Approximate two-dimensional model of radar imaging and its super-resolution algorithm

Publisher:epsilon15Latest update time:2011-04-18 Reading articles on mobile phones Scan QR code
Read articles on your mobile phone anytime, anywhere

The existing radar imaging super-resolution algorithm is based on the two-dimensional sinusoidal signal model of the target echo signal, so the model error, especially the range movement error, will seriously degrade the algorithm performance or make it invalid. To this end, this paper adopts the first-order approximate radar imaging two-dimensional signal model under the range movement error and proposes a parameterized super-resolution algorithm based on the nonlinear least squares criterion. In the algorithm, the range movement error compensation and target parameter estimation are carried out jointly. The article also gives the Cramer-Rao bound and simulation results of the algorithm estimation performance.
Keywords: range movement error; compensation; super-resolution; radar imaging

A Super Resolution Radar Imaging Algorithm Based on the 2-D Approximate Model

SUN Chang-yin,BAO Zheng
(Kay Laboratory for Radar Signal Processing,Xidian University,Xi’an 710071,China)

Abstract:The recently proposed super resolution radar imaging algorithms,which are based on the 2-D sinusoid signal model,often suffer from the motion through resolution cell error(MTRC) and failed completely.In this paper,an algorithm is proposed based on the 2-D approximate radar imaging model.By minimizing a nonlinear least-squares cost function,the algorithm combines the parameter estimation with the compensation of MTRC errors.The Cramer-Rao bounds are derived and simulation results are also presented to demonstrate the performance of the algorithm.
Key words:motion through resolution cell error;compensation;super resolution;radar imaging

I. Introduction
Radar imaging is based on the scattering point model of the target. Radar usually emits a long-duration chirp signal, then uses a reference signal to dechirp the echo, and then arranges the dechirped echoes horizontally. Under certain conditions, it can be approximated as a two-dimensional sinusoidal signal model. Through two-dimensional Fourier transform, the two-dimensional image of the target can be reconstructed; using super-resolution algorithms [1-3], a more detailed two-dimensional target image can be obtained.
It should be pointed out that the above two-dimensional model assumes that the scattering point does not move beyond the resolution unit during imaging. It is approximately assumed that the movement of the scattering point only affects the phase shift of the echo, while the sub-echo The wave envelope remains fixed. This approximation is only applicable to imaging of finite small-sized targets near the reference point at small observation angles.
If the target is large, especially far away from the reference point, the multi-resolution unit movement (MTRC) will occur, making the image obtained with a simple two-dimensional model blurred. The traditional solution is to use polar coordinate-rectangular coordinate interpolation according to the rotation of the target. Interpolation will inevitably have errors, and super-resolution algorithms are usually based on parameterized estimates and are more sensitive to errors, which will affect the imaging quality.
This paper introduces a two-dimensional model with a higher approximation, and uses this model to obtain better results through super-resolution algorithm imaging.

2. Dimensional echo model
Assume that the target has K scattering points, and the radar illuminates the target from bottom to top with a plane wave (Figure 1). The target rotates relative to the radar beam with the reference point as the origin. After N pulses are emitted, the scattering point Pk moves to P′k. The vertical coordinate of the scattering point at the nth pulse is:

ykn=yk+Δykn=xksin(nδθ)+ykcos(nδθ),n=0,1,…,N-1 (1)

Where δθ is the rotation angle of adjacent pulses, and the total observation angle Δθ=(N-1)δθ. Considering that the radar transmits a long-duration line frequency modulation signal, the line frequency modulation is processed with the origin as the reference, and the signal is sampled at a frequency, and the target echo signal (discrete form) is obtained as follows:

g84.gif (2442 bytes) (2)

Where Ak is the complex amplitude of the sub-echo signal of the kth scattering point; fc and γ are the radar carrier frequency and modulation frequency respectively, c is the speed of light; and e(m,n) is the additive noise.

t84-1.gif (1497 bytes)

Figure 1. 2D radar target geometry

Since the observation angle Δθ is very small, we take the approximation sin(nδθ)≈nδθ and cos(nδθ)≈1, then equation (2) can be approximately written as:

g85-1.gif (1711 bytes) (3)

In the formula g85-2.gif (622 bytes)
The third term in the exponential term of formula (3) is the time-frequency coupling term, which is unique to the line frequency modulation signal (whose ambiguity function is an oblique ellipse). If a narrow pulse is used for transmission, this term does not exist. If this term is ignored, formula (3) becomes a commonly used echo two-dimensional sinusoidal signal model.
In fact, the third term of formula (3) is the "distance movement" term, which is proportional to the horizontal coordinate xk of the scattering point. It must be considered when the target area is large, and this is far from enough. The Doppler movement of the scattering point must also be considered. For this reason, let sin(nδθ)≈nδθ and cos(nδθ)≈1-(nδθ)2/2, then the more accurate approximation of formula (2) can be written as:

g85-3.gif (2315 bytes) (4)

Compared with equation (3), equation (4) adds two terms to the index. The first term is the "Doppler shift" term. The larger the ordinate yk is, the greater the impact is. This can make up for the deficiency of equation (3). The second term is the Doppler shift term of time-frequency coupling. Since Mγ/Fs<

g85-4.gif (1774 bytes) (5)

It should be pointed out that there is the following relationship between the parameters of each scattering point: ωk/μk=2γ/Fsfcδθ2 and ts85-1.gif (92 bytes) k/vk=fcFs/γδθ. Since the radar parameters (fc,γ,Fs) and the motion parameters (δθ) are known, only three of the five parameters to be estimated are independent. This paper assumes that the five parameters are independent, and the relationship between the parameters has been considered in the imaging calculation.
Let {ξk}Kk=1≡{αk,ωk, ts85-1.gif (92 bytes) k,μk,vk}Kk=1, now we want to estimate the parameter {ξk}Kk=1 from y(m,n).

3. Two-dimensional generalized RELAX algorithm
For the signal model shown in equation (5), let:

Y=[y(m,n)]M×N

Then in formula g85-5.gif (1215 bytes) (6)

g85-6.gif (3131 bytes)

Assume that the estimated value of ξk is g85-7.gif (561 bytes) , then the estimation problem of ξk can be solved by optimizing the following cost function:

g85-8.gif (1588 bytes) (7)

In the formula, ‖.‖F represents the Frobenius norm of the matrix, and ⊙ represents the Hadamard product of the matrix.
The optimization of C1 in the above formula is a multidimensional space optimization problem, which is very complicated. This paper generalizes the RELAX[3] algorithm to solve it. To this end, we first do the following preparation work, let:

g85-9.gif (1243 bytes) (8)

That is, assuming that { ts85-6.gif (102 bytes) i}i=1,2,…,K,i≠k has been found, then the minimization of C1 in equation (7) is equivalent to the minimization of the following equation:

C2(ξk)=‖Yk-αk(aM(ωk)bTN( ts85-1.gif (92 bytes) k)Pk)⊙Dk(vk)‖2F (9)

Let: Zk=YkP-1k⊙Dk(-vk) (10)
Since Pk is a unitary matrix, the modulus of each element of the matrix Dk |Dk(m,n)|=1, and it is obvious that the F norm of the matrix Yk and Zk is the same, so the minimization of C2 is equivalent to the minimization of the following formula:

C3=‖Zk-αkaM(ωk)bTN( ts85-1.gif (92 bytes) k)‖2F (11)

By finding the minimum value of αk for the above formula, we can obtain the estimated value ts82.gif (98 bytes) k of αk:

ts82.gif (98 bytes) k=aHM(ωk)Zkb*N( ts85-1.gif (92 bytes) k)/(MN) (12)

From equation (12), we can see that: is the value of ts82.gif (98 bytes) the normalized two-dimensional discrete Fourier transform of Zk at {ωk, k}, so as long as the estimated value { k, k, k, k} is obtained, k can be obtained by 2D-FFT . After substituting the estimated value k into equation (11), the estimated value { k, k, k, k} can be optimized by the following equation: ts85-1.gif (92 bytes)ts85-2.gif (93 bytes)ts85-3.gif (102 bytes)ts85-4.gif (105 bytes)ts85-5.gif (93 bytes)ts82.gif (98 bytes)
ts82.gif (98 bytes)ts85-2.gif (93 bytes)ts85-3.gif (102 bytes)ts85-4.gif (105 bytes)ts85-5.gif (93 bytes)

g85-10.gif (1590 bytes) (13)

It can be seen from the above formula that for a fixed value of {μk, vk}, the estimated value { ts85-2.gif (93 bytes) k, ts85-3.gif (102 bytes) k} is the two-dimensional frequency value at the main peak of the normalized periodogram |aHM(ωk)Zkb*N( k)|2/(MN). In this way, the optimization problem of formula (13) is reduced to: find a point { k, k} ts85-1.gif (92 bytes) within the possible range of values ​​on the (μk, vk) plane , at which the main peak of the periodogram |aHM(ωk)Zkb*N( k)|2/(MN) is larger than the main peaks at the other points. Therefore, we obtain the estimated value { k, k } of {μk, vk} through the above two-dimensional optimization , and then obtain the estimated value {k, k} of {ωk, k} from formula (13) . k}. In practice, in order to speed up the calculation, the optimization of the two-dimensional (μk, vk) plane can be implemented using the function Fmin() in Matlab. After the above preparations, the parameter estimation steps based on the generalized RELAX algorithm are as follows: Step 1: Assume that the number of signals K = 1, and use equations (13) and (12) to calculate 1. Step 2 (2): Assume that the number of signals K = 2, first substitute the 1 obtained in the first step into equation (8) to obtain Y2, and then use equations (13) and (12) to calculate 2; substitute the calculated 2 into equation (8) to obtain Y1, and then use equations (13) and (12) to recalculate 1. This process is repeated until convergence. Step 3: Assume that the number of signals K = 3, first Substitute 1 and 2 obtained in the second step into formula (8) to obtain Y3, and then use formula (13) and formula (12) to calculate 3; substitute the calculated 3 and 2 into formula (8) to obtain Y1, and then use formula (13) and formula (12) to recalculate 1; substitute the calculated 1 and 3 into formula (8) to obtain Y2, and then use formula (13) and formula (12) to recalculate 2. This process is repeated until convergence. Remaining steps: Let K = K + 1, and continue the above steps until K is equal to the number of signals to be estimated. The convergence criterion in the above process is the same as that of the RELAX algorithm, that is, compare the change value of the cost function C1 in the two iterative processes. If this change value is less than a certain value, such as ε = 10-3, the process is considered to converge. ts85-4.gif (105 bytes)ts85-5.gif (93 bytes)ts85-1.gif (92 bytes)ts85-4.gif (105 bytes)ts85-5.gif (93 bytes)ts85-1.gif (92 bytes)ts85-2.gif (93 bytes)ts85-3.gif (102 bytes)


ts85-6.gif (102 bytes)
ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)
ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)ts85-6.gif (102 bytes)

IV. Numerical simulation
1. Algorithm parameter estimation performance simulation
The simulation data is generated by equation (5), M=10, N=10, and the number of signals K=2. The signal parameters and experimental conditions are shown in Table 1, which is complex Gaussian white noise. Note that the frequency difference between the two signals is less than the FFT resolution Δf=Δω/(2π)=0.1. Table 1 gives the statistical results of the root mean square error of signal parameter estimation and the CR bounds for the corresponding situations. It can be seen that the estimated root mean square error is very close to the CR bound. In addition, the table also gives the estimated mean, which is also very close to the true value.

Table 1 Parameter estimation, CRB and comparison with RMS error for two-dimensional signals

2. SAR imaging simulation
Radar parameters are: center frequency f0 = 24.24 GHz, modulation frequency γ = 33.357 × 1011 Hz/s, bandwidth B = 133.5 MHz, pulse width tp = 40 μs. Four point targets are placed in a square, 50 meters apart, and the point in the lower left corner is used as the reference point. The radar is 1 km away from the target, the observation angle Δθ = 3.15, and the data length is 128 × 128. When the FFT imaging method is used, the longitudinal and lateral distance resolution is ρr = ρa = 1.123 meters. The maximum target range required to prevent the MTRC phenomenon is [4]: ​​longitudinal size Dr < 4ρ2r/λ = 40 meters, lateral size Da < 4ρ2a/λ = 40 meters. When the conventional super-resolution method is used, the target size Dr = Da > 10 meters will show a significant performance degradation. Figures 2 and 3 show the RELAX method and the extended RELAX (Extended Resolution Image Processing Method) in this paper, respectively. It can be seen that since the target is far away from the reference center, the distance movement has occurred in the horizontal and vertical directions, and the conventional super-resolution RELAX algorithm produces image blur. For the algorithm in this paper, a basically correct imaging result is obtained. Figures 4 and 5 compare the scattering point intensity estimation results of the RELAX algorithm and the generalized RELAX algorithm. It can be seen that the intensity of the scattering points (except the reference point) is reduced due to the influence of the distance movement in the RELAX algorithm. For the algorithm in this paper, the scattering point intensity is close to the true value.

t84-2.gif (2232 bytes) t86-1.gif (2338 bytes)

Figure 2 RELAX imaging results under range movement error

Figure 3: Distance movement error

t86-2.gif (3010 bytes) t86-3.gif (2871 bytes)

Fig.4 Signal intensity estimated by RELAX method and generalized RELAX imaging results

Figure 5 Signal strength estimated by generalized RELAX method

5. Conclusion
The existing radar imaging super-resolution algorithm is based on the two-dimensional sinusoidal signal model of the target echo signal, so it is only applicable when the target is located in a small area near the reference point. When the target is far away from the reference point, the model error, especially the distance movement error, will seriously degrade the algorithm performance or make it invalid. To this end, this paper proposes a super-resolution algorithm based on the radar imaging approximate two-dimensional model, thereby expanding the scope of application of the super-resolution algorithm. Further work in this paper includes SAR measured data imaging and ISAR maneuvering target imaging, and the results will be reported in another paper.

Appendix: CR bounds for parameter estimation
Below we give the CR bound expression for parameter estimation of two-dimensional signals as shown in equation (5). At the same time, it is assumed that the additive noise in equation (5) is zero-mean Gaussian colored noise, and its covariance matrix is ​​unknown. Let:

y=vec(Y) (A.1)
e=vec(E) (A.2)
dk=vec(Dk) (A.3)

Where vec(X)=(xT1,xT2,…,xTN)T, and vector xn(n=1,2,…,N) is the column vector of matrix X. We rewrite equation (5) into the following vector form:

g86.gif (1322 bytes) (A.4)

In the formula ts86-4.gif (84 bytes) , represents the Kronecker product, Ω=[{[P1bN( ts85-1.gif (92 bytes) 1)] ts86-4.gif (84 bytes) aM(ω1)}⊙d1…{[PkbN( ts85-1.gif (92 bytes) K)] ts86-4.gif (84 bytes) aM(ωK)}⊙dK], α=(α1,α2,…,αK)T.
Let Q=E(eeH) be the covariance matrix of e, then for the two-dimensional signal model shown in formula (A.4), the Slepian-Bangs formula generalized for the ijth element of its Fisher information matrix (FIM) is[5,6]:
(FIM)ij=tr(Q-1Q′iQ-1Q′j)+2Re[(αHΩH)′iQ-1(Ωα)′j] (A.5)
In the formula, X′i represents the derivative of the matrix X with respect to the i-th parameter, tr(X) is the trace of the matrix, and Re(X) is the real part of the matrix. Since Q is independent of the parameters in Ωα, and Ωα is also independent of the elements of Q, it is obvious that FIM is a diagonal matrix. Therefore, the CR bound matrix of the parameter to be estimated is obtained from the second term of (A.5).

令:η=([Re(α)]T[Im(α)]TωT ts85-1.gif (92 bytes) TμTvT)T (A.6)

In the formula, ω=(ω1,ω2,…,ωK)T, μ=(μ1,μ2,…,μK)T, ts85-1.gif (92 bytes) =( ts85-1.gif (92 bytes) 1, ts85-1.gif (92 bytes) 2,…, ts85-1.gif (92 bytes) K)T, v=(v1,v2,…,vK)T.
Let: F=[Ω jΩ DωΘ D ts85-1.gif (92 bytes) Θ DμΘ DvΘ] (A.7)
In the formula, the k-th column of the matrices Dω, D ts85-1.gif (92 bytes) , Dμ, Dv are: ts69-1.gif (92 bytes) [{[PkbN( ts85-1.gif (92 bytes) k)] ts86-4.gif (84 bytes) aM(ωk)}⊙dk]/ ts69-1.gif (92 bytes) ωk, ts69-1.gif (92 bytes) [{[PkbN( ts85-1.gif (92 bytes) k)] ts86-4.gif (84 bytes) aM(ωk)}⊙dk]/ ts69-1.gif (92 bytes) ts85-1.gif (92 bytes) k, ts69-1.gif (92 bytes) [{[PkbN( ts85-1.gif (92 bytes) k)] ts86-4.gif (84 bytes) aM(ωk)}⊙dk]/ ts69-1.gif (92 bytes) μk, ts69-1.gif (92 bytes) [{[PkbN( ts85-1.gif (92 bytes) k)] ts86-4.gif (84 bytes) aM(ωk)}⊙dk]/ ts69-1.gif (92 bytes) vk, Θ=diag{α1 α2 … αK}. Then the CRB matrix with respect to the parameter vector η is

CRB(η)=[2Re(FHQ-1F)]-1 (A.8)

Reference address:Approximate two-dimensional model of radar imaging and its super-resolution algorithm

Previous article:Improving the detection of weak moving targets using adaptive wavelet transform
Next article:Ultra-high-speed radar digital signal processing technology

Latest Analog Electronics Articles
Change More Related Popular Components

EEWorld
subscription
account

EEWorld
service
account

Automotive
development
circle

About Us Customer Service Contact Information Datasheet Sitemap LatestNews


Room 1530, 15th Floor, Building B, No.18 Zhongguancun Street, Haidian District, Beijing, Postal Code: 100190 China Telephone: 008610 8235 0740

Copyright © 2005-2024 EEWORLD.com.cn, Inc. All rights reserved 京ICP证060456号 京ICP备10001474号-1 电信业务审批[2006]字第258号函 京公网安备 11010802033920号