<?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">IJCNS</journal-id><journal-title-group><journal-title>International Journal of Communications, Network and System Sciences</journal-title></journal-title-group><issn pub-type="epub">1913-3715</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijcns.2017.108B022</article-id><article-id pub-id-type="publisher-id">IJCNS-78397</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject></subj-group></article-categories><title-group><article-title>
 
 
  Optimization of Adaptive MTI Filter
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Wenxu</surname><given-names>Zhang</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>Shudi</surname><given-names>Ma</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>Qiuying</surname><given-names>Du</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Information and Communication Engineering, Harbin Engineering University, Harbin, China</addr-line></aff><pub-date pub-type="epub"><day>14</day><month>08</month><year>2017</year></pub-date><volume>10</volume><issue>08</issue><fpage>206</fpage><lpage>217</lpage><history><date date-type="received"><day>May</day>	<month>31,</month>	<year>2017</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>August</month>	<year>11,</year>	</date><date date-type="accepted"><day>August</day>	<month>14,</month>	<year>2017</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>
 
 
  
    Moving target indication (MTI) is an effective means for radar to find moving targets in clutter environment. This paper introduces the basic principles of MTI, how to avoid the blind speed problem and the optimization of MTI filter. Implementing the multi-notch adaptive moving target indication (AMTI) filter that designed by using the stagger code in varied cases, which is based on a feature vector method optimization. 
  
 
</p></abstract><kwd-group><kwd>Adaptive Moving Target Indication (AMTI)</kwd><kwd> Stagger Code</kwd><kwd> Feature Vector Method</kwd><kwd> Multi-Notch</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>MTI band-stop filter as a “single channel”, followed by detection is relatively simple. When the target speed is large and the repetition frequency is low, make sure that there is no distance blur, through the “variable week” variable repeat cycle or repeat and “time varying” [<xref ref-type="bibr" rid="scirp.78397-ref1">1</xref>]. Can overcome the blind speed problem, the drawback is no improvement in noise. In general, the mess is not very strong, the radar can handle a limited number of pulses, suitable for the use of repetitive and time-varying weighted system. The adaptive has a variety of ways to achieve, in which the performance is better “first order” and “second order”. The first- order basic method is to use the interval-based velocity measurement and the zero-point distribution method to determine the weighting parameters of the clutter cancellation filter to obtain the filter whose notch is aligned with the center of the clutter spectrum [<xref ref-type="bibr" rid="scirp.78397-ref2">2</xref>]. Its advantages are simpler, the disadvantage is that it cannot be adaptive with the clutter spectrum, so sometimes the performance is worse. The second-order basic method is to estimate the clutter covariance matrix, and then use matrix inversion or feature decomposition feature vector method to determine the filter weight coefficient.</p><p>This paper first analyzes the moving target indication (MTI), on this basis, the MTI is optimized, and the appropriate filter coefficients are designed by the feature vector method, which can effectively suppress the clutter. And the use of stagger code design MTI filter to eliminate the impact of blind speed. For motion clutter, the spectral center is not at zero frequency, and is time-varying. In order to suppress such clutter, this paper adopts adaptive motion clutter suppression technique AMTI, and designs multi-notch AMTI filter [<xref ref-type="bibr" rid="scirp.78397-ref3">3</xref>].</p></sec><sec id="s2"><title>2. Research on Adaptive Clutter Suppression Algorithm</title><p>The earliest MTI filter is a delay line canceller, is currently one of the most commonly used MTI filter. According to the different number of cancellation, but also divided into single delay line canceller, double delay line canceller and multi-delay line canceller [<xref ref-type="bibr" rid="scirp.78397-ref4">4</xref>].</p><p>Single delay line canceller as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, the impulse response of the single delay line canceller is expressed as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x2.png" xlink:type="simple"/></inline-formula>, and output <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x3.png" xlink:type="simple"/></inline-formula> is equal to the convolution between the impulse response <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x4.png" xlink:type="simple"/></inline-formula> and the input <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x5.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.78397-ref5">5</xref>].</p><p>The impulse response of the counter is:</p><disp-formula id="scirp.78397-formula358"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x6.png"  xlink:type="simple"/></disp-formula><p>The power gain of the single delay line canceller is:</p><disp-formula id="scirp.78397-formula359"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x7.png"  xlink:type="simple"/></disp-formula><p>Double delay line canceller as shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>. The response of the double delay line canceller is</p><disp-formula id="scirp.78397-formula360"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x8.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Single delay line canceller</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x9.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Double delay line canceller</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x10.png"/></fig><p>The double delay line canceller impulse response is:</p><disp-formula id="scirp.78397-formula361"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x11.png"  xlink:type="simple"/></disp-formula><p>The adaptive moving target indication (AMTI) filter is usually composed of a FIR filter with a horizontal structure. The output of the MTI filter is:</p><disp-formula id="scirp.78397-formula362"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x12.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x13.png" xlink:type="simple"/></inline-formula> is the weight vector and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x14.png" xlink:type="simple"/></inline-formula> is the input signal vector. The frequency response of this filter is:</p><disp-formula id="scirp.78397-formula363"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x15.png"  xlink:type="simple"/></disp-formula><p>In the radar system, in order to avoid the occurrence of blind effects, usually the use of “variable T” approach, that is, by regularly changing the radar launch pulse period so that the frequency of blindness is greater than the target possible Doppler frequency. Adaptive clutter suppression is compatible with parametric techniques, meaning that the clutter suppression filter must be time-varying. For the determined <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x16.png" xlink:type="simple"/></inline-formula> value, the frequency characteristic of the MTI filter is determined only by the weight vector, so the calculation of the weight vector is the core of the MTI process, according to different design methods, the optimal weight vector is generally different. In engineering practice, the improvement factor is often used to measure the performance of MTI system. The improvement factor of the MTI filter is defined as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x17.png" xlink:type="simple"/></inline-formula>. Obviously, the greater the<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x18.png" xlink:type="simple"/></inline-formula>, the better the effect of the system on clutter suppression. It has been proved that the optimal weight vector of the MTI filter should be the eigenvector corresponding to the minimum eigenvalue of the covariance matrix of the input clutter, in order to maximize the average improvement factor of the MTI. At this point the improvement factor is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x19.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.78397-ref6">6</xref>].</p><sec id="s2_1"><title>2.1. Optimal Design of Filter</title><p>The so-called optimization design requires a set of optimal filter coefficients, to maximize the improvement factor, a lot of design methods. In the case of the variable T, the better methods are feature vector method, matching algorithm, zero-point allocation method and linear prediction method [<xref ref-type="bibr" rid="scirp.78397-ref7">7</xref>]. The feature vector method is the solution that minimizes the clutter output power when the target gain is constant. The zero-point assignment method is to set the frequency response zero at the notch when designing the band-stop filter. The matching algorithm and the linear prediction method are the solutions that minimize the clutter output power when one of the elements of the weight vector is constant. So the feature vector method has better performance [<xref ref-type="bibr" rid="scirp.78397-ref8">8</xref>].</p><p>The feature vector method is a clutter suppression method based on the maximum improvement factor.</p><p>It is usually assumed that the clutter has a Gaussian power spectrum, the spectral center is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x20.png" xlink:type="simple"/></inline-formula>, the spectral width is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x21.png" xlink:type="simple"/></inline-formula>, and the spectral density function is:</p><disp-formula id="scirp.78397-formula364"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x22.png"  xlink:type="simple"/></disp-formula><p>According to the Wiener filter theory, if the clutter is a stationary stochastic process, its power spectrum and autocorrelation function are Fourier transform pairs. Therefore, the clutter autocorrelation function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x23.png" xlink:type="simple"/></inline-formula> is the Fourier transform of its power spectrum<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x24.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.78397-formula365"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x25.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x26.png" xlink:type="simple"/></inline-formula>is the relevant time. If the center of the clutter spectrum is zero, then</p><disp-formula id="scirp.78397-formula366"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x27.png"  xlink:type="simple"/></disp-formula><p>We obtain the clutter autocorrelation matrix A of N pulses</p><disp-formula id="scirp.78397-formula367"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x28.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x29.png" xlink:type="simple"/></inline-formula>, the Doppler spectrum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x30.png" xlink:type="simple"/></inline-formula> of the target echo signal can be expressed as</p><disp-formula id="scirp.78397-formula368"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x31.png"  xlink:type="simple"/></disp-formula><p>The target autocorrelation function is</p><disp-formula id="scirp.78397-formula369"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x32.png"  xlink:type="simple"/></disp-formula><p>Assume that the clutter data and the target data of the N pulse MTI input are respectively</p><disp-formula id="scirp.78397-formula370"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x33.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78397-formula371"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x34.png"  xlink:type="simple"/></disp-formula><p>Then the MTI output of the clutter power and signal power are</p><disp-formula id="scirp.78397-formula372"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x35.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78397-formula373"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x36.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x37.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x38.png" xlink:type="simple"/></inline-formula> represent the clutter power and the signal power at the MTI filter input, respectively, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x39.png" xlink:type="simple"/></inline-formula>is the weight vector of the FIR filter. According to the definition of the improvement factor of the MTI filter</p><disp-formula id="scirp.78397-formula374"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x40.png"  xlink:type="simple"/></disp-formula><p>By <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x41.png" xlink:type="simple"/></inline-formula> know, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x42.png" xlink:type="simple"/></inline-formula>for the unit array, therefore,</p><disp-formula id="scirp.78397-formula375"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x43.png"  xlink:type="simple"/></disp-formula><p>The characteristic equation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x44.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.78397-formula376"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x45.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x46.png" xlink:type="simple"/></inline-formula> is the eigenvector corresponding to the eigenvalue<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x47.png" xlink:type="simple"/></inline-formula>. Among them</p><disp-formula id="scirp.78397-formula377"><graphic  xlink:href="http://html.scirp.org/file/78397x48.png"  xlink:type="simple"/></disp-formula><p>In the eigenvalues of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x49.png" xlink:type="simple"/></inline-formula>, the subspace of the eigenvector corresponding to the large eigenvalue is the subspace of the signal, and the main points of the clutter are located in this subspace. The subspace of the eigenvector corresponding to the small eigenvalue is the noise subspace. Since the noise subspace is orthogonal to the signal subspace, the eigenvector B corresponding to the minimum eigenvalue <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x50.png" xlink:type="simple"/></inline-formula> is taken as the weight vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x51.png" xlink:type="simple"/></inline-formula> of the MTI filter, this can suppress the clutter component to the greatest extent, which is the biggest improvement factor [<xref ref-type="bibr" rid="scirp.78397-ref9">9</xref>].</p></sec><sec id="s2_2"><title>2.2. Stagger Repetition Frequency</title><p>In general, it is not possible to obtain a PRF that can meet the required ambiguous distance and Doppler coverage. Therefore, a method of stagger repetition frequency is proposed. Stagger repetition frequency is a measure that can be used to prevent blind influence [<xref ref-type="bibr" rid="scirp.78397-ref10">10</xref>].</p><p>If the radar uses N repetition frequencies, their repetition periods can be expressed as</p><disp-formula id="scirp.78397-formula378"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x52.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x53.png" xlink:type="simple"/></inline-formula>is the maximum convention period for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x54.png" xlink:type="simple"/></inline-formula>, then the odds ratio is:</p><disp-formula id="scirp.78397-formula379"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x55.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x56.png" xlink:type="simple"/></inline-formula>is the stagger code, the ratio of the largest <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x57.png" xlink:type="simple"/></inline-formula> value to the minimum<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x58.png" xlink:type="simple"/></inline-formula> value in the parametric code is called the maximum ratio <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x59.png" xlink:type="simple"/></inline-formula> of the azimuth cycle.</p><disp-formula id="scirp.78397-formula380"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x60.png"  xlink:type="simple"/></disp-formula><p>If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x61.png" xlink:type="simple"/></inline-formula> is mutually different and satisfies Equation (22), then the first true blind velocity corresponds to the Doppler frequency<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x62.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.78397-formula381"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x63.png"  xlink:type="simple"/></disp-formula><p>The average repetition period of the radar is</p><disp-formula id="scirp.78397-formula382"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x64.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x65.png" xlink:type="simple"/></inline-formula>is the mean of the difference. Therefore</p><disp-formula id="scirp.78397-formula383"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x66.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.78397-formula384"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x67.png"  xlink:type="simple"/></disp-formula><p>Because <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x68.png" xlink:type="simple"/></inline-formula> is the average radar repetition frequency, it is also called <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x69.png" xlink:type="simple"/></inline-formula> for the blind expansion factor.</p><p>The coefficient of the MTI filter between the pulses is different for each pulse of the three pulse canceller, so it is a time-varying filter. If the radar uses three repetition frequencies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x70.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x71.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x72.png" xlink:type="simple"/></inline-formula>at one time, three sets of MTI filters work in turn. The depth of the stagger MTI filter speed response notch is independent of the form of the canceller and is independent of the pulse received in the radar antenna beam and is related to the maximum ratio of the azimuth cycle. The larger the maximum change ratio, the shallower the corresponding notch depth.</p></sec><sec id="s2_3"><title>2.3. Optimization of Adaptive MTI Filter</title><p>In the clutter region, the spectral center <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x73.png" xlink:type="simple"/></inline-formula> of the motion clutter in the input signal is estimated to obtain the Doppler frequency <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x74.png" xlink:type="simple"/></inline-formula> estimate of the center of the clutter spectrum. And then estimate the spectral width <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x75.png" xlink:type="simple"/></inline-formula> to obtain the estimated value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x76.png" xlink:type="simple"/></inline-formula> of the spectral width. Then we obtain the weight coefficient of the multi-notch filter by using the obtained estimator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x77.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x78.png" xlink:type="simple"/></inline-formula> into the feature vector method, and design the MTI filter with multi-notch. As shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><p>First estimate the motion of the clutter spectrum center.</p><p>The radar suffers from narrowband clutter and noise that can be expressed as</p><disp-formula id="scirp.78397-formula385"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x79.png"  xlink:type="simple"/></disp-formula><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Optimization design of adaptive MTI filter</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x80.png"/></fig><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x81.png" xlink:type="simple"/></inline-formula>is the amplitude, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x82.png" xlink:type="simple"/></inline-formula>is the Doppler frequency of the clutter, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x83.png" xlink:type="simple"/></inline-formula>is the initial phase, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x84.png" xlink:type="simple"/></inline-formula> is the additive noise. Noise is not related to clutter, and noise between different PRI is uncorrelated.</p><p>Delay the signal after a PRI</p><disp-formula id="scirp.78397-formula386"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x85.png"  xlink:type="simple"/></disp-formula><p>The correlation function of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x86.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x87.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.78397-formula387"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x88.png"  xlink:type="simple"/></disp-formula><p>Therefore, the center frequency estimate of the clutter spectrum is obtained</p><disp-formula id="scirp.78397-formula388"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x89.png"  xlink:type="simple"/></disp-formula><p>After obtaining the center frequency of the clutter spectrum, the spectral width estimation is performed by the integral method.</p><p>Combined with the Gauss spectrum, there are Gaussian power spectra</p><disp-formula id="scirp.78397-formula389"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x90.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x91.png" xlink:type="simple"/></inline-formula>is the frequency variance of the Gaussian power spectrum, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x92.png" xlink:type="simple"/></inline-formula>is the center of the power spectrum, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x93.png" xlink:type="simple"/></inline-formula> is the corresponding power spectrum at zero Doppler frequency. According to the definition of half power points <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x94.png" xlink:type="simple"/></inline-formula></p><p>According to the nature of Gaussian distribution, there are</p><disp-formula id="scirp.78397-formula390"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/78397x95.png"  xlink:type="simple"/></disp-formula><p>Prior to the estimated spectrum as the center to both sides of the center <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x96.png" xlink:type="simple"/></inline-formula> of the accumulated clutter power spectrum (corresponding to integration), to 95.44% for the energy threshold, and then using the relationship between <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x97.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x98.png" xlink:type="simple"/></inline-formula> to the spectral width <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x99.png" xlink:type="simple"/></inline-formula> of the spectral estimate Gauss. After obtaining the estimated spectral center and estimating the spectrum width, the weight coefficient of the filter is obtained by using the feature vector method.</p><p>It is found that the power spectrum is the sum of their respective power spectra for the stagger clutter of multiple Gaussian spectra. The autocorrelation function should also have the sum of the corresponding multi-clutter components. Thus, we can derive the weight coefficients of two or more notch filters to design a multi-notch AMTI filter.</p></sec></sec><sec id="s3"><title>3. Simulation and Performance Analysis</title><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref>, obviously, the frequency response of the single delay line canceller and the double delay line canceller changes cyclically, and the period is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x100.png" xlink:type="simple"/></inline-formula>. The peak appears at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x101.png" xlink:type="simple"/></inline-formula>, and the zero value appears at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x102.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/78397x103.png" xlink:type="simple"/></inline-formula>. As</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Normalized frequency response of single delay line canceller and double delay line supporter. (a) dB. (b) Volt.</title></caption><fig id ="fig4_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x104.png"/></fig><fig id ="fig4_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x105.png"/></fig></fig-group><p>can be seen from the figure, the double delay line canceller has a deeper notch and a more flat passband response than a single delay line canceller.</p><p>In <xref ref-type="fig" rid="fig5">Figure 5</xref>, the frequency response is still cyclical when the T is equal. It can be clearly seen from the figure that the notch depth is significantly enhanced compared to the delay line canceller, the passband response is also more flat, and the frequency of the notches can be set at the same time.</p><p>In <xref ref-type="fig" rid="fig6">Figure 6</xref>, it can be seen that the use of staggered repetition frequency can greatly improve the first blind speed. The larger stagger ratio, the lighter the</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Normalized frequency response of the MTI filter. (a) Center of the clutter spectrum: 0 Hz. (b) Center of the clutter spectrum: 50 Hz.</title></caption><fig id ="fig5_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x106.png"/></fig><fig id ="fig5_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x107.png"/></fig></fig-group><p>corresponding notch, and avoid the loss of weak targets in one of them.</p><p><xref ref-type="fig" rid="fig7">Figure 7</xref> shows the normalized frequency response of the MTI filter designed using the feature vector method, Filter length of 4 order, the average pulse repetition frequency of 100 Hz, the stagger ratio of 15:16:17, The center of the clutter spectrum is selected as 0 Hz and 50 Hz, respectively, the spectral width is 0.64 Hz. The filter has a very deep notch at the clutter component, the entire pass band is relatively flat, and effectively suppresses the blind speed.</p><p>In <xref ref-type="fig" rid="fig8">Figure 8</xref>, filter length of 4 order, the average pulse repetition frequency of 100 Hz, the stagger ratio of 15:16:17. The clutter center frequency is 0 Hz, the</p><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Normalized frequency response of the three-pulse differential register. (a) Stagger ratio: 13:16:19. (b) Stagger ratio: 15:16:17.</title></caption><fig id ="fig6_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x108.png"/></fig><fig id ="fig6_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x109.png"/></fig></fig-group><p>spectral width is 0.64 Hz, the meteorological clutter center frequency is 30 Hz, the spectral width is 1.4 Hz. It can be seen from the figure at 0 Hz and 30 Hz with a deeper notch, can inhibit the clutter.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In the process of receiving the echo signal by the radar, the presence of the clutter signal has been interfering with the detection and extraction of the useful signal, it is necessary to suppress clutter. The moving target indication (MTI) technique has a good ability to suppress static clutter, but it is powerless for dynamic clutter. The use of adaptive technology can effectively inhibit the dynamic</p><fig-group id="fig7"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Normalized frequency response for the 15: 16: 17MTI filter. (a) Center of the clutter spectrum: 0 Hz. (b) Center of the clutter spectrum: 50 Hz.</title></caption><fig id ="fig7_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x110.png"/></fig><fig id ="fig7_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x111.png"/></fig></fig-group><p>clutter. In this paper, we propose an algorithm for processing AMTI based on the maximum average improvement factor, and give the corresponding MATLAB simulation waveform. Especially with the development of DSP chip, the pro- cessing speed has been improved, which made this method very suitable for practical application.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work is supported partly by National Natural Science Foundation of China under Grant No. 61301205 and No. 61571146, National Defense Based Science</p><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Normalized frequency response of multi-notch adaptive MTI (AMTI)</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/78397x112.png"/></fig><p>Research Program under Grant No. JCKY2013604B001. This paper is funded by the International Exchange Program of Harbin Engineering University for Innovation-oriented Talents Cultivation.</p></sec><sec id="s6"><title>Cite this paper</title><p>Zhang, W.X., Ma, S.D. and Du, Q.Y. (2017) Optimization of Adaptive MTI Filter. Int. J. Communications, Network and System Sciences, 10, 206-217. https://doi.org/10.4236/ijcns.2017.108B022</p></sec></body><back><ref-list><title>References</title><ref id="scirp.78397-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Geng, F.L. (2006) Radar Principle. Xi’an University of Electronic Science and Technology Press, Xi’an.</mixed-citation></ref><ref id="scirp.78397-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Wu, S.J. and Mei, X.C. (2008) Radar Signal Pro-cessing and Data Processing Technology. Electronic Industry Press, Beijing, 106-134.</mixed-citation></ref><ref id="scirp.78397-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Yuan, B.H., Zhang, W.X. and Zhong, X.K. (2017) Reconfigurable Multi-Channel Radar Transmitter Based on SDR. Applied Science and Technolo-gy.</mixed-citation></ref><ref id="scirp.78397-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Chen, J.C. and Geng, F.L. (1999) An Adaptive Moving Clutter Rejec-tion Technique. J Xi’an Electronics Technology University, 26, 174-177.</mixed-citation></ref><ref id="scirp.78397-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Yang, R. (2012) For the Cognitive Radar Waveform and Staggered Filter Optimization Algorithm. Xi’an University of Electronic Science and Technology.</mixed-citation></ref><ref id="scirp.78397-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Sun, C., Li, M. and Tao, H.H. (2014) Design of Gradi-ent MTI Filter Based on Gradient Immune Algorithm. Journal of China Institute of Electronic Science and Technology, 1673-5692.</mixed-citation></ref><ref id="scirp.78397-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Malanowski, M. (2006) Comparison of Adaptive Methods for Clutter Removal in PCL Radar. In-ternational Radar Symposium, Krakow, 24-26 May 2006, 1-4.  
https://doi.org/10.1109/IRS.2006.4338044</mixed-citation></ref><ref id="scirp.78397-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Hu, L.X. (2013) Application of EMD Algorithm in Radar Clutter Suppression. Xi’an University of Electronic Science and Technology.</mixed-citation></ref><ref id="scirp.78397-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Zhu, W. (2010) Research and Implementation of MTI &amp; MTD in Some VHF Radar. Xi’an University of Electronic Science and Technology.</mixed-citation></ref><ref id="scirp.78397-ref10"><label>10</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Hu</surname><given-names> K.X. </given-names></name>,<etal>et al</etal>. (<year>2006</year>)<article-title>Application of an Adaptive Clutter Rejection Technique in Radar</article-title><source> Modern Electronics Technique</source><volume> 29</volume>,<fpage> 24</fpage>-<lpage>26</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref></ref-list></back></article>