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  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>3d synthetic aperture radar image</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>A N Leukhin</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>A A Rozentsov</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>V I Bezrodnyy</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>A A Voronin</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>D Yu Karasev</string-name>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>N A Kokovihina</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Mari State University</institution>
          ,
          <addr-line>Lenin square 1, Yoskar-Ola, Russia, 424000</addr-line>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Volga State University of Technology</institution>
          ,
          <addr-line>Lenin square 3, Yoskar-Ola, Russia, 424000</addr-line>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2018</year>
      </pub-date>
      <fpage>330</fpage>
      <lpage>335</lpage>
      <abstract>
        <p>Synthetic aperture radar (SAR) is a coherent active microwave imaging method. In remote sensing it is used for mapping the scattering properties of the Earth's surface in the respective wavelength domain. The algorithms for the formation of 3D radar images in multiposition interferometric systems for remote sensing of the Earth are considered. Examples of reconstruction of the relief map for systems with one and two transmit antenna are presented.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>2. “Two transmitters, two receivers” system</title>
      <p>Figure 1 shows the basic geometric equations for the 3D SAR system, for the case when the aircraft is
equipped with two transmitter and two receivers, operating through its own spaced from each other
antenna.</p>
      <p>
        Using the basis of the Pythagorean theorem we can write:
(H1  h)2  r12  R12
 2
(H2  h)2  (r1  d )2  R2
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
      </p>
      <p>
        Values of the heights H1 and H 2 of the antennas and antenna spacing d in the horizontal plane
can be considered known while SAR is working. Also known and sloped range R1 and R2 . You need
to find the horizontal distance r1 and the height of the object h . Before solving the equation (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) we can
first calculate r1 and then determine h or vice versa. The solution to the system is determined by the
ratio between the values d and H1  H 2 . If H1  H2  d you choose the first method, otherwise
the second. Two solutions are obtained when you use each method. A preference in favor of a solution
that gives value r1 least different from the values of the horizontal range, designed for zero height
r(0)  (R12  H 2 )1/ 2 , i.e. r1  r1(0)  min [3].
1 1
      </p>
      <p> H1 R12  H1 R22  H 2  R12  H 2  R22  d 
 (H12  2  H1 H 2  H 22  R12  2  R1 R2  R22  d 2 )1/ 2 
 (2  H1 H 2  H12  H 22  R12  2  R1 R2  R22  d 2 )1/ 2 ) 
r  
</p>
      <p>1
2  (H12  2  H1 H 2  H 22  d 2 ) ;
R12  R22  d 2  (H 2  h)2  (H1  h)2</p>
      <p>2  d</p>
      <p>
        On the practice ranges R1 and R2 are known with an item resolution accuracy, so the calculations
of value h and r1 use value R  R2  R1 , calculated on the basis of the measurement result of the
phase difference
R   (w)    2 1  , (
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
      </p>
      <p>4 4
where 1 and  2 - phases of the signals received from the first and second antennas, respectively; 
wave`s length.</p>
      <p>Because the value of the phase shift is in the range [0,2 ) , as a rule, there is ambiguity of the
measurement values R . To fix it uses the "unwrap" phase. Consider possible approaches to its
implementation [4].</p>
      <p>The first approach is based on the preliminary construction of the dependence of phase shifts to the
zero level, depending on slant range to the antenna A1 [5]:</p>
      <p>
         0R1   4R0R1 /  4 ((H22  ((R12  H12 )1/ 2  d )2 )1/ 2  R1) /
Then the value of the phase shift  uR1 used to calculate the difference between the sloping
distances, determined from the relationship:
 uR1    w  trunc  0R1  2 (
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
      </p>
      <p> 2 
The value of the slant range R2 used for the calculation h and r1 is determined from the relation:
 u
R2  R1 </p>
      <p>  2m
4</p>
      <p>To determine the value m , you can use the following approach. Typically, the height difference
between adjacent pixels is relatively small and we can assume that the height of the object in some
neighborhood is constant. Presented according to m estimates of the altitude differences in the
neighboring pixels have a pronounced minimum, and calculations show that this minimum is achieved
when the value of the parameter mˆ corresponding to the true values of the altitude and slant range.
The algorithm of the calculation value mˆ is the following:
1. Around the current image point with coordinates x0 , y0 , set the gate;
2. Sets the range of values m : m  mmin...mmax
3. For each point in the gate with coordinates x , y , a values rx, y and hx, y are calculated with
current value m ;
4. Calculate total measurement error of the heights and horizontal distances. Terms y1  y0  and
y2  y0  take into account the current offset of pixels in the horizontal range:
hm 
rm 
x0dx y0dy x0dx y0dy</p>
      <p>   
x1x0dx y1 y0dy x2x0dx y2 y0dy
x0dx y0dy x0dx y0dy</p>
      <p>    yx1,x2,y1,y2
x1x0dx y1 y0dy x2x0dx y2 y0dy
yx1,x2,y1,y2  rx1,y1  y1  y0  rx2,y2  y2  y0 
hx1,y1  hx2,y2</p>
      <sec id="sec-1-1">
        <title>5. As a result, selects the value mˆ at which</title>
        <p>hmˆ  min , кmˆ  min (9)</p>
        <p>
          Because of spacing antennas, the resulting images have some mutual shift, and its magnitude will
depend on the range. In this regard, before calculating the elevation, you must perform the mutual
correction of the shifts of image elements. For this calculate values of distances R2 corresponding to
(
          <xref ref-type="bibr" rid="ref5">5</xref>
          )
(
          <xref ref-type="bibr" rid="ref7">7</xref>
          )
(8)
the range R1 on the zero level and overwrite the elements of the second array with the ranges R2 in
cells that correspond to values in the range R1 [6]:
        </p>
        <p>J Rк1о,рx  J 2</p>
        <p>R2 ,x
R2  (H22  ((R12  H12 )1/ 2  d )2 )1/ 2
(10)
where J 2</p>
        <p>R2,x - image from the second antenna.</p>
        <p>
S2  S1  m, m  ...,2,1,0,1,2,... (11)</p>
        <p>2</p>
        <p>Knowing the values of the parameters S1 , S2 , H1 , H 2 , d , you can find value and a horizontal
range r1 :</p>
        <p>D2  (d 2  (d 2  S12  2  H12  S 22  2  H 22  S 22  2  S1 d 2  S 2  S 24  H 22  S12 
 4  H13  H 2  2  d 2  S 22  H12  S12  d 4  2  H 22  d 2  H14  H 24  2  H12  d 2 
 6  H12  H 22  2  S1 S 2  H12  2  S1 S 23  4  H1 H 2  d 2  4  H1 H 23  4  H1 H 2  S12 </p>
        <p> 4  H1 H 2  S1 S 2  2  H 22  S1 S 2  4  H1 H 2  S 22  S12  S 22 ))0.5
h 
 H1 S1 S 2  H 2  d 2  H12  H 2  H13  H 23  H1 d 2  H 2  S 22 </p>
        <p>2  (H12  H 22  d 2  2  H1 H 2)
 H1 S 22  H 2  S1 S 2  H1 H 22  D2</p>
        <p>2  (H12  H 22  d 2  2  H1 H 2)
As in the first case, measuring the phase shift may be ambiguous. The dependence of phase shifts on
the zero level from the slant range to the antenna A1 is described by the expression:
 0R1  2
(H22  ((R12  H12 )1/ 2  d )2 )1/ 2  R1
</p>
        <p>
          Then the value of the phase shift  uR1 is used to calculate the difference between the sloping
distances is determined from the equation (
          <xref ref-type="bibr" rid="ref6">6</xref>
          ). Path S2 is used for the calculation h and r1 is
determined from the expression:
        </p>
        <p>S2  2R1 
 u  2m
2
</p>
      </sec>
      <sec id="sec-1-2">
        <title>The value m is chosen by the equation (9).</title>
        <p>Still from the spacing antennas, the elements of the resulting images can have some mutual shift.
To compensate for this shift is necessary to perform the image correction according to the relation [7]:
J Rк1о,рx  J R21R2 ,x (15)</p>
        <p>2 ,
where R2 is computed as in equation (10).</p>
        <p>Figure 4 shows an example of the recovery bump maps for the considered case when the following
system parameters H1  H2  10m , d  5m the maximum altitude of the relief 5m.
(12)
(13)
(14)</p>
      </sec>
    </sec>
    <sec id="sec-2">
      <title>4. Conclusions</title>
      <p>Solution of a problem of restoration of a landscape`s in a synthetic aperture radar at various
configuration of a reception-transmitting path is considered in this work. An original phase
unwrapping algorithm based on joint minimization of the estimating error of object`s height and
sloped range in neighboring pixels of the image is proposed. Examples of the restored 3D images are
presented.</p>
    </sec>
    <sec id="sec-3">
      <title>Acknowledgments</title>
      <p>The work is executed at financial support of the Ministry of Education and Science of the Russian
Federation, project No. 2.2226.2017/Project Part and project No. 2.9140.2017/Basic Part. The work is
performed under financial support of Russian Found of Basic Research, research project No.
15-0799514.</p>
    </sec>
  </body>
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