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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Low Complexity Joint Super-Resolution Algorithm for Range Azimuth of TDM-MIMO LFMCW Radar 1</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Bingxia Cao</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Runhu Liu</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Fenggang Yan</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Ming Jin</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Institute of Information Engineering, Harbin Institute of Technology</institution>
          ,
          <addr-line>Weihai, CN 264200</addr-line>
        </aff>
      </contrib-group>
      <abstract>
        <p>Aiming to solve the problem that the joint range and azimuth super-resolution algorithm of vehicle millimeter wave radar is too complex to be implemented quickly, a low complexity joint super-resolution method based on direct selection of frequency domain data is presented. The algorithm first transforms the space-time range-domain joint data into frequency domain by fast Fourier transformation, and stores and processes the two-dimensional frequency domain data of the area of interest. Based on the equivalence between Fourier transformation and beam space transformation based on DFT transformation, the range-azimuth joint MUSIC super-resolution in frequency domain data is achieved, and the fast joint estimation of target information is completed. The orthogonality of frequency domain subspace and the theory of frequency domain beam dimension reduction super-resolution algorithm are deduced. The relationship between the resolution and estimation performance of distance and azimuth of the algorithm and signal-to-noise ratio is simulated. The simulation results show that the accuracy and resolution of the algorithm are much higher than traditional FFT, and the computational complexity of the algorithm is greatly reduced compared with traditional MUSIC.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;LFMCW</kwd>
        <kwd>Joint distance-azimuth estimation</kwd>
        <kwd>Frequency domain</kwd>
        <kwd>Beam space</kwd>
        <kwd>MUSIC</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <sec id="sec-1-1">
        <title>Among the target parameter estimation algorithms of vehicle mounted radar, the estimation</title>
        <p>accuracy and resolution of the traditional Fast Fourier Transform (FFT) algorithm is insufficient. And
super-resolution algorithms such as Multiple Signal Classification (MUSIC) algorithm and Estimating
Signal Parameter via Rotational Invariance Technologies (ESPRIT) algorithm have high accuracy and
resolution but huge computation.</p>
      </sec>
      <sec id="sec-1-2">
        <title>The high efficiency and low complexity of space-time multi parameter joint super-resolution</title>
        <p>algorithm is an urgent problem to be solved at present, which can not be avoided in engineering.
Bienvenu G[1] et al. proposed a high-resolution target bearing estimation method to improve accuracy
and resolution and even the statistical stability[3]-[4].</p>
      </sec>
      <sec id="sec-1-3">
        <title>Based on the joint super-resolution complexity of vehicle mounted radar, this paper proposes a</title>
        <p>range azimuth joint super-resolution method based on frequency domain beam dimensionality
reduction. Based on the equivalence of range angle FFT and multi-dimensional Discrete Fourier
Transform (DFT) beam space transformation of space-time data, the corresponding frequency domain
data area of the target area is selected according to the prior information of the target, MUSIC joint
super-resolution based on beam dimension reduction. The dimension of beam space data is greatly
reduced, which makes it possible to realize joint super resolution engineering and realize fast joint
estimation of multiple parameters of vehicle borne radar. Compared with the traditional FFT
algorithm, the resolution of target parameter estimation is significantly improved, which is a fast joint
super-resolution algorithm feasible in engineering.
2. TDM-MIMO LFMCW Radar Signal Model</p>
      </sec>
      <sec id="sec-1-4">
        <title>Set the number of transmitting antennas of Division Multiplexing Multiple Input Multiple Output</title>
        <p>（TDM-MIMO）radar as LTX , and the number of receiving antenna elements as LRX . The simplified
array model is shown in Figure 1(a). Set the spacing of receiving antenna elements as dr =λ 2 , the
spacing of transmitting antenna elements as dt , and meet the requirements of dt =LRX × dr . Assume
that the spacing between any receiving antenna lRX and the first receiving antenna in the receiving
antenna array is drlRX = (lRX −1) dr .</p>
        <sec id="sec-1-4-1">
          <title>Transmitting array</title>
          <p>Receiving array RxLRx
Tx1</p>
          <p>dt
Tx1
...</p>
          <p>TxLTx</p>
          <p>Rx1 dr
...</p>
          <p>LRx
...</p>
          <p>TxLTx
...
...</p>
          <p>LRx
...
f
B
f
fIF</p>
        </sec>
        <sec id="sec-1-4-2">
          <title>Transmit signal</title>
          <p>Tm
τ</p>
        </sec>
        <sec id="sec-1-4-3">
          <title>Echo signal</title>
          <p>t</p>
        </sec>
        <sec id="sec-1-4-4">
          <title>Beat signal</title>
          <p>Virtual array：L=LTx×LRx
t
(a)TDM-MIMO radar array model.
(b) Sawtooth time-frequency diagram.</p>
        </sec>
      </sec>
      <sec id="sec-1-5">
        <title>The sawtooth Linear Frequency Modulated Continuous Wave (LFMCW) signal and echo signal is shown in Figure 1(b).</title>
        <p>Under the above model, obtain TDM-MIMO LFMCW radar sawtooth beat signal model[5] x(t) as
x (t ) = Ampe
j2π  2vcfc + 2μcR + 2μvmTm t+ 2Rcfc + 2 fcvmTm +ldr sinθ </p>
        <p>c  c λ  + G (t )</p>
        <p>In the formula, Amp represent the signal amplitudes, fc represents the signal carrier frequency,
μ = B Tm represents the FM slope, where B represents the signal bandwidth, Tm represents the signal
repetition period, m = 0,1...., M −1 represents the sequence number of repetition period, l = 0,1...., L −1
represents the array element sequence number of virtual array receiving antenna, dr = λ 2 is the
virtual antenna spacing. G(t) is additive white Gaussian noise.</p>
      </sec>
      <sec id="sec-1-6">
        <title>Assume that the number of sampling points in each Chirp is N , and according to space-time equivalence, the guidance vectors for super-resolution of angle dimension and distance dimension are:</title>
        <p>aR ( R) = 1, e− j2π 2cμfsR ,, e− j2π 2cμfsR(N −1) 
 </p>
        <p>T</p>
        <p>
aθ (θ ) = 1, e

− j2π d sinθ
λ ,, e
− j2π d sinθ (L−1) T
λ 

3. Beam space transformation in frequency domain based on time-frequency
equivalence</p>
        <p>
          The beam space dimension reduction super-resolution algorithm based on DFT transform is to
obtain the beam space data by multiplying the original sampling data and the beam space conversion
matrix. At the same time, the steering vector also reduces the dimension according to the beam
selection. In this method, the multi-dimensional data are first FFT transformed, and only the
frequency domain data corresponding to the parameter region of interest are stored; Only when the
(
          <xref ref-type="bibr" rid="ref1">1</xref>
          )
(
          <xref ref-type="bibr" rid="ref2">2</xref>
          )
data directly selected in the frequency domain is equivalent to the beam space transformation data, the
super-resolution of some frequency domain data is equivalent to the beam space reduced
superresolution of the original data.
        </p>
        <p>
          According to reference [6] and space-time equivalence, the beam conversion matrix in the beam
space array flow pattern of each dimension is defined. The beam transformation matrices defining the
angle and range dimensions are WθH ∈ Lb×L ,WRH ∈ Nb×N respectively, and the number of effective
beam selections in the angle and range dimensions are Lb , Nb respectively, that is, the reduced
dimension data length. Then the l and n elements are
wθH = 1 e− jl 2Lπb  e− j(Lb −1)l 2Lπb  wRH = 1 e− jn 2Nπb ,, e− j(Nb −1)n 2Nπb  (
          <xref ref-type="bibr" rid="ref3">3</xref>
          )
        </p>
        <p>   </p>
        <p>In the formula, l, 0 ≤ l ≤ ( Lb −1) , Lb ≤ L , when Lb = L , that is, WθH is the angle dimension full beam
transformation matrix. 0 £ n £ (Nb - 1), Nb £ N , when Nb = N , WRH is the range dimension full
beam transformation matrix.</p>
        <p>Assuming that the matrices of one-dimensional Fourier transform are FN and FL respectively,
where N、L respectively represent the length of the vector to be operated in the distance dimension
and angle dimension, and data X NL is the distance angle two-dimensional raw data of N × L , then the
frequency domain data matrix YNL obtained by two-dimensional Fourier transform is expressed as:</p>
        <p>YNL = FN X NL FLT</p>
      </sec>
      <sec id="sec-1-7">
        <title>From Eq. (5)and Eq.(6), it can be seen that the two-dimensional beam space transform is</title>
        <p>
          equivalent to the two-dimensional Fourier transform. Eq. (
          <xref ref-type="bibr" rid="ref5">5</xref>
          )is another expression of two-dimensional
FFT, and also has the same form as that of two-dimensional beam space transformation when all
beams are taken; That is, two-dimensional FFT and two-dimensional beam space are equivalent in full
beam. When the two dimensions of beam space dimensionality reduction are reduced to Lb and Nb
respectively, it is also corresponding to the two-dimensional FFT data directly selecting data
according to the linear correspondence of the beam. Therefore, it is equivalent to take 2D frequency
domain data directly and reduce the dimension of 2D beam space.
        </p>
        <p>
          The above proves the equivalence of beam space dimensionality reduction and direct selection of
frequency domain data. For the beam space super-resolution algorithm, literature [6] has completed
the one-dimensional MUSIC proof based on the beam space. The beam space based MUSIC
algorithm can be expanded from one-dimensional to two-dimensional through equation (
          <xref ref-type="bibr" rid="ref5">5</xref>
          ). In the
range azimuth two-dimensional joint estimation, equation (
          <xref ref-type="bibr" rid="ref6">6</xref>
          ) realizes the dimensionality reduction
transformation from the original data matrix X NL to the data matrix Z , which is covariance
estimation It provides a basis for reducing the computation of eigenvalue decomposition and
subsequent peak searching operations. The beam space search guidance vector is defined as:
        </p>
      </sec>
      <sec id="sec-1-8">
        <title>From left to right, it is FFT for each column, from right to left, it is FFT for each row, and it is the</title>
        <p>same to do the left first and the right first. Two dimensional Fourier transforms are two
onedimensional Fourier transforms, and they are independent of order. The same is true for higher
dimensional Fourier transforms. If x1,, xL is the column vector of X NL , X NL can be written as</p>
        <p>L
X NL =  xieiT transformation, where ei is the ith column of the identity matrix IL , so
i</p>
        <p>  L  L L
vec (YNL ) = vec ( FN X NL FLT ) = vec FN   xieiT  FLT  =  vec ( FN xieiT FLT ) =  vec{( FN xi )( FLei )T }
 i=1  i=1 i=1</p>
        <p>L L
=  FLei ⊗ FN xi = ( FL ⊗ FN )  (ei ⊗ xi ) = ( FL ⊗ FN ) vec ( X NL )</p>
        <p>i=1 i=1</p>
      </sec>
      <sec id="sec-1-9">
        <title>Where ⊗ represents Kronecker multiplication. Reference [7] defines the data matrix after twodimensional beam space transformation as Z , and</title>
        <p>
          vec ( Z ) = (WRH ⊗WθH ) vec ( X NL )
(
          <xref ref-type="bibr" rid="ref4">4</xref>
          )
(
          <xref ref-type="bibr" rid="ref5">5</xref>
          )
(
          <xref ref-type="bibr" rid="ref6">6</xref>
          )
        </p>
      </sec>
      <sec id="sec-1-10">
        <title>The covariance matrix is:</title>
        <p>b (θ, R ) = (WRH aR ) ⊗ (WθH aθ ) = bR ⊗ bθ</p>
        <p>Rbeam−2MUSIC =</p>
        <p>1
Nb Lb</p>
        <p>
          ZZ H
(
          <xref ref-type="bibr" rid="ref7">7</xref>
          )
(8)
(9)
        </p>
        <p>After eigenvalue decomposition, the noise subspace Un−beam−2MUSIC can be obtained, and the spectral
peak search function is obtained as follows:</p>
        <p>Pbeam−2MUSIC = bH (θ, R )Un−beam−2MUSICUnH−beam−2MUSICb (θ, R)
1</p>
        <p>The spectral peak is obtained by searching the spectral peak of the above equation, and the
corresponding information of the peak is the two-dimensional information of the range azimuth angle
of the target. Compared with the traditional two-dimensional MUSIC algorithm, the MUSIC
algorithm after the beam space reduces the data dimension in terms of covariance estimation,
eigenvalue decomposition and spectral peak search, greatly reducing the calculation time.Based on the
joint super-resolution in the frequency domain, the data storage pressure and computational
complexity have been significantly reduced. According to existing research, the resolution and
parameter estimation performance of the beam space dimension reduction algorithm under the
condition of reasonable beam selection.</p>
      </sec>
    </sec>
    <sec id="sec-2">
      <title>4. Simulation experiment</title>
      <sec id="sec-2-1">
        <title>The conditions for simulation are as follows: The 24GHz millimeter wave TDM-MIMO radar</title>
        <p>platform transmits FMCW signals with a bandwidth of 150MHz. The period of a Chirp is 16 us, the
number of snapshots is 300, the number of transmitting and receiving antennas is 2 and 15
respectively. The search points of azimuth dimension and distance dimension are ls = 89, ns = 236 . The
number of wave beams in angle dimension and distance dimension is Lb = 8 and Nb = 13 respectively.
Set the parameters as Target1: (110 m, 12 °); Target2: the (110.5 m ,15 °).
4.1 Effective Estimation Diagram of Target Information</p>
        <p>When plotting SNR = 0 dB , the range velocity dimension effectiveness estimation diagram of the
range azimuth joint frequency domain beam reduction MUSIC algorithm is compared with the
effectiveness estimation diagram of the traditional 2DFFT algorithm, as shown in Figure 2 and Figure</p>
      </sec>
      <sec id="sec-2-2">
        <title>3 respectively.</title>
        <p>)
B
(edud
lti
p
m</p>
        <p>A
(a) The proposed algorithm spectral peak estimation
(b) Effective estimation of the proposed algorithm
(a) 2DFFT algorithm joint information estimation spectral peak (b) 2DFFT algorithm joint information effective estimation</p>
      </sec>
      <sec id="sec-2-3">
        <title>It can be seen from the observation in Figure 2 that the algorithm proposed in this paper can</title>
        <p>effectively realize the effective estimation of target information. The comparison between Figure 3
and Figure 2 shows that under this condition, 2DFFT cannot distinguish two targets. The algorithm
proposed in this paper can achieve effective resolution of two targets and more accurate parameter
estimation.
4.2 Target Information Distribution Map</p>
        <p>Through 50 Monte Carlo experiments, parameters distribution diagram of the proposed algorithm
in this paper and 2DFFT algorithm are compared as in Figure 4.
14.5
14
13.5
13
12.5
120
Azimuth true value 1
Azimuth true value 2
Proposed algorithm azimuth estimate1
Proposed algorithm azimuth estimate2
2DFFT azimuth estimate</p>
        <p>Azimuth true value 1
Azimuth true value 2
Proposed algorithm azimuth estimate1
Proposed algorithm azimuth estimate2
2DFFT azimuth estimate
(a) Distance dimension target information distribution.</p>
        <p>(b) Azimuth dimension target information distribution.</p>
      </sec>
      <sec id="sec-2-4">
        <title>It can be seen from Figure 4 that under the current simulation conditions, the traditional 2DFFT algorithm cannot complete the target resolution of Target1 and Target2, while the algorithm proposed in this paper can successfully resolve two targets. The algorithm realizes two-dimensional superresolution.</title>
        <p>4.3 Performance Analysis - RMSE Statistics</p>
        <p>Set the echo signal to noise ratio variation range of the signal as −30 dB:10 dB:20 dB , and the
number of Monte Carlo is 50. The traditional 2DFFT algorithm and the proposed algorithm proposed
in this paper are used to analyze the estimation error of Target1. The experimental results are as
follows.
1.2
1
0
-30 -25 -20 -15 -10 SNR-5(dB) 0 5 10 15 20
0
-30 -25 -20 -15 -10 SNR-5(dB) 0 5 10 15 20
(a) Distance dimension RMSE.</p>
        <p>(b) Azimuth dimension RMSE.</p>
      </sec>
      <sec id="sec-2-5">
        <title>It can be seen from the simulation results in Figure 5 that under different signal-to-noise ratios, the</title>
        <p>proposed algorithm proposed in this paper has higher estimation accuracy than the traditional 2DFFT
algorithm in terms of target range and angle dimensions, and its estimation performance improves
with the increase of signal-to-noise ratio, and the range dimension estimation accuracy is slightly
higher than the angle dimension estimation accuracy.</p>
      </sec>
    </sec>
    <sec id="sec-3">
      <title>4.4 Complexity analysis</title>
      <sec id="sec-3-1">
        <title>According to the above parameters, for the traditional 2DMUSIC algorithm, the data storage</title>
        <p>amount is  (( NL)) after data acquisition. The algorithm proposed in this paper can reduce the data
storage amount to  (( Nb Lb )) , which can reduce the data storage amount by (30 × 200) (8×13) = 57.7 .
ae 3 ö
Based on MUSIC joint super-resolution algorithm, the computational complexity includes  ççç(NL) ÷÷
è ÷ø
of eigenvalue decomposition processing part and  ((NL) nl ) of spectral peak search part. The total
ae 3 ö
complexity of the algorithm is  ççç(NL) +(NL) nl÷÷÷ . The complexity of the proposed algorithm,
è ø
ae 3 ö
eigenvalue processing and spectral peak search is reduced to  ççç(NbLb ) ÷÷÷ø and  ((NbLb ) nl )
è
respectively, and t Total computational complexity reduced to 6.5×104 . When the selected target area
is small, the number of beams can also be smaller to further reduce the complexity.</p>
      </sec>
    </sec>
    <sec id="sec-4">
      <title>5. Conclusion</title>
      <p>In this paper, a range azimuth joint super-resolution algorithm based on frequency domain beam
dimensionality reduction for vehicle borne radar is proposed. Compared with the traditional 2DFFT
algorithm, the algorithm can effectively improve the resolution and estimation accuracy. Compared
with the general MUSIC algorithm, the dimensionality reduction of the frequency domain space-time
beam greatly reduces the data storage pressure and the scale of data processing, realizes the
multilevel reduction of data storage and computational complexity, facilitates the realization of engineering
applications, and provides effective technical support and reasonable solutions for the solution of the
vehicle borne radar target accurate detection problem.</p>
    </sec>
    <sec id="sec-5">
      <title>6. References</title>
    </sec>
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