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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Vibration Region Extraction Method of Bridge Based on Ground- Based MIMO Radar 1</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Xiang Cao</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Xiangfei Nie</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Yunkai Deng</string-name>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Zhengquan Hu</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Fei Xiang</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Beijing Institute of Technology Chongqing Innovation Centre</institution>
          ,
          <addr-line>Chongqing, 401120</addr-line>
          ,
          <country country="CN">China</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>School of Electronic and Information Engineering, Chongqing Three Gorges University</institution>
          ,
          <addr-line>Chongqing, 404000</addr-line>
          ,
          <country country="CN">China</country>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>School of Information and Electronics, Beijing Institute of Technology</institution>
          ,
          <addr-line>Beijing, 100081</addr-line>
          ,
          <country country="CN">China</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>Ground-based multiple-input multiple-output (GB-MIMO) radar is suitable for vibration monitoring of all kinds of bridges because of its high accuracy, wide detection range and noncontact characteristics. It is necessary to select effective pixels with stable amplitude and regular phase to achieve accurate estimation of bridge vibration. In this paper, a new method for extracting vibration regions of bridges based on GB-MIMO radar is proposed. In the first step, the mask in image processing is combined with the average amplitude to extract the bridge pixels in the radar image and the circle fitting method is used to suppress the static clutter in the bridge pixel sequence. In the second step, the amplitude dispersion index is used to screen out the points with stable pixel amplitude. In the third step, the pixels with stable amplitude are divided into vibrational and non-vibrational regions by vibration similarity. Finally, the Welch method is used to analyze the phase spectrum of pixel sequence in the vibration region to estimate the vibration frequency. In order to verify the effectiveness of the proposed algorithm for bridge vibration detection, the measured data of a bridge in Chongqing is taken as an example to test the algorithm. The results show that the algorithm improves the effective detection rate of vibration region.</p>
      </abstract>
      <kwd-group>
        <kwd>eol&gt;GB-MIMO radar</kwd>
        <kwd>vibration area</kwd>
        <kwd>static echo suppression</kwd>
        <kwd>Frequency estimation</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>
        Various kinds of bridge structures are affected by dynamic loads such as moving vehicles, crowds
and earthquake during long-term use which will lead to fatigue damage or premature aging of local
bridge structures. If the damaged part of the bridge structure cannot be identified and repaired in time.
Over time, aging will accelerate further. It will lead to the accumulation of systemic damage of the
bridge structure and the attenuation of bridge resistance and even cause serious disasters such as
collapse, which poses a great threat to social property and people. Therefore, the research on bridge
health monitoring technology is of great significance to ensure the normal and safe operation of highway
bridges [
        <xref ref-type="bibr" rid="ref1">1-2</xref>
        ]. Vibration monitoring is an important method to evaluate the stability of bridge structure.
As an advanced non-contact sensor, real aperture radar has been widely used in structural health
monitoring. Its data acquisition speed is in the sub-millisecond level [
        <xref ref-type="bibr" rid="ref2">3</xref>
        ], but it has no azimuth resolution
ability. GB-MIMO radar has the ability of two-dimensional high-resolution imaging which can resolve
the vibration target in different directions on the same range gate and provides an effective technical
means for vibration measurement.
      </p>
      <p>
        Since the measurement of vibration by GB-MIMO radar needs to process and analyze the differential
interference phase sequence of pixels in time and frequency domain, the pixels of radar image affected
by noise are not suitable for vibration measurement. In order to achieve accurate estimation of bridge
vibration, effective pixels with stable amplitude and continuous phase need to be selected. In 1999,
amplitude dispersion index (ADI) was proposed to effectively screen out points with relatively stable
amplitude in pixel time series [
        <xref ref-type="bibr" rid="ref5">6</xref>
        ]. In 2007, the double threshold method of amplitude intensity and
amplitude deviation index was proposed to solve the problem of ignoring the strong scattering of the
target by the amplitude deviation method alone [
        <xref ref-type="bibr" rid="ref6">7</xref>
        ]. In 2019, Tian et al. [
        <xref ref-type="bibr" rid="ref7">8</xref>
        ] proposed the vibration
similarity index (VSI) according to the frequency angle of the vibration phase sequence to represent the
similarity between the phase sequence signal of the detected pixel and the ideal sinusoidal signal. The
pixels with continuous phase sequence are effectively screened but the stability of scattering
characteristics isn’t considered and the pixels with unstable amplitude are easily selected. This article
combines the characteristics of vibration pixels and phase sequences. The combination of ADI and VSI
is used to screen the effective pixels of bridge vibration.
      </p>
      <p>This paper is divided into five parts. The first part introduces the research background and content
of this paper. The second part analyzes the vibration measurement principle of GB-MIMO radar. The
third part describes the experimental methods. The fourth part discusses the test results of Chongqing
Bridge. The fifth part is the summary of this paper.</p>
    </sec>
    <sec id="sec-2">
      <title>2. Vibration measurement principle of GB-MIMO radar</title>
      <p>
        The realization of vibration target localization by GB-MIMO radar mainly depends on the
twodimensional high-resolution capability of GB-MIMO radar. A series of two-dimensional high resolution
radar images are generated by imaging the received signals [
        <xref ref-type="bibr" rid="ref8 ref9">9-10</xref>
        ]. The imaging results in an imaging
unit can be expressed as
j4π R
      </p>
      <p>I (m, n) = I (m, n) e λ</p>
      <p>Where, I (m, n) represents the imaging result after focusing at the position of grid (m, n) . I (m, n)
is the amplitude of the imaging result. R is the radial distance between the scatterer of (m, n) and the
radar.</p>
      <p>According to equation (1), the phase of the imaging result of each pixel contains the distance
information between the scatterer and radar in the scene corresponding to the pixel. For the vibration
target in the scene, the phase of the imaging result will show a certain periodicity along with the
vibration, so the phase curve of the multi-frame imaging result can be used for vibration analysis. After
extracting the signal of the same imaging unit from multiple consecutive imaging results, the signal
sequence of a vibrating object can be expressed as</p>
      <p>j4π Rvib j4π Avib sin(2πfvibkΔt)
I(m,n) (k ) = I(m,n) (k ) e λ e λ
(1)
(2)</p>
      <p>Where, I(m,n) (k ) is the signal of imaging unit (m, n) in the k th imaging results. Rvib is the radial
distance from the vibration center to the center of radar aperture. Δt is the time for collecting imaging
data of an image. Avib and fvib represent the vibration amplitude and frequency of the vibrating object,
respectively.</p>
    </sec>
    <sec id="sec-3">
      <title>3. The proposed method</title>
      <p>This paper is mainly divided into three parts: preprocessing, bridge vibration pixel extraction and
frequency estimation. Firstly, the radar image is preprocessed to extract the target region and suppress
the static echo of the vibration signal. Secondly, the vibration pixels of the bridge deck were screened
by combining ADI and VSI. Finally, the frequency of the selected pixel sequence is estimated. The
flow of the proposed method is shown in Fig. 1.</p>
      <p>
        Where, Ak is the amplitude value of a pixel in the kth radar image. According to experience, the
threshold can be set to -10dB [
        <xref ref-type="bibr" rid="ref12">13</xref>
        ].
      </p>
      <p>
        Finally, according to the characteristics that the stationary target echo does not change with time
while the vibration echo phase changes periodically with time, the circular fitting method [
        <xref ref-type="bibr" rid="ref10">11</xref>
        ] is used
to suppress the stationary clutter of the target candidate pixel sequence.
      </p>
    </sec>
    <sec id="sec-4">
      <title>3.2. Select bridge deck pixels</title>
      <p>
        After preprocessing, the approximate range of bridge pixels is filtered out. Because the bridge is an
artificial structure the surface is relatively smooth. The scattering intensity of each structure location is
inconsistent and unpredictable. So, it is necessary to determine the pixels with high SNR when selecting
the effective pixels. ADI is based on the statistical characteristics of pixel amplitude on the time series
to select the point of amplitude stability. For a pixel with a high SNR, the noise level of its phase is
equivalent to the amplitude dispersion index [
        <xref ref-type="bibr" rid="ref5">6</xref>
        ]. Therefore, the ADI method can effectively screen out
the pixels with stable bridge amplitude by setting an appropriate threshold. The expression is as follows:
      </p>
    </sec>
    <sec id="sec-5">
      <title>3.1. Preprocessing</title>
      <p>The purpose of preprocessing is to extract target region from radar image region and suppress clutter.
The first step is to extract the target region by using the mask in image segmentation according to the
observed scene image. The second step is based on the strong scattering characteristics of the target
echo signal, which is characterized by high energy and large amplitude of the echo signal. The average
amplitude threshold method is used to detect the target region. The pixel with high amplitude is selected
as the target candidate point by setting an appropriate threshold. The expression is as follows:
DA =σmAA
(3)
(4)</p>
      <p>
        In equation (3), σ A and mA are the amplitude standard deviation and amplitude average value of N
radar images in the temporal dimension. DA is the dispersion index. Empirically, the threshold can be
set to 0.15 [
        <xref ref-type="bibr" rid="ref11">12</xref>
        ].
      </p>
    </sec>
    <sec id="sec-6">
      <title>3.3. Select vibrating pixels</title>
      <p>
        The bridge amplitude stable pixels selected by ADI can be directly used for deformation monitoring
because the bridge deforms very slowly. In order to realize vibration monitoring of bridge, it is
necessary to select pixels with regular phase. Vibration Similarity Index (VSI) [
        <xref ref-type="bibr" rid="ref10 ref7 ref8 ref9">8-11</xref>
        ] can represent the
Similarity between phase sequence signal and ideal sinusoidal signal. When the VSI is larger, the
Vibration amplitude is larger. The expression is as follows:
      </p>
      <p>
        Where, Smax and Smean represent the peak amplitude of the spectrum after removing the DC
component and the average amplitude of the whole spectrum, respectively. By setting an appropriate
threshold VSIT , the pixel meeting condition VSI &gt; VSIT is the vibration pixel. When choosing VSIT ,
first determine the number of sampling points and the required detection probability. The detection rate
is the probability that the highest value in the spectrum except the zero-frequency point corresponds to
the vibration frequency. Then the requirement of SNR is obtained according to the required detection
probability. Finally, we find the corresponding VSIT [
        <xref ref-type="bibr" rid="ref7">8</xref>
        ].
      </p>
      <p>Finally, the common pixels of (4) and (5) are obtained. Since the vibration pixels of the structure are
not isolated in the image domain, the isolated pixels are removed by the filtering operation in binary
morphology.</p>
    </sec>
    <sec id="sec-7">
      <title>3.4. Frequency estimation</title>
      <p>
        As shown in Equation (2), the phase of the extracted signal includes the vibration of the vibrating
object. Therefore, Welch method [
        <xref ref-type="bibr" rid="ref15">16</xref>
        ] can be used to estimate the vibration frequency according to the
phase of the signal sequence. The expression is as follows:
      </p>
      <p>P=
1 L N</p>
      <p>  xi (n)ω (n) exp (− jω n)
L i=1 n=1
2</p>
      <p>Where xi represents the ith data segment with N elements, L is the segment number, ω (n) is the
window function. The position of the spectral peak corresponds to the estimated vibration frequency.</p>
    </sec>
    <sec id="sec-8">
      <title>4. Bridge vibration experiment</title>
    </sec>
    <sec id="sec-9">
      <title>4.1. Experimental information</title>
      <p>A bridge in Chongqing was monitored by 16 ×16 GB-MIMO radar in the experiment. System
parameters are shown in Table 1, and experimental scenes are shown in Fig 2</p>
      <p>(a) Monitoring scene diagram
Fig. 2 Monitoring scene and MIMO radar imaging results
(b) Imaging results</p>
      <sec id="sec-9-1">
        <title>Parameter</title>
      </sec>
      <sec id="sec-9-2">
        <title>Central Frequency</title>
      </sec>
      <sec id="sec-9-3">
        <title>Range Resolution PRT</title>
      </sec>
      <sec id="sec-9-4">
        <title>Measurement Range</title>
        <p>Value
16.2 GHz
0.375 m
0.082 ms
50-500 m
(5)
(6)</p>
      </sec>
    </sec>
    <sec id="sec-10">
      <title>4.2. Experimental results</title>
      <p>A. Preprocessing: As mentioned in 3.1, Fig. 3 (a) plots the target area extracted by artificial mask
in image processing. The entire bridge shape can be clearly seen from the target area. According to (3),
the bridge pixels with large amplitude in the target area are screened out, as shown in Fig. 3 (b). Then
the candidate pixels are suppressed by circle fitting. Firstly, the trajectory of the bridge pixel sequence
is fitted to the complex plane to obtain the center of the circle and the center of the circle is moved back
to the origin of coordinates, as shown in Fig. 3 (c). Fig. 3 (d) shows the pixel distribution after clutter
suppression.</p>
      <p>1
0.5
0
-0.5
-1
-1.5
-2
(a) Target area</p>
      <p>(b) Distribution of candidate pixels
Beforeclut ersuppression</p>
      <p>After clut er suppression</p>
      <p>B. Select bridge deck pixels: The local graph of ADI value according to (4) is shown in Fig. 4 (a)
after preprocessing. Some of the stronger amplitude pixels on the bridge have poorer ADI values due
to dihedral Angle scattering and dwell. Fig.4 (b) shows the distribution of bridge deck pixels after
screening by setting ADI threshold.</p>
      <p>(d) Distribution after clutter suppression
(a) Local graph of ADI value
Fig. 4 The rule of ADI
(b) Pixel distribution of bridge deck</p>
      <p>
        C. Select vibrating pixels: According to equation (5), the preprocessed pixel sequence is taken as
the input to calculate the VSI then setting an appropriate threshold according to experience [
        <xref ref-type="bibr" rid="ref7">8</xref>
        ] to select
the vibration pixels. Fig. 5 (a) shows the distribution of the vibration pixels. A total of 52302 vibrating
pixels were selected. As the bridge body is a whole, its deformation in the same period should be regular
[
        <xref ref-type="bibr" rid="ref13">14</xref>
        ]. The phase sequence of the selected pixels is used for deformation estimation [
        <xref ref-type="bibr" rid="ref14">15</xref>
        ]. Fig. 4 (b) shows
the deformation curve of the selected pixels. The deformation of the bridge body is disorderly. This is
because the selected vibration pixels of the bridge body include the vibration pixels outside the bridge
body. Therefore, it is necessary to screen the bridge structure pixels (pixels with stable amplitude)
before screening the vibration pixels.
      </p>
      <p>(a) Distribution of vibration pixel
Fig. 5 VSI selection result
(b) Deformation curve</p>
      <p>Finally, the pixels common to the bridge deck pixels and vibration pixels are defined as effective
pixels, a total of 12587 pixels. Then, the isolated pixels are removed through binary morphology
filtering operation, and a total of 12132 pixels are selected, as shown in Fig. 6 (a). Fig. 6 (b) shows the
deformation curve of the effective pixel. The deformation changes of selected pixels are basically the
same. Therefore, this method can effectively screen the vibrating pixels of the bridge deck.
(a) Effective pixel distribution
Fig. 6 Results of the proposed method selection
(b)</p>
      <sec id="sec-10-1">
        <title>Deformation curve</title>
        <p>
          D. Frequency estimation: Fig. 7(a) depicts the phase curve of a vibrating pixel in the vibration area
of the bridge. According to Section 3.4, the vibration frequency of the vibrating pixel is estimated to be
0.34Hz, as shown in Fig. 7(b). According to the data, the natural frequency of the first order vibration
of long-span cable-stayed bridge is about 0.2~0.5Hz [
          <xref ref-type="bibr" rid="ref16">17</xref>
          ]. So, it is considered that the result is reliable.
        </p>
        <p>(a) Vibration phase curve of vibrating pixels</p>
        <p>Finally, the vibration frequencies of the bridge vibration regions selected by the double threshold
method and the bridge vibration regions selected by the VSI method are estimated respectively. Fig 8
(a) is the first-order frequency distribution of the proposed method and Fig 8 (b) is the first-order
frequency distribution of the VSI method.</p>
        <p>1 2 frequency/3Hz 4 5
(b) Spectrum diagram of vibration phase curve
(a) First order vibration frequency distribution
diagram (The proposed method)
(b) First order vibration frequency distribution
diagram (VSI method)</p>
        <p>In order to further compare the vibration region recognition effects of the two methods, the vibration
frequencies in Fig. 8(a) and Fig. 8(b) were statistically analyzed. The results are shown in Table 2. The
frequencies of pixels selected by the two methods are all concentrated at 0.34Hz. The pixels with a
frequency of 0.34Hz selected by the proposed method accounted for 75.3% of the total selected structure
pixels, which was larger than that of the VSI method. Therefore, the detection rate of bridge vibration
region is higher with the proposed method.</p>
      </sec>
    </sec>
    <sec id="sec-11">
      <title>5. Conclusion</title>
      <sec id="sec-11-1">
        <title>Measured pixels 9136 18363</title>
        <p>Vibration
frequency</p>
        <p>In the bridge vibration measurement technology, in order to ensure the accuracy and reliability of
the bridge vibration estimation, the bridge vibration region with stable amplitude and regular phase is
selected. This article uses the stability characteristics of deck amplitude in time series and the energy
distribution characteristics of vibration phase sequence spectrum. A method combining amplitude
dispersion index and vibration similarity index is proposed, which can effectively improve the detection
rate of bridge vibration region based on GB-MIMO radar. In the experiment, GB-MIMO radar is used
to observe a bridge in Chongqing and obtain multiple radar image data continuously. The vibration
region of radar image is selected by using the vibration similarity index method and the improved
method. Finally, the frequency of selected vibration region is estimated by spectrum analysis principle.
The experimental results show that the proposed method can effectively improve the detection rate of
bridge vibration region.</p>
      </sec>
    </sec>
    <sec id="sec-12">
      <title>6.Acknowledgments</title>
    </sec>
    <sec id="sec-13">
      <title>7.References</title>
      <p>This work was supported by the National Natural Science Foundation of China (619701037); Youth
project of science and technology research program of Chongqing Education Commission of China.
(Grant No. KJQN202101226).
[1] T. Pa, A. Ja, D. Ga, et al. "Remote Structural Health Monitoring System for Bridges", 2020 IEEE
International Students' Conference on Electrical, Electronics and Computer Science (SCEECS),
2020, pp. 1-4.</p>
    </sec>
  </body>
  <back>
    <ref-list>
      <ref id="ref1">
        <mixed-citation>
          [2]
          <string-name>
            <given-names>R.</given-names>
            <surname>Li</surname>
          </string-name>
          ,
          <string-name>
            <given-names>T.</given-names>
            <surname>Mo</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Yang</surname>
          </string-name>
          , et al.
          <article-title>"Ontologies-Based Domain Knowledge Modeling and Heterogeneous Sensor Data Integration for Bridge Health Monitoring Systems"</article-title>
          ,
          <source>in IEEE Transactions on Industrial Informatics</source>
          ,
          <year>2021</year>
          , vol.
          <volume>17</volume>
          , no.
          <issue>1</issue>
          , pp.
          <fpage>321</fpage>
          -
          <lpage>332</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref2">
        <mixed-citation>
          [3]
          <string-name>
            <given-names>Y.</given-names>
            <surname>Zhu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>B.</given-names>
            <surname>Xu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Z.</given-names>
            <surname>Li</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Hou</surname>
          </string-name>
          , et al.
          <article-title>"Monitoring Bridge Vibrations Based on GBSAR and Validation by High-Rate GPS Measurements"</article-title>
          ,
          <source>in IEEE Journal of Selected Topics in Applied Earth Observations and Remote Sensing</source>
          ,
          <year>2021</year>
          , vol.
          <volume>14</volume>
          , pp.
          <fpage>5572</fpage>
          -
          <lpage>5580</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref3">
        <mixed-citation>
          [4]
          <string-name>
            <given-names>A.</given-names>
            <surname>Zong</surname>
          </string-name>
          .
          <article-title>"Research on Radar MTI/MTD clutter suppression"</article-title>
          , Hubei University,
          <year>2012</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref4">
        <mixed-citation>
          [5]
          <string-name>
            <given-names>K.</given-names>
            <surname>Kulpa</surname>
          </string-name>
          ,
          <string-name>
            <given-names>B.</given-names>
            <surname>Dawidowicz</surname>
          </string-name>
          ,
          <string-name>
            <given-names>L.</given-names>
            <surname>Maslikowski</surname>
          </string-name>
          , et al.
          <article-title>"Single channel clutter cancelation in mobile PCL"</article-title>
          ,
          <year>2018</year>
          22nd
          <string-name>
            <given-names>International</given-names>
            <surname>Microwave</surname>
          </string-name>
          and Radar Conference (MIKON),
          <year>2018</year>
          , pp.
          <fpage>593</fpage>
          -
          <lpage>594</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref5">
        <mixed-citation>
          [6]
          <string-name>
            <given-names>C. R.</given-names>
            <surname>Farrar</surname>
          </string-name>
          ,
          <string-name>
            <given-names>T. W.</given-names>
            <surname>Darling</surname>
          </string-name>
          ,
          <string-name>
            <given-names>A.</given-names>
            <surname>Migliori</surname>
          </string-name>
          , and
          <string-name>
            <given-names>W. E.</given-names>
            <surname>Baker</surname>
          </string-name>
          , “
          <article-title>Microwave interferometers for noncontact vibration measurements on large struc-tures”</article-title>
          ,
          <source>Mech. Syst. Signal Process</source>
          .
          <year>1999</year>
          , vol.
          <volume>13</volume>
          , no.
          <issue>2</issue>
          , pp.
          <fpage>241</fpage>
          -
          <lpage>253</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref6">
        <mixed-citation>
          [7]
          <string-name>
            <given-names>X.</given-names>
            <surname>Luo</surname>
          </string-name>
          ,
          <string-name>
            <given-names>D.</given-names>
            <surname>Huang</surname>
          </string-name>
          ,
          <string-name>
            <given-names>G.</given-names>
            <surname>Liu</surname>
          </string-name>
          , et al.
          <article-title>"Automatic detection of permanent scatterers in time serial differential radar interference"</article-title>
          ,
          <source>Journal of Southwest</source>
          Jiaotong University,
          <year>2007</year>
          , vol.
          <volume>42</volume>
          , no.
          <issue>4</issue>
          , pp:
          <fpage>414</fpage>
          -
          <lpage>418</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref7">
        <mixed-citation>
          [8]
          <string-name>
            <given-names>W.</given-names>
            <surname>Tian</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y.</given-names>
            <surname>Li</surname>
          </string-name>
          ,
          <string-name>
            <given-names>C.</given-names>
            <surname>Hu</surname>
          </string-name>
          , et al.
          <article-title>"Vibration Measurement Method for Artificial Structure Based on MIMO Imaging Radar"</article-title>
          ,
          <source>in IEEE Transactions on Aerospace and Electronic Systems</source>
          ,
          <year>2020</year>
          , vol.
          <volume>56</volume>
          , no.
          <issue>1</issue>
          , pp.
          <fpage>748</fpage>
          -
          <lpage>760</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref8">
        <mixed-citation>
          [9]
          <string-name>
            <given-names>A.</given-names>
            <surname>Boag</surname>
          </string-name>
          .
          <article-title>"A fast multilevel domain decomposition algorithm for radarimaging"</article-title>
          ,
          <source>IEEE Trans. Antennas Propag</source>
          ,
          <year>2001</year>
          , vol.
          <volume>49</volume>
          , no.
          <issue>4</issue>
          , pp:
          <fpage>666</fpage>
          -
          <lpage>671</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref9">
        <mixed-citation>
          [10]
          <string-name>
            <given-names>H.</given-names>
            <surname>Mei</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y.</given-names>
            <surname>Li</surname>
          </string-name>
          ,
          <string-name>
            <given-names>W.</given-names>
            <surname>Tian</surname>
          </string-name>
          et al.
          <source>"Weak Vibration Measurement Based on MIMO Imaging Radar System," 2018 China International SAR Symposium (CISS)</source>
          ,
          <year>2018</year>
          , pp:
          <fpage>1</fpage>
          -
          <lpage>5</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref10">
        <mixed-citation>
          [11]
          <string-name>
            <given-names>P.</given-names>
            <surname>Wang</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y.</given-names>
            <surname>Xu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>J.</given-names>
            <surname>Xu</surname>
          </string-name>
          , et al.
          <article-title>"Study on removal method of static clutter from deformation monitoring signal of ground-based interference radar"</article-title>
          ,
          <source>Bulletin of Surveying and Imageping</source>
          ,
          <year>2014</year>
          , no.
          <issue>10</issue>
          , pp:
          <fpage>15</fpage>
          -
          <lpage>18</lpage>
          +
          <fpage>40</fpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref11">
        <mixed-citation>
          [12]
          <string-name>
            <given-names>C.</given-names>
            <surname>Hu</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y.</given-names>
            <surname>Deng</surname>
          </string-name>
          ,
          <string-name>
            <given-names>W.</given-names>
            <surname>Tian</surname>
          </string-name>
          , and
          <string-name>
            <given-names>J.</given-names>
            <surname>Wang</surname>
          </string-name>
          .
          <article-title>“A PS processing framework for long-term and real-time GB-SAR monitoring”</article-title>
          ,
          <source>Int. J. Remote Sens</source>
          . vol.
          <volume>40</volume>
          , no.
          <issue>16</issue>
          , pp.
          <fpage>6298</fpage>
          -
          <lpage>6314</lpage>
          , Mar.
          <year>2019</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref12">
        <mixed-citation>
          [13]
          <string-name>
            <given-names>M.</given-names>
            <surname>Zhu</surname>
          </string-name>
          .
          <article-title>"High Precision Deformation Measurement Using Ground Based Synthetic Aperture Radar (GBSAR) Based on Dynamic Persistent Scatterer (PS) Technique"</article-title>
          , Beijing Institute of Technology,
          <year>2016</year>
          .
        </mixed-citation>
      </ref>
      <ref id="ref13">
        <mixed-citation>
          [14]
          <string-name>
            <given-names>Z.</given-names>
            <surname>Zhao</surname>
          </string-name>
          ,
          <string-name>
            <given-names>F.</given-names>
            <surname>Jiang</surname>
          </string-name>
          ,
          <string-name>
            <given-names>G.</given-names>
            <surname>Yin</surname>
          </string-name>
          .
          <article-title>"Brief Discussion on the Causes and Observation Methods of Bridge Deformation"</article-title>
          , Forest Engineering,
          <year>1999</year>
          , no.
          <issue>01</issue>
          , pp:
          <fpage>52</fpage>
          -
          <lpage>53</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref14">
        <mixed-citation>
          [15]
          <string-name>
            <given-names>Y.</given-names>
            <surname>Jia</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Z.</given-names>
            <surname>Gao</surname>
          </string-name>
          ,
          <string-name>
            <given-names>S.</given-names>
            <surname>Liu</surname>
          </string-name>
          , et al.
          <article-title>"Application of FMCW MMW radar in dynamic deflection monitoring of high⁃speed railway bridge"</article-title>
          ,
          <source>Modern Electronics Technique</source>
          ,
          <year>2022</year>
          , vol.
          <volume>45</volume>
          , no.
          <issue>15</issue>
          , pp:
          <fpage>15</fpage>
          -
          <lpage>19</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref15">
        <mixed-citation>
          [16]
          <string-name>
            <given-names>W.</given-names>
            <surname>Pan</surname>
          </string-name>
          ,
          <string-name>
            <given-names>L.</given-names>
            <surname>Wang</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y.</given-names>
            <surname>Song</surname>
          </string-name>
          .
          <article-title>"Recognition of Double- curvature Arch Bridge Natural Frequency Detection Signal Using Welch Power Spectrum Estimation"</article-title>
          ,
          <source>Industrial Control Computer</source>
          ,
          <year>2006</year>
          , vol.
          <volume>19</volume>
          , no.
          <issue>11</issue>
          , pp:
          <fpage>22</fpage>
          -
          <lpage>23</lpage>
          .
        </mixed-citation>
      </ref>
      <ref id="ref16">
        <mixed-citation>
          [17]
          <string-name>
            <given-names>B.</given-names>
            <surname>Xiang</surname>
          </string-name>
          ,
          <string-name>
            <given-names>Y. Zhou. X.</given-names>
            <surname>Chen</surname>
          </string-name>
          .
          <article-title>"Study on Dynamic Characteristics Monitoring System of Dongshuimen Yangtze River Bridge"</article-title>
          ,
          <source>Western Transportation Technology</source>
          ,
          <year>2015</year>
          , no.
          <issue>11</issue>
          , pp:
          <fpage>46</fpage>
          -
          <lpage>50</lpage>
          .
        </mixed-citation>
      </ref>
    </ref-list>
  </back>
</article>