2017 International Conference on Computer, Electronics and Communication Engineering (CECE 2017) ISBN: 978-1-60595-476-9
Stepped Frequency Continuous Wave Ground Penetrating Radar
Imaging Algorithm Based on Multi-task Bayesian Compressive Sensing
Yan-peng SUN, Xiao-dan LU
*, Le-le QU and Yi-lin WANG
Department of Electronic Information Engineering, Shenyang Aerospace University, No.37 Daoyinan Street 110136, Liaoning, China
*Corresponding author
Keywords: SFCW-GPR, Compressive sensing, BCS, MT-BCS.
Abstract. Aiming at the joint sparsity of target imaging space of SFCW-GPR, the idea of multi-task learning is introduced into the Bayesian compressive sensing reconstruction algorithm, multi-task Bayesian compressive sensing(MT-BCS) algorithm is proposed in the paper. A common prior hierarchical Bayesian model is used for different tasks, MT-BCS algorithm can fully exploit the statistical characteristics and structural information of radar echo data and recover original signals from far fewer random samples. The simulation results show that the reconstruction accuracy of MT-BCS algorithm is better than BCS algorithm under the same conditions.
Introduction
SFCW-GPR is one of the Ground Penetrating Radar (GPR) systems. GPR as non-destructive technique for detecting underground targets has been widely used in many fields, such as earth science, environmental engineering, geological exploration, archeology and so on[1].Because the working frequency of SFCW-GPR system is step by step, it takes a long time to achieve working bandwidth, the imaging speed is slow[2]. How to effectively shorten the data acquisition time and improve the imaging speed of SFCW-GPR system are the problems to be solved. The problems can be solved when theory of CS is proposed. The CS theory have proved, when the signal is sparse in the transform domain, sampling frequency can no longer depend on the bandwidth of the signal, which mainly depend on two-basic principles: sparsity and irrelevance[3].
Focusing on the datas come from the same scenario have statistic correlation. MT-BCS algorithm based on sparse Bayesian learning has been proposed. A common prior hierarchical Bayesian model is used in the algorithm for different tasks, making full use of the statistical correlation between the tasks, giving each element of the coefficient vector a priori probability distribution to limit the complexity of the model and introduce hyperparameters[4,5,6]. The simulation results show that the SFCW-GPR reconstruction algorithm based on MT-BCS can take into account both the computational efficiency and the accuracy of reconstruction.
Signal Model
x w
1
[image:2.612.131.483.64.191.2]KL
Figure 1. SFCW-GPR model. Figure 2. Grid division.
We assume the antenna measurement apertures areM , the scanning frequency of transmit antennas fromf0 to fN1in a scan period. Targets pare existed in the detection area. The complex echo signals can be obtained in each antenna measurement apertures as:
, 1
( ) P exp( 2 )
m n p n p m
p
f j f
s τ
(1) Where m1, 2M n, 1, 2N ,
p denote complex reflection coefficient of thetargetp,τp m, denote round-trip delay from antenna measurement apertures m to the target p. The figure1 can be converted into KL1 dimensions vector through column stack shown in figure
2 and denoted as wx.The formula (1) can also be expressed as:
m m x
S B w (2)
Where dictionary matrixBm N KL,Sm [ ( ), , (s0 f0 sm fN1)]T areN1dimensions frequency domain measurement vectors. sm( )fn are echo datas that the measurement aperture is mand the frequency is fn. The jth column of dictionary matrix Bmcan be expressed as:
2 0m j, , , 2 N1m j,T
j f j f
j e e
m
B
(3) Where j1,2KL,
m j, are round-trip delay from grid jto the measurement aperture m . The antennas measurement apertures are m , so all measurement datas can be combined the vectorsx
S , T
m
T T T
x 1 2
S S ,S , ,S ,SxNM1 . The corresponding dictionary matrix Bx can express as T
m
T T T
x 1 2
B B ;B ; ;B .The relationship between Sx and reflection coefficient vectorswx as follows:
x x x
S B w (4) In general, reflection coefficient vectorswxare sparse, we randomly select the apertures Q1 from antennas measurement apertures m and the datasQ2 from measurement datas N .Measurement matrixΨQ Q1 2NMandQ Q1 2NM ,the measurement vectors txcan be expressed as:
x x x x x
x ΨS ΨB w Θ w
t , Θx ΨBx, ΘxQ Q1 2KL (5)
MT-BCS Imaging Algorithm
R e( )
R e(
)
Im ( )
Im (
)
x x
x x
x x
t
w
v
θ
t
w
Re( ) Im( )
Im( ) Re( )
x x
x
x x
Θ Θ
Φ
Θ Θ (6)
The formula(5) can be rewritten as:
x
x x
xv
Φ θ
n
(7)( 1,..., )
x x M
n are residual error vector corresponding to each task, each element in the residual
error vector are following normal distribution of zero mean and variance reciprocal is
0. Thedensity function of the compressed sampling vector vx under the parameters θxand
0can beexpressed[9]:
2
0 2
0
0
2
( ) ( ) e x p ( )
2
x x x x
N
x x
p v / θ ,
v Φ θ(8) For each element of θx is assumed to be Gauss prior distribution of zero mean:
2
1 ,
1
(
x)
K L(
x j/ 0,
j)
j
p
N
v / α
(9)
,
x j
can be expressed the element j in the task x.
1, 2, , 2
T KL
α
are a set parameters that
shared by all tasks. Hyper parameter
α
and residual error parameter
0 is assumed to follow gamma distribution. According to Bayesian rule, posterior probability density function of x j, are following multidimensional Gaussian distribution[10].0 0
0
(
/
,
) (
/ )
(
/
, ,
)
(
/
,
)
(
/
,
) (
/ )
x x x
x x x x x
x x x x
p
p
p
N
d
p
p
v
θ
θ
α
θ
v α
θ
μ Σ
θ
v
θ
θ
α
(10)
x
μ
and Σxare the means and covariance respectively of coefficient vector for each task, they can
be expressed as:
0
x
x x xT
μ
Σ Φ v
10
(
)
x
x x
T
Σ
Φ Φ
A
(11)Where Adiag( , 1 2,2KL),Hyper parameter
can be obtained by fast relevance vectormachine[11], we obtain hyper parameter α, the coefficient vector θx can be solved by formula (11).
Simulation and Experimental Results
BCS ( ) crossrange cm () dow nr ange cm
5 10 15 20 25 30 35 40 30 32 34 36 38 40 42 44 46 48 50 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 BCS ( ) crossrange cm () dow nr ange cm
5 10 15 20 25 30 35 40 30 32 34 36 38 40 42 44 46 48 50 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 MT-BCS crossrange(cm) do w nr ange( cm )
5 10 15 20 25 30 35 40 30 32 34 36 38 40 42 44 46 48 50 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 MT-BCS crossrange(cm) dow nr an ge( cm )
5 10 15 20 25 30 35 40 30 32 34 36 38 40 42 44 46 48 50 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
[image:4.612.86.523.68.159.2](a)Measurement ratio is 15% (b) Measurement ratio is 25% (a)Measurement ratio is15% (b) Measurement ratio is25% Figure 3. Reconstruction results of BCS. Figure 4. Reconstruction results of MT-BCS.
[image:4.612.80.512.252.518.2]The experimental results show that BCS algorithm have more noise points and false targets. The reconstruction reflection coefficients and computational time of the two algorithms are given in table 1.
Table 1. Comparision of two algorithms. Imaging methods Measurement ratio Reflection coefficient of
target Computational time BCS algorithm 15%
25%
(0.1032,0.0906,0.1012) (0.1014,0.1018,0.0901)
0.842s 1.036s MT-BCS algorithm 15%
25%
(0.1008,0.0926,0.0914) (0.1021,0.1016,0.1018)
0.594s 0. 782s
The Mean Squared Error (MSE) is used to quantitatively analyze the effect of reconstruction.
2 2
ˆ
MSE f f f
, f and fˆ represent the true and estimated value of the signal.
Figure 5. Comparision of reconstruction effects under different measurement ratio.
The results show that the MT-BCS algorithm can get better reconstruction performance than the BCS algorithm under the same observation data.
Summary
In the paper, the MT-BCS algorithm is be introduced. MT-BCS algorithm can exploit the statistical and structural characteristics of sparse signal, achieving reconstruction for many relevant signals at the same time. Experimental results have shown that the reconstruction performance of MT-BCS is better than the BCS algorithm under few observation data.
Acknowledgement
L2013069.
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