave number in is effectively inhibited, and then realizes one-dimensional range profile high-resolution imaging.
The technical scheme is that
A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise, which is characterized in that including following
Step:
The one-dimensional range profile imaging model that S1, building are interfered containing phase noise:
In the bandwidth of wideband radar transmitting signal, oversampled discrete processing is carried out to radar echo signal, building contains
The one-dimensional range profile imaging model of phase noise interference, shown in following formula 1:
lr=Ψ Ds+n (formula 1)
In formula 1, lrIndicate echo vector, Ψ indicates phase noise matrix, and D indicates observing matrix, s be scattering coefficient to
Amount, n is noise vector;
S2, it the one-dimensional range profile based on phase recovery is imaged to non-convex problem is converted to and convex being asked based on what auto-correlation was restored
Topic:
Phase recovery is mainly that the amplitude information for utilizing linearly to measure restores echo signal, and the present invention utilizes observation square
Fourier's base characteristic of battle array D constructs the one-dimensional range profile based on phase recovery and is imaged shown in the non-following formula 2 of convex problem:
H=| Ψ Ds |2+ e (formula 2)
In formula 2, h indicates that measurement vector, e indicate noise vector;
In order to restore vector s from vector h, the present invention considers that least square cost constructs phase retrieval problem, because this
A problem is non-convex, therefore can obtain unique solution without algorithm, in order to solve this problem, most using minimum phase criterion
The one-dimensional range profile based on phase recovery is imaged with auto-correlation formula under minimum phase criterion for smallization minimum mean-square error
Non- convex problem is expressed as shown in following formula 3:
In formula 3, r is the auto-correlation vector of scattering coefficient vector, and E=diag { [1,2 ..., 2] } is diagonal matrix;
S3, optimal auto-correlation vector r is obtained:
Augmented Lagrangian Functions are constructed, the function is calculated relative to the derivative of auto-correlation vector and to enable it is zero, obtain
Iterative equation about auto-correlation vector;
Reservation threshold ε and maximum number of iterations T is set, auto-correlation vector r is solved from formula 3 using alternately multiplier method,
In an iterative process, stop when the residual error of auto-correlation vector is less than reservation threshold ε or the number of iterations is greater than maximum number of iterations T
Only, optimal auto-correlation vector r is obtained;
S4, scattering coefficient vector is obtained:
Corresponding scattering coefficient vector is solved by auto-correlation vector r using Ke Ermoge love spectral factorization method.
The total technical solution of the present invention, firstly, being carried out in the bandwidth of wideband radar transmitting signal to radar echo signal
Oversampled discreteization processing, constructs the one-dimensional range profile imaging model based on phase recovery;Secondly, using in Fu of observing matrix
One-dimensional range profile based on phase recovery is imaged non-convex problem and is converted to the convex problem restored based on auto-correlation by phyllopodium characteristic;
Augmented Lagrangian Functions are constructed, the function is calculated relative to the derivative of auto-correlation vector and to enable it is zero, are obtained about from phase
Close the iterative equation of vector;Iterative processing is executed, until residual error is less than reservation threshold or the number of iterations greater than maximum number of iterations
When stop, obtaining optimal auto-correlation vector;Finally, under minimum phase criterion, to the auto-correlation vector Ke Ermo found out
The method of dagger-axe love spectral factorization solves corresponding scattering coefficient vector.
Further, step S1 method particularly includes:
Assuming that then one-dimensional distance is expressed as 4 institute of formula to scattering center model there are N number of ideal scattering point in scene
Show:
In formula 4, lrIndicate echo-signal, k representation space frequency, σpIndicate the scattering coefficient of p-th of scattering point, △ R
(xp) indicate p-th of scattering point to scene center distance,Indicate the phase noise in p-th of scattering point echo;
The echo of single scattering center is carried out to the oversampled discreteization processing of frequency, frequency over-sampling points are M, then return
Wave vector lr=[lr1,lr2,…,lrN], scattering coefficient vector is expressed as s=[σ1,σ2,…,σN]T, phase noise matrix isObserving matrix is expressed as D=[d1,d2,…,dN], wherein di=
[d(f1),d(f2),…,d(fM)]T, and 0≤i≤N, d (fj)=exp {-j2 π k △ R (xj)},0≤j≤N。
Further, with auto-correlation formula that the one-dimensional range profile imaging based on phase recovery is non-convex in the step S2
The formula 2 of problem is expressed as formula 3 method particularly includes:
The auto-correlation vector of scattering coefficient is expressed asVector form isIt enablesR=[r is enabled after eliminating redundancy0,r1,…,rN-1], then haveWherein { [1,2 ..., 2] } E=diag.
Bound term in formula 3 is that r is limited autocorrelation sequence, and the necessary and sufficient condition that r is limited autocorrelation sequence is r
Discrete time Fourier transform be more than or equal to 0, i.e.,Exist respectively to R (w)
Point is sampled, this operation is equivalent to matrix vector multiplication FLS, wherein FLBe L point it is discrete when
Between the preceding N of Fourier transformation arrange shown in following formula (5)
In formula 5, φ=e-j2π/L。
The beneficial effects of the present invention are: the present invention combines alternating multiplier method and Ke Ermoge love spectral factorization method to broadband
One-dimensional range profile imaging is carried out while phase noise is inhibited, and is divided first containing the target echo that phase noise interferes
One-dimensional range profile based on phase recovery is imaged non-convex problem using Fourier's base characteristic of observing matrix and is converted to by analysis modeling
Based on the convex problem that auto-correlation is restored, solved to obtain optimal auto-correlation vector using alternately multiplier method.Then, in minimum
Under phase criterion, corresponding scattering coefficient vector is solved by auto-correlation vector using Ke Ermoge love spectral factorization method.This hair
The bright concrete form for not considering phase noise, but the structural advantage of secondary amplitude observation model is utilized, to phase noise square
Battle array is inhibited using the method that transposition is multiplied, and since calculation matrix is over-sampling, and the present invention is not needed to target field
Scape carry out sparse prior it is assumed that therefore have preferable noiseproof feature, to reflection target longitudinal direction fine structure, target detection,
Tracking and identification have great importance.
Detailed description of the invention
Fig. 1 is radar imagery geometrized structure graph;
Fig. 2 is the spectrogram using auto-correlation vector of the invention;
Fig. 3 is the high-resolution lattice image differently obtained in simulating, verifying, and (a) is tradition SDA method, (b)
For method of the invention.
Specific embodiment
With reference to the accompanying drawings and examples, the technical schemes of the invention are described in detail:
The radar geometry that the present invention uses is as shown in Figure 1, wherein wideband radar constantly emits and connects to target scene
Pulse is received, specific implementation step of the invention is as follows:
Step 1, the one-dimensional range profile imaging model interfered containing phase noise is constructed:
1.1) wideband radar works in microwave band, and target length is much larger than wavelength, at this moment target can be approximately one group from
Scattered ideal scattering point, transmitting signal form scattering idea echo, target echo is after by the delay of each scattering point and amplitude modulation
Be each scattering idea echo and, it can thus be concluded that one-dimensional distance is to scattering center model:
Wherein lr(k) echo-signal is indicated, N is the number of ideal scattering center in target scene, σpIndicate scene midpoint p
Scattering coefficient, k is spatial frequency,For phase noise;
1.2) number that ideal scattering center is arranged in the present invention is N=200, and spatial frequency sampling number is M, and is made
M=20N is obtained, vector form is denoted as, constructs one-dimensional range profile imaging mould when having N number of scattering center in target scene
Type:
lr=Ψ Ds+n
Wherein, lrFor echo vector, Ψ is phase noise matrix, and s is scene scatters coefficient vector, and D is observing matrix, n
Indicate noise vector;
Step 2, phase recovery mainly restores original signal from the amplitude information that linearly converts, according to observation square
Fourier's base characteristic of battle array D constructs the one-dimensional range profile based on phase recovery and rebuilds non-convex problem.The present invention is proposed with minimum phase
One-dimensional range profile based on phase recovery is rebuild non-convex problem weight with auto-correlation formula by the criterion of minimizing minimum mean-square error in position
Structure is the convex problem restored based on auto-correlation, and solves auto-correlation vector using alternately multiplier method:
2.1) phase recovery mainly restores original signal from the amplitude information that linearly converts, and utilizes observing matrix
Fourier's base characteristic, one-dimensional range profile based on phase recovery is imaged non-convex problem and can state are as follows:
H=| Ψ Ds |2+e
Wherein, h indicate measurement vector, e indicate noise vector, give as follows measurement vector most preceding 4 and
4 last values:
956344.768958355
969469.536257930
984190.736648139
993031.439383133
……
981176.583440932
960831.851019310
952150.404583882
956344.768958355
2.2) non-convex problem reformulation is imaged in the one-dimensional range profile based on phase recovery is convex asking of being restored based on auto-correlation
Inscribe model.The discrete fourier sampling number L=20N of r is set first, and is existed respectively to itPoint
Discrete sampling is carried out, then can obtain sampling matrix FL:
2.4) iteration factor λ=0, ρ=0 are set, and reservation threshold is ε=1e-5, maximum number of iterations T=100, is introduced auxiliary
Help variableWhen the residual values of auto-correlation vector in iterative process are big less than reservation threshold ε=1e-5 or the number of iterations
Stop when maximum number of iterations T=100, obtain optimal auto-correlation vector, specific iterative equation is as follows:
Wherein, Z is the auxiliary variable introduced, diagonal matrix E=diag { [1,2 ..., 2] }, rk+1Be in kth time iteration more
New auto-correlation vector, Zk+1It is the auxiliary variable updated in kth time iteration, λk+1It is the coefficient updated in kth time iteration.For
Obtained optimal auto-correlation vector is solved, Fig. 2 illustrates the spectrogram of auto-correlation vector, gives auto-correlation vector r as follows most
4 preceding and 4 last values:
1000511.96176304+0.00000000000000i
477.932961976909+2.18140192724284e-10i
477.932961977524-1.22061440209938e-10i
500.277937547207-25.8125130313545i
……
477.932961972361-6.50920079632485e-09i
477.932961978081+8.29003513697613e-09i
477.932961967987-1.17880427427074e-08i
477.932961982636-1.59174930667994e-09i
Step 3: the auto-correlation vector obtained according to step 2 iteration solves the minimum phase for generating this auto-correlation vector
Scattering coefficient vector:
3.1) discrete time Fourier transform is carried out to auto-correlation vector r, obtains the power spectrum R (w) of scattering coefficient vector,
And there is R (w)=sH(w)s(w);
3.2) by that 3.1) can obtain ln [R (w)]=2lns (w), and ln [R (w)]=α (w)+j β (w), wherein α (w) is indicated
Amplitude response, β (w) indicate phase response;
3.3) assume that knowing that the amplitude response of auto-correlation vector Fourier transformation and phase response meet wishes by minimum phase
The relationship of your Bert transformation, it can obtain β (w) by carrying out Hilbert transform to α (w);
3.4) it can be obtained by the auto-correlation vector acquired in step 2:
Wherein,Expression takes corresponding real part,Expression takes corresponding imaginary part, and sgn (w) indicates sign function;
3.5) minimum for generating auto-correlation vector in step 2 can be acquired by the relationship between auto-correlation vector sum scattering coefficient
Phase scattering coefficient vector:
Effect of the invention can be illustrated by following emulation experiments:
The present invention handles the echo data of simulating scenes, right while inhibition to phase noise in echo
Target scene carries out one-dimensional range profile High resolution reconstruction.Centre carrier frequency in the present invention are as follows: f0=9GHz, signal bandwidth are as follows: B
=1.0GHz, scene size are as follows: N=200 pixel, over-sampling points are as follows: M=20N, auto-correlation sampling number are as follows: L=20N, with
Machine phase noise obedience is uniformly distributed: [- π/4, π/4], additive gaussian white noise are as follows: SNR=20dB.It is carried out using distinct methods
The result of one-dimensional range profile imaging is as shown in figure 3, figure culminant star labelled notation curve indicates original one-dimensional range profile, circles mark curve
It indicates to rebuild one-dimensional range profile.Fig. 3 (a), which shows, utilizes sparse driving self-focusing method (Sparsity-driven
Autofocus, SDA) carry out one-dimensional range profile imaging as a result, Fig. 3 (b) show using algorithm proposed by the present invention progress
The result of one-dimensional range profile imaging.It can be obtained from Fig. 3, when noise jamming containing random phase in radar return, SDA algorithm cannot
One-dimensional range profile high-resolution imaging is carried out, and algorithm proposed by the present invention can carry out good imaging to one-dimensional range profile, obtain
High-resolution one-dimensional range profile.Table 1 lists the reconstruction performance of the different next algorithms of signal-to-noise ratio, and present invention primarily contemplates following
Reconstruction performance: 1) mean square error (RMSE) is rebuild:Wherein D indicates that observing matrix, s indicate original and dissipate
Coefficient vector is penetrated,Indicate the scattering coefficient vector rebuild;2) target background ratio (TBR):Wherein ΩtIndicate the supported collection of target,Indicate the supplementary set of object support collection,Indicate background element number.As can be seen that compared with SDA algorithm, propose algorithm can obtain better target background ratio and
Residual error, table 1 show the reconstruction performance parameter comparison of each algorithm under different signal-to-noise ratio.
The reconstruction performance of each algorithm under the different signal-to-noise ratio of table 1
Claims (3)
1. a kind of one-dimensional range profile high-resolution imaging method that can inhibit wideband phase noise, which is characterized in that including following step
It is rapid:
The one-dimensional range profile imaging model that S1, building are interfered containing phase noise:
In the bandwidth of wideband radar transmitting signal, oversampled discrete processing is carried out to radar echo signal, building is based on phase
The one-dimensional range profile imaging model of bit recovery, shown in following formula 1:
lr=Ψ Ds+n (formula 1)
In formula 1, lrIndicate that echo vector, Ψ indicate that phase noise matrix, D indicate observing matrix, s is scattering coefficient vector, n
It is noise vector;
S2, the one-dimensional range profile based on phase recovery is imaged non-convex problem be converted to based on auto-correlation restore convex problem:
Using Fourier's base characteristic of observing matrix D, it is as follows to construct the non-convex problem of one-dimensional range profile imaging based on phase recovery
Shown in formula 2:
H=| Ψ Ds |2+ e (formula 2)
In formula 2, h indicates that measurement vector, e indicate noise vector;
Using the criterion of minimizing minimum mean-square error of minimum phase, under minimum phase criterion, phase will be based on auto-correlation formula
The one-dimensional range profile of bit recovery is imaged non-convex problem and is expressed as shown in following formula 3:
In formula 3, r is the auto-correlation vector of scattering coefficient vector, and E=diag { [1,2 ..., 2] } is diagonal matrix;Table
Show and takes corresponding real part;
S3, optimal auto-correlation vector r is obtained:
Construct Augmented Lagrangian Functions, calculate the function relative to the derivative of auto-correlation vector and to enable it be zero, obtain about
The iterative equation of auto-correlation vector;
Reservation threshold ε and maximum number of iterations T is set, auto-correlation vector r is solved from formula 3 using alternately multiplier method, repeatedly
During generation, stop when the residual error of auto-correlation vector is less than reservation threshold ε or the number of iterations is greater than maximum number of iterations T,
Obtain optimal auto-correlation vector r;
S4, scattering coefficient vector is obtained:
Corresponding scattering coefficient vector is solved by auto-correlation vector r using Ke Ermoge love spectral factorization method.
2. a kind of one-dimensional range profile high-resolution imaging method that can inhibit wideband phase noise according to claim 1,
It is characterized in that, step S1's method particularly includes:
Assuming that then one-dimensional distance is expressed as shown in formula 4 to scattering center model there are N number of ideal scattering point in scene:
In formula 4, lrIndicate echo vector, k representation space frequency, σpIndicate the scattering coefficient of p-th of scattering point, Δ R (xp) table
Show p-th of scattering point to scene center distance,Indicate the phase noise in p-th of scattering point echo;
The echo of single scattering center is carried out to the oversampled discreteization processing of frequency, frequency over-sampling points are M, then echo to
Measure lr=[lr1,lr2,…,lrN], scattering coefficient vector is expressed as s=[σ1,σ2,…,σN]T, phase noise matrix isObserving matrix is expressed as D=[d1,d2,…,dN], wherein di=
[d(f1),d(f2),…,d(fM)]T, and 0≤i≤N, d (fj)=exp {-j2 π k Δ R (xj)},0≤j≤N。
3. a kind of one-dimensional range profile high-resolution imaging method that can inhibit wideband phase noise according to claim 2,
It is characterized in that, the one-dimensional range profile based on phase recovery is imaged in the step S2 with auto-correlation formula the formula of non-convex problem
2 are expressed as formula 3 method particularly includes:
The auto-correlation vector of scattering coefficient is expressed asVector form isIt enablesR=[r is enabled after eliminating redundancy0,r1,…,rN-1], then haveWherein { [1,2 ..., 2] } E=diag.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710364405.7A CN107193002B (en) | 2017-05-22 | 2017-05-22 | A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710364405.7A CN107193002B (en) | 2017-05-22 | 2017-05-22 | A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise |
Publications (2)
Publication Number | Publication Date |
---|---|
CN107193002A CN107193002A (en) | 2017-09-22 |
CN107193002B true CN107193002B (en) | 2019-04-26 |
Family
ID=59874660
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201710364405.7A Active CN107193002B (en) | 2017-05-22 | 2017-05-22 | A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN107193002B (en) |
Families Citing this family (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108572363A (en) * | 2018-04-27 | 2018-09-25 | 中国人民解放军国防科技大学 | Electromagnetic vortex high-resolution imaging method based on sparse Bayesian learning |
CN110223238B (en) * | 2019-04-30 | 2021-04-27 | 北京理工大学 | Encoding illumination imaging reconstruction method and device |
CN111257287B (en) * | 2020-01-22 | 2022-11-25 | 清华大学深圳国际研究生院 | Large-field-of-view scattering imaging method and device based on no-priori target positioning |
CN116679301B (en) * | 2023-07-28 | 2023-10-20 | 西安电子科技大学 | Method for rapidly reconstructing target range profile of broadband radar in super-resolution mode |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102805613A (en) * | 2012-08-13 | 2012-12-05 | 电子科技大学 | Two-time scanning-based high-resolution optical scanning holographic section imaging method |
CN102882530A (en) * | 2012-09-17 | 2013-01-16 | 南京邮电大学 | Compressed sensing signal reconstruction method |
CN103605116A (en) * | 2013-12-04 | 2014-02-26 | 西安电子科技大学 | Online imaging radar channel parameter compensation method based on sparse analysis |
CN105182335A (en) * | 2015-08-31 | 2015-12-23 | 西安电子科技大学 | Geosynchronous orbit SAR imaging method based on singular value decomposition |
-
2017
- 2017-05-22 CN CN201710364405.7A patent/CN107193002B/en active Active
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102805613A (en) * | 2012-08-13 | 2012-12-05 | 电子科技大学 | Two-time scanning-based high-resolution optical scanning holographic section imaging method |
CN102882530A (en) * | 2012-09-17 | 2013-01-16 | 南京邮电大学 | Compressed sensing signal reconstruction method |
CN103605116A (en) * | 2013-12-04 | 2014-02-26 | 西安电子科技大学 | Online imaging radar channel parameter compensation method based on sparse analysis |
CN105182335A (en) * | 2015-08-31 | 2015-12-23 | 西安电子科技大学 | Geosynchronous orbit SAR imaging method based on singular value decomposition |
Non-Patent Citations (2)
Title |
---|
Noise Robust Radar HRRP Target Recognition Based on Scatterer Matching Algorithm;Lan Du等;《IEEE Sensors Journal》;20151119;第16卷(第6期);全文 * |
一维距离像特性分析及目标识别方法研究;杨莉;《道客巴巴》;20151115;全文 * |
Also Published As
Publication number | Publication date |
---|---|
CN107193002A (en) | 2017-09-22 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN107193002B (en) | A kind of one-dimensional range profile high-resolution imaging method can inhibit wideband phase noise | |
CN103713288B (en) | Sparse Bayesian reconstruct linear array SAR formation method is minimized based on iteration | |
Fromenteze et al. | Single-shot compressive multiple-inputs multiple-outputs radar imaging using a two-port passive device | |
CN106021637B (en) | DOA estimation method based on the sparse reconstruct of iteration in relatively prime array | |
CN105137424B (en) | Real beam scanning radar angle ultra-resolution method under a kind of clutter background | |
CN108717189B (en) | Bistatic MIMO radar imaging method based on compressed sensing theory | |
CN105137425B (en) | The preceding visual angle ultra-resolution method of scanning radar based on Deconvolution principle | |
CN104950305A (en) | Real beam scanning radar angle super-resolution imaging method based on sparse constraint | |
CN103698763A (en) | Hard threshold OMP (orthogonal matching pursuit)-based linear array SAR (synthetic aperture radar) sparse imaging method | |
CN107607945B (en) | Scanning radar foresight imaging method based on spatial embedding mapping | |
CN108562884A (en) | A kind of Air-borne Forward-looking sea-surface target angle ultra-resolution method based on maximum a posteriori probability | |
CN103293528B (en) | Super-resolution imaging method of scanning radar | |
CN104794264A (en) | Radar communication waveform design method based on sparse frequency | |
CN107390216A (en) | High speed super-resolution stationary point scan imaging method based on wave-number domain coherence factor | |
CN112147608A (en) | Rapid Gaussian gridding non-uniform FFT through-wall imaging radar BP method | |
CN108562901B (en) | ISAR high-resolution imaging method based on maximum signal-to-noise-and-noise ratio criterion | |
CN108919263B (en) | ISAR high-resolution imaging method based on maximum mutual information criterion | |
Molaei et al. | Fourier-based near-field three-dimensional image reconstruction in a multistatic imaging structure using dynamic metasurface antennas | |
Xiong et al. | Sub‐band mutual‐coherence compensation in multiband fusion ISAR imaging | |
CN107479053B (en) | STAP-based robust transmitting and receiving joint design method for ship-borne MIMO radar | |
Molaei et al. | MIMO Coded Generalized Reduced Dimension Fourier Algorithm for 3-D Microwave Imaging | |
CN113608218A (en) | Frequency domain interference phase sparse reconstruction method based on back projection principle | |
CN115825953B (en) | Forward-looking super-resolution imaging method based on random frequency coding signal | |
CN105891826A (en) | Airborne radar fast maximum posteriori imaging method | |
Zhuge et al. | Human body imaging by microwave UWB radar |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
GR01 | Patent grant | ||
GR01 | Patent grant | ||
TR01 | Transfer of patent right |
Effective date of registration: 20220130 Address after: No.3, 14th floor, building 2, No.368, Tianfu 2nd Street, high tech Zone, Chengdu, Sichuan 610000 Patentee after: SICHUAN HONGCHUANG ELECTRONIC TECHNOLOGY Co.,Ltd. Address before: 611731, No. 2006, West Avenue, hi tech West District, Sichuan, Chengdu Patentee before: University of Electronic Science and Technology of China |
|
TR01 | Transfer of patent right |