<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OPJ</journal-id><journal-title-group><journal-title>Optics and Photonics Journal</journal-title></journal-title-group><issn pub-type="epub">2160-8881</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/opj.2016.68B005</article-id><article-id pub-id-type="publisher-id">OPJ-70295</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Study of Full-Size Objects’ Bistatic Rader Cross Section Measurement Based on Photoelectric Conversion
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yilong</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Tao</surname><given-names>Hong</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhihua</surname><given-names>Chen</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>59th Research Institute of China Ordnance Industry, Chongqing, China</addr-line></aff><aff id="aff1"><addr-line>College of Electronic and Information Engineering, Beijing University of Aeronautics and Astronautics, 
Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>25</day><month>08</month><year>2016</year></pub-date><volume>06</volume><issue>08</issue><fpage>24</fpage><lpage>29</lpage><history><date date-type="received"><day>22</day>	<month>April</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>19</month>	<year>August</year>	</date><date date-type="accepted"><day>25</day>	<month>August</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   
   In the past years, bistatic Radar Cross Section (RCS) characteristic has been caught increasing attention. The paper presents a bistatic RCS measurement system of full-size goals, which uses photoelectric conversion technology to solve the problem that excessive electrical signal attenuation exits because of the large distance between sending and receiving antenna. The paper analyzes the basic principle of photoelectric conversion and RCS measurement system, applies photoelectric conversion technology to RCS measurement system, and tests whether RCS measurement system works well while using photoelectric conversion technology. The test results show that the system can efficiently obtain the bistatic RCS characteristic of full-size targets. 
  
 
</p></abstract><kwd-group><kwd>Full-Size Targets</kwd><kwd> Bistatic RCS Characteristic</kwd><kwd> Photoelectric Conversion Technology</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The main purpose of stealth technology is to reduce the Radar Cross Section of target. Today, RCS measurement can be divided into Near-field, Outdoor-field measurement, as well as single and double station measurement. Near-field measurement as an advanced measurement technology has been widely used in radiation scattering measurements and radar target imaging. Without requiring a huge outdoor testing field, Near-field measurement can acquire a large amount of information, high precision and small interference by outside, good privacy. In addition, Near-field measurement can work around the clock and have a series of advantages such as diagnostic function [<xref ref-type="bibr" rid="scirp.70295-ref1">1</xref>]. Compared with the Near-field measurement, the main features of Outdoor-field measurement are: size of the object can be within a wide range; the measurement results are closer to the real situation of the target; Far-field measurement condition is easy to satisfy, and can be directly used for the acceptance of products’ electromagnetic scattering properties [<xref ref-type="bibr" rid="scirp.70295-ref2">2</xref>]. Because of the advantages of Outdoor-field measurement, it is now at home and abroad to build a lot of Outdoor test field, such as the US RATSCAT [<xref ref-type="bibr" rid="scirp.70295-ref3">3</xref>], Range 8, UK Underwood Quarry, etc. with the development of bi/multi-static radar system [<xref ref-type="bibr" rid="scirp.70295-ref4">4</xref>] and radar detection of hypersonic target in Near Space [<xref ref-type="bibr" rid="scirp.70295-ref5">5</xref>].</p><p>Bistatic RCS measurement has been gradually developing at home and abroad. Compared to traditional single-station RCS measurements, bistatic RCS measurement can simulate multi-base anti-stealth system to measure the measured target stealth performance at different pitch angle, which reflects the targets’ actual stealth performance. Thus, the bistatic RCS measurement systems have sprung up in recent years, which have been applied in the Near field and Outdoor games, and developed rapidly.</p><p>Today, the bistatic RCS anti-stealth is applied to an increasing number of occasions, for example, 52E6MU Struna-1MU/Barrier E (NNIIRT, Russia) is the proposed multistatic system that can detect against low RCS targets [<xref ref-type="bibr" rid="scirp.70295-ref6">6</xref>].</p></sec><sec id="s2"><title>2. Bistatic RCS Testing System</title><p><xref ref-type="fig" rid="fig1">Figure 1</xref> is a schematic diagram of the RCS linear sweep system [<xref ref-type="bibr" rid="scirp.70295-ref7">7</xref>], RF signal source emits a sweep wave signal. After coupling, the signal is divided into two signals, one of which is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x4.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.70295-formula213"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x5.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula214"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x6.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x7.png" xlink:type="simple"/></inline-formula>is the bandwidth of the sweep, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x8.png" xlink:type="simple"/></inline-formula>is scan time, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x9.png" xlink:type="simple"/></inline-formula>is the initial phase, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x10.png" xlink:type="simple"/></inline-formula>is the signal amplitude. The remaining signal after amplification is transmitted out by the transmitting antenna.</p><p>One signal is received by the receiving antenna, enlarged by LNA, and become echo signal. R is the distance from the measured target to the receiving antenna, which causes time delay <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x11.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.70295-formula215"><graphic  xlink:href="http://html.scirp.org/file/70295x12.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula216"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x13.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula217"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x14.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x15.png" xlink:type="simple"/></inline-formula>is Echo signal, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x16.png" xlink:type="simple"/></inline-formula>is the phase shift by target scattering, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x17.png" xlink:type="simple"/></inline-formula>is the attenuated signal amplitude. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x18.png" xlink:type="simple"/></inline-formula>is IF signal obtained after mixing. A is amplitude of the IF signal. By processing the IF signal, we can get the measured target’s one-dimensional, two-dimensional, and even three-dimensional image.</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Schematic diagram of the RCS linear sweep system</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70295x19.png"/></fig></sec><sec id="s3"><title>3. Photoelectric Conversion System</title><sec id="s3_1"><title>3.1. Theory</title><p><xref ref-type="fig" rid="fig2">Figure 2</xref> is a process of the photoelectric conversion, the modulation mode is AM modulation. Firstly, unmodulated signal can be modulated by laser source, and become modulated optical signal [<xref ref-type="bibr" rid="scirp.70295-ref8">8</xref>]. Then, the signal is transmitted to photo detector, demodulated and filtered. Finally, we can get the initial electric signal [<xref ref-type="bibr" rid="scirp.70295-ref9">9</xref>].</p><disp-formula id="scirp.70295-formula218"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x20.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula219"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x21.png"  xlink:type="simple"/></disp-formula><p>Laser source is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula>, unmodulated signal is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x24.png" xlink:type="simple"/></inline-formula>is the amplitude of the modulated signal, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x25.png" xlink:type="simple"/></inline-formula>is the frequency of the modulated signal, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x26.png" xlink:type="simple"/></inline-formula>is the amplitude of the modulated signal, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x27.png" xlink:type="simple"/></inline-formula>is the frequency of the modulated signal, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x28.png" xlink:type="simple"/></inline-formula>is initial phase. Modulated optical signal is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x29.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.70295-formula220"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x30.png"  xlink:type="simple"/></disp-formula><p>The process of demodulation:</p><disp-formula id="scirp.70295-formula221"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x31.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula222"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x32.png"  xlink:type="simple"/></disp-formula><p>Finally, optical signal becomes electric signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x33.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.70295-formula223"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x34.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2"><title>3.2. Applied to RCS</title><p><xref ref-type="fig" rid="fig3">Figure 3</xref> shows the processthat the receiving anttena’s signal transports back to the processor by photoelectric conversion systerm. Electrical signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x35.png" xlink:type="simple"/></inline-formula>, after modulated by the optical modulator, becomes the light signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x36.png" xlink:type="simple"/></inline-formula>. Transported by optical fiber, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x37.png" xlink:type="simple"/></inline-formula>becomes the signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x38.png" xlink:type="simple"/></inline-formula>. Undemodulated by photodetection, the</p><p>light signal is converted to the electrical signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x39.png" xlink:type="simple"/></inline-formula>. Finally, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x40.png" xlink:type="simple"/></inline-formula>is mixed with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x41.png" xlink:type="simple"/></inline-formula> to get the signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x42.png" xlink:type="simple"/></inline-formula>, which is critical to RCS characteristic.</p><disp-formula id="scirp.70295-formula224"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x43.png"  xlink:type="simple"/></disp-formula><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Process of the photoelectric conversion</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70295x44.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Transfer chart of the received signal</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70295x45.png"/></fig><disp-formula id="scirp.70295-formula225"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x46.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula226"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x47.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula227"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x48.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula228"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x49.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x50.png" xlink:type="simple"/></inline-formula>is optical insertion loss, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x51.png" xlink:type="simple"/></inline-formula>is fiber loss. The equation may also be expressed as:</p><disp-formula id="scirp.70295-formula229"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula230"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x53.png"  xlink:type="simple"/></disp-formula><p>S is light sensitivity of the detector. After filtering, signal become<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x54.png" xlink:type="simple"/></inline-formula>. After mixing, we get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x55.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/70295x56.png" xlink:type="simple"/></inline-formula>is mixer insertion loss.</p><disp-formula id="scirp.70295-formula231"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x57.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.70295-formula232"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/70295x58.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_3"><title>3.3. Testing</title><p><xref ref-type="fig" rid="fig4">Figure 4</xref> is the result of phase delay. Obviously, the phase delay is linear. This result indicates that, after transmission of the photoelectric conversion system, the phase delay of the signal is linear and distortion does not happen. <xref ref-type="fig" rid="fig5">Figure 5</xref> is a phase noise plot, the black broken line represents the phase noise of the original signal, red polylines indicates signal’s phase noise after transported by the system. Obviously, after transmission of the photoelectric conversion system, the phase noise of the signal does not deteriorate.</p></sec></sec><sec id="s4"><title>4. The Actual Test of RCS</title><p><xref ref-type="fig" rid="fig6">Figure 6</xref> is a test result of RCS characteristic. Measured object can be clearly distinguished from the background. This suggests that by applying photoelectric conversion system to the RCS, we have successfully measured objects’ RCS characteristic in Outdoor-field measurement.</p></sec><sec id="s5"><title>5. Conclusions</title><p>By testing photovoltaic systems, we know that, transported through the photoelectric conversion transmission system, the phase and amplitude of the signal vary linearly, which guarantees the accuracy of signal transmission. At the same time, transported through the system, the changes of phase noise is within the error range.</p><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> The result of phase dela</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70295x59.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Phase noise plot</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70295x60.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> The result of RCS characteristic</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/70295x61.png"/></fig><p>This solves the problem of long-distance transmission of the received signal.</p><p>In a word, applying photoelectric conversion system to RCS measurement technology does solve the problem of signals’ long transmission, which makes it possible to measure full-size objects’ bistatic RCS characteristics.</p></sec><sec id="s6"><title>Cite this paper</title><p>Yilong Chen,Tao Hong,Zhihua Chen, (2016) The Study of Full-Size Objects’ Bistatic Rader Cross Section Measurement Based on Photoelectric Conversion. 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