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:
(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.
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: (3)
In the formula
(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<
(5)
It should be pointed out that there is the following relationship between the parameters of each scattering point: ωk/μk=2γ/Fsfcδθ2 and
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.
3. Two-dimensional generalized RELAX algorithm
Y=[y(m,n)]M×N
Then
in formula
(6)
Assume that the estimated value of ξk is
, then the estimation problem of ξk can be solved by optimizing the following cost function:
(7)
In the formula, ‖.‖F represents the Frobenius norm of the matrix, and ⊙ represents the Hadamard product of the matrix.
(8)
That is, assuming that {
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(
k)Pk)⊙Dk(vk)‖2F (9)
Let: Zk=YkP-1k⊙Dk(-vk) (10)
C3=‖Zk-αkaM(ωk)bTN(
k)‖2F (11)
By finding the minimum value of αk for the above formula, we can obtain the estimated value
k of αk:
k=aHM(ωk)Zkb*N(
k)/(MN) (12)
From equation (12), we can see that:
is
the value of
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:
(13)
It can be seen from the above formula that for a fixed value of {μk, vk}, the estimated value {
k,
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}
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.
IV. Numerical simulation
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. |
Figure 2 RELAX imaging results under range movement error |
Figure 3: Distance movement error |
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
y=vec(Y) (A.1)
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: (A.4)
In the formula
, represents the Kronecker product, Ω=[{[P1bN(
1)]
aM(ω1)}⊙d1…{[PkbN(
K)]
aM(ωK)}⊙dK], α=(α1,α2,…,αK)T.
令:η=([Re(α)]T[Im(α)]TωT TμTvT)T (A.6)
In the formula, ω=(ω1,ω2,…,ωK)T, μ=(μ1,μ2,…,μK)T,
=(
1,
2,…,
K)T, v=(v1,v2,…,vK)T.
CRB(η)=[2Re(FHQ-1F)]-1 (A.8) |
Previous article:Improving the detection of weak moving targets using adaptive wavelet transform
Next article:Ultra-high-speed radar digital signal processing technology
- Popular Resources
- Popular amplifiers
- High signal-to-noise ratio MEMS microphone drives artificial intelligence interaction
- Advantages of using a differential-to-single-ended RF amplifier in a transmit signal chain design
- ON Semiconductor CEO Appears at Munich Electronica Show and Launches Treo Platform
- ON Semiconductor Launches Industry-Leading Analog and Mixed-Signal Platform
- Analog Devices ADAQ7767-1 μModule DAQ Solution for Rapid Development of Precision Data Acquisition Systems Now Available at Mouser
- Domestic high-precision, high-speed ADC chips are on the rise
- Microcontrollers that combine Hi-Fi, intelligence and USB multi-channel features – ushering in a new era of digital audio
- Using capacitive PGA, Naxin Micro launches high-precision multi-channel 24/16-bit Δ-Σ ADC
- Fully Differential Amplifier Provides High Voltage, Low Noise Signals for Precision Data Acquisition Signal Chain
- Innolux's intelligent steer-by-wire solution makes cars smarter and safer
- 8051 MCU - Parity Check
- How to efficiently balance the sensitivity of tactile sensing interfaces
- What should I do if the servo motor shakes? What causes the servo motor to shake quickly?
- 【Brushless Motor】Analysis of three-phase BLDC motor and sharing of two popular development boards
- Midea Industrial Technology's subsidiaries Clou Electronics and Hekang New Energy jointly appeared at the Munich Battery Energy Storage Exhibition and Solar Energy Exhibition
- Guoxin Sichen | Application of ferroelectric memory PB85RS2MC in power battery management, with a capacity of 2M
- Analysis of common faults of frequency converter
- In a head-on competition with Qualcomm, what kind of cockpit products has Intel come up with?
- Dalian Rongke's all-vanadium liquid flow battery energy storage equipment industrialization project has entered the sprint stage before production
- Allegro MicroSystems Introduces Advanced Magnetic and Inductive Position Sensing Solutions at Electronica 2024
- Car key in the left hand, liveness detection radar in the right hand, UWB is imperative for cars!
- After a decade of rapid development, domestic CIS has entered the market
- Aegis Dagger Battery + Thor EM-i Super Hybrid, Geely New Energy has thrown out two "king bombs"
- A brief discussion on functional safety - fault, error, and failure
- In the smart car 2.0 cycle, these core industry chains are facing major opportunities!
- The United States and Japan are developing new batteries. CATL faces challenges? How should China's new energy battery industry respond?
- Murata launches high-precision 6-axis inertial sensor for automobiles
- Ford patents pre-charge alarm to help save costs and respond to emergencies
- New real-time microcontroller system from Texas Instruments enables smarter processing in automotive and industrial applications
- Analog Basics: How Sample and Hold Circuits Work and Ensure ADC Accuracy
- The role of the volatile keyword
- Apple's contract factory violated the rules by using student workers, Apple responded by suspending its new business cooperation
- AD sampling average current
- Assembling a single-phase solid-state relay circuit using discrete components
- Motor Control Advanced 3——PID Cascade Control (with full code download)
- [Evaluation of domestic FPGA Gaoyun GW1N-4 series development board] ——9. Internal OSC and rPLL IP core test
- Zero-Drift Amplifiers: Features and Benefits
- Interference issues
- Help, the SD card cannot communicate normally, and the measured pin voltage is abnormal