<?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.2016.96023</article-id><article-id pub-id-type="publisher-id">IJCNS-67687</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>
 
 
  Waveform Design for Cognitive Radar with Deterministic Extended Targets in the Presence of Clutter
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vahid</surname><given-names>Karimi</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>Reza</surname><given-names>Mohseni</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>Yaser</surname><given-names>Norouzi</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohammad</surname><given-names>Javad Dehghani</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Electrical Engineering, Amirkabir University of Technology, Tehran, Iran</addr-line></aff><aff id="aff1"><addr-line>Department of Electrical Engineering, Shiraz University of Technology, Shiraz, Iran</addr-line></aff><pub-date pub-type="epub"><day>24</day><month>06</month><year>2016</year></pub-date><volume>09</volume><issue>06</issue><fpage>250</fpage><lpage>268</lpage><history><date date-type="received"><day>24</day>	<month>January</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>21</month>	<year>June</year>	</date><date date-type="accepted"><day>24</day>	<month>June</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>
 
 
  Adjusting radar transmitted waveform to its environment is one of the most important roles in cognitive radar; having the capability of updating transmitted waveforms in different applications is a key point. It has been shown in many studies that if the waveform is designed according to the target and clutter characteristics, the detection performance will improve significantly. The uncertainty of the target radar signatures decreases via maximizing MI and the probability of extended target detection is increases via maximizing SNR. In this paper, a waveform design approach based on maximizing both SNR and MI and with regard to target and clutter shape is presented. The detection performance for proposed waveform is compared with previous proposed waveforms. The present paper compares different scenarios of target and clutter and using the probability of detection as a cost function to investigate the advantages and disadvantages of each waveform in different scenarios which are mainly discussed in this text. The desired waveform for cognitive radar is selected based on simultaneously making compromises between SNR and MI, which plays an important role in cognitive radar systems and based on the assumption addressed in the text, the best waveform transmitted into the environment.
 
</p></abstract><kwd-group><kwd>Signal to Noise Ratio</kwd><kwd> Mutual Information</kwd><kwd> Cognitive Radar</kwd><kwd> Deterministic Extended Target</kwd><kwd> Clutter</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Cognitive radar is a radar system which selects its transmitted waveform to adapt to the radar environment by using feedback structure from the receiver to the transmitter. In these systems waveforms can be adaptively optimized based on preceding knowledge about the targets and environments; it leads to the improvement of the total performance of system [<xref ref-type="bibr" rid="scirp.67687-ref1">1</xref>] . Design of transmitting waveform has an important effect on the performance and efficiency of radar system. Adaptive waveform design for target detection and recognition has been developed during the past decade, and also recently most studies have been devoted to radar waveform optimization. In these approaches, one method is based on signal-to-noise ratio (SNR) maximizing under a particular model of the system, interference, clutter and targets [<xref ref-type="bibr" rid="scirp.67687-ref2">2</xref>] . Another approach is based on mutual information which is first proposed by Bell [<xref ref-type="bibr" rid="scirp.67687-ref3">3</xref>] . Bell shows for estimating the parameters of a target from a given ensemble, the radar waveform should be designed to maximize the mutual information between the received signal and the target ensemble [<xref ref-type="bibr" rid="scirp.67687-ref4">4</xref>] . SNR-based optimum matched waveform for a specific target via frequency domain approach is proposed in [<xref ref-type="bibr" rid="scirp.67687-ref5">5</xref>] . An optimal waveform for T-72 and M1 main battle tanks detection is proposed in [<xref ref-type="bibr" rid="scirp.67687-ref6">6</xref>] .</p><p>The information-based approach in the presence of signal-dependent clutter is investigated in [<xref ref-type="bibr" rid="scirp.67687-ref7">7</xref>] . In their work, optimum waveform is investigated both from SNR maximization and information-theoretic approaches. The optimal waveform for detecting extended target in signal-dependent interference is proposed in [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] . They derive optimal waveform energy spectral density (ESD) by maximizing SNR. A method for waveform design based on mutual information is proposed in [<xref ref-type="bibr" rid="scirp.67687-ref9">9</xref>] in which the general water-filling method is utilized to solve the waveform design for the recognition of multiple extended targets. They have shown that their proposed method has the higher classification rate at higher SNRs and higher detection performance in lower SNRs as compared to LFM and water-filling signals. In [<xref ref-type="bibr" rid="scirp.67687-ref10">10</xref>] , the performance of waveform design in cognitive radar is discussed and a new iterative algorithm is proposed to synthesize a constant modulus waveform to maximize SNR and MI simultaneously. Designing matched waveforms based on maximizing SNR and MI for both deterministic and stochastic targets are discussed in [<xref ref-type="bibr" rid="scirp.67687-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.67687-ref12">12</xref>] ; using multiple transmission of obtaining waveform a target identification problem is investigated. A new technique is proposed in [<xref ref-type="bibr" rid="scirp.67687-ref13">13</xref>] , which improves the classification performance of SNR-based matched waveforms. In [<xref ref-type="bibr" rid="scirp.67687-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.67687-ref14">14</xref>] , a closed-loop strategy is applied to discriminate target classes rather than a finite ensemble of known targets. In [<xref ref-type="bibr" rid="scirp.67687-ref15">15</xref>] , optimization problem based on mutual information for waveform design in signal dependent clutter is discussed and a new waveform using interior-point method to carry out the optimization task is proposed. In previous papers such as [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.67687-ref16">16</xref>] , SNR improvement for proposed waveforms over LFM waveform is investigated and in this paper, we evaluate SNR and MI values for different waveforms and compare the results with LFM waveforms and show the best performance of obtaining waveforms.</p><p>The contributions of this paper include an analysis of applying both the information-based and SNR-based approach to different deterministic extended targets and clutter scenarios considering the energy constraint. In this study, energy distribution for optimum waveform in clutter and noise scenario with the energy constraint have been addressed and we focus on the point that waveform should put a considerable amount of available energy on the frequency bands in which the target spectrum frequency components is considerable while the clutter is negligible. We derive various waveforms for each scenario and finally compare our results with linear frequency modulated (LFM) waveform to verify the performance of the proposed waveform.</p><p>This paper is organized as follows: first a radar system model is described in Section 2 and then the derivation of MI-based and SNR-based waveforms in the presence of Gaussian clutter and other scenarios are derived. In Section 3, using the obtained relations in Section 2, transmit waveform spectrum for two deterministic extended targets are illustrated and the energy allocation realized by obtaining waveforms are briefly discussed. Section 4 generally discusses the performance of obtaining waveforms and other predefined waveforms and a new closed-loop structure for detecting targets in different scenarios is proposed. Finally, in Section 5, we provide a general conclusion.</p></sec><sec id="s2"><title>2. Problem Formulation</title><sec id="s2_1"><title>2.1. Signal, Clutter and Target Model</title><p>To analyze a radar system, all constituent blocks should be defined. We consider a signal model of a Gaussian extended target in the presence of clutter as shown in <xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref>. Now we define the essential target and clutter models to analyze the overall performance of a radar system.</p><p>Let x(t) be a finite-energy waveform with duration T. We assume x(t) is energy-limited and non-zero only in the time interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x7.png" xlink:type="simple"/></inline-formula> which has a bandwidth w; The energy content of this signal is:</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1"><xref ref-type="fig" rid="fig">Figure </xref>1</xref></label><caption><title> Known Gaussian extended target model in the presence of clutter [<xref ref-type="bibr" rid="scirp.67687-ref7">7</xref>] </title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x8.png"/></fig><disp-formula id="scirp.67687-formula920"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x9.png"  xlink:type="simple"/></disp-formula><p>c(t) is assumed to be sea clutter with known power spectral density (PSD) which can be approximated as follows:</p><disp-formula id="scirp.67687-formula921"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x10.png"  xlink:type="simple"/></disp-formula><p>Here f<sub>c</sub> is the peak locations of the Gaussian function; g<sub>c</sub> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x11.png" xlink:type="simple"/></inline-formula> are parameters which are specified according to problem conditions. h(t) is the impulse response of target. Once the impulse responses are generated, it is assumed that they are exactly known to the transmitter. In this study, target is assumed to have a Gaussian mixture shape with the following power spectral density:</p><disp-formula id="scirp.67687-formula922"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x12.png"  xlink:type="simple"/></disp-formula><p>where a<sub>i</sub> and f<sub>i</sub> are respectively determined between a specific amplitude range and an appropriate interval due to clutter and noise specifications. The variance <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x13.png" xlink:type="simple"/></inline-formula> is supposed to have a constant value. Finally n(t) denotes the noise, which is a complex zero mean WSS Gaussian random process with known PSD P<sub>n</sub>(f). Now let r(t) be the received signal that is equal to:</p><disp-formula id="scirp.67687-formula923"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x14.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2_2"><title>2.2. Waveform Derivation</title><p>In this part, the Energy Spectral Density (ESD) of MI-based is computed with the assumption of known target in different scenarios and compared with SNR-based waveform discussed in [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] . Like [<xref ref-type="bibr" rid="scirp.67687-ref11">11</xref>] , using Lagrangian multiplier, we have derived optimum waveform ESD based on MI criteria in both signal-dependent interference and signal-independent noise. The MI between a Gaussian target ensemble and the received signal without the presence of clutter is equal to:</p><disp-formula id="scirp.67687-formula924"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x15.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x16.png" xlink:type="simple"/></inline-formula> is the continuous target signature. Now let ε<sub>x</sub>(f) be the energy spectral density (ESD) of the waveform, so we have:</p><disp-formula id="scirp.67687-formula925"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x17.png"  xlink:type="simple"/></disp-formula><p>The desired waveform ESD is found by solving the constrained optimization problem:</p><disp-formula id="scirp.67687-formula926"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x18.png"  xlink:type="simple"/></disp-formula><p>With the energy constraint:</p><disp-formula id="scirp.67687-formula927"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x19.png"  xlink:type="simple"/></disp-formula><p>Now using the Lagrangian multiplier method, the waveform ESD will be obtained as follows:</p><disp-formula id="scirp.67687-formula928"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x20.png"  xlink:type="simple"/></disp-formula><p>We can equivalently maximize:</p><disp-formula id="scirp.67687-formula929"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x21.png"  xlink:type="simple"/></disp-formula><p>The first and the second derivatives of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x22.png" xlink:type="simple"/></inline-formula> with respect to ε<sub>x</sub>(f) are given by:</p><disp-formula id="scirp.67687-formula930"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x23.png"  xlink:type="simple"/></disp-formula><p>Since the second derivative is negative for all ε<sub>x</sub>(f), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x24.png" xlink:type="simple"/></inline-formula>is a concave function and by putting equating (10) to zero the desired ε<sub>x</sub>(f) is obtained as follows:</p><disp-formula id="scirp.67687-formula931"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x25.png"  xlink:type="simple"/></disp-formula><p>where the parameter λ is found by solving the following equation:</p><disp-formula id="scirp.67687-formula932"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x26.png"  xlink:type="simple"/></disp-formula><p>In Equation (12), we see that the waveform ESD will be equal to zero for those frequencies satisfying:</p><disp-formula id="scirp.67687-formula933"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x27.png"  xlink:type="simple"/></disp-formula><p>Thus, we can consider λP<sub>n</sub>(f) as a threshold which depends on coefficient λ which means the waveform only puts energy into those frequencies where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x28.png" xlink:type="simple"/></inline-formula>. Thus, for a radar system to be cognitive, it should customize the transmit waveform in such a way that it emphasizes frequency bands where the target spectrum is greater than the obtained threshold and deemphasizes frequency bands where the target is negligible as compared with clutter.</p><p>The mutual information between the received signal and the target ensemble with the presence of clutter is:</p><disp-formula id="scirp.67687-formula934"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x29.png"  xlink:type="simple"/></disp-formula><p>And like previous step for deriving non-clutter case we have:</p><disp-formula id="scirp.67687-formula935"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x30.png"  xlink:type="simple"/></disp-formula><p>We can equivalently maximize:</p><disp-formula id="scirp.67687-formula936"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x31.png"  xlink:type="simple"/></disp-formula><p>Now the first and second derivatives of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x32.png" xlink:type="simple"/></inline-formula> with respect to ε<sub>x</sub>(f) are computed and by following a procedure like the previous step for deriving MI-based waveform without the presence of clutter, leading to the waveform described by:</p><disp-formula id="scirp.67687-formula937"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x33.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.67687-formula938"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x34.png"  xlink:type="simple"/></disp-formula><p>And the parameter λ is found by solving the energy constraint equation:</p><disp-formula id="scirp.67687-formula939"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x35.png"  xlink:type="simple"/></disp-formula><p>In Equation (18), we see that the waveform ESD will put energy into those frequencies satisfying:</p><disp-formula id="scirp.67687-formula940"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x36.png"  xlink:type="simple"/></disp-formula><p>Here again the threshold λP<sub>n</sub>(f) is obtained by solving the energy constraint Equation (20) showing that the parameter λ is totally different for each energy constraint presented in this paper. A noteworthy point is that although the thresholds are absolutely similar, their values are different due to parameter λ. Consequently, the waveform energy allocation is different from the non-clutter case. It has been shown in simulation results that this waveform distributes most of its energy into frequency bands which the target PSD is high and the clutter PSD is low.</p><p>The waveform ESD for SNR-based waveform for a known target with the presence of clutter is described in [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] . SINR for a deterministic target in the presence of clutter is computed as:</p><disp-formula id="scirp.67687-formula941"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x37.png"  xlink:type="simple"/></disp-formula><p>And the waveform ESD using the Lagrangian multiplier technique is [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] :</p><disp-formula id="scirp.67687-formula942"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x38.png"  xlink:type="simple"/></disp-formula><p>where parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x39.png" xlink:type="simple"/></inline-formula> is found by solving:</p><disp-formula id="scirp.67687-formula943"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x40.png"  xlink:type="simple"/></disp-formula><p>As mentioned in [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] , the obtained waveform only puts energy into those frequencies where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x41.png" xlink:type="simple"/></inline-formula></p><p>as we derived for MI-based waveforms and λP<sub>n</sub>(f) is considered as a threshold with different values for all waveforms. The last waveform discussed here is the waveform ESD for SNR-based waveform without the presence of clutter. In this case by putting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x42.png" xlink:type="simple"/></inline-formula>, SNR expression in (22) is reduced to:</p><disp-formula id="scirp.67687-formula944"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x43.png"  xlink:type="simple"/></disp-formula><p>Using the Lagrange multiplier technique, we form the objective function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x44.png" xlink:type="simple"/></inline-formula> like previous steps, and we see that the first derivative of this function is independent of ε<sub>x</sub>(f) and simply implies that no solution exists using this technique. However, by the technique discussed in [<xref ref-type="bibr" rid="scirp.67687-ref2">2</xref>] and [<xref ref-type="bibr" rid="scirp.67687-ref11">11</xref>] , the transmit waveform x(t) with time duration T that optimizes (25) is defined by:</p><disp-formula id="scirp.67687-formula945"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x45.png"  xlink:type="simple"/></disp-formula><p>In summary, the transmit waveform x(t) that maximizes SNR is the Eigenfunction corresponding to the maximum eigenvalue of the kernel M(t) which is described by:</p><disp-formula id="scirp.67687-formula946"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x46.png"  xlink:type="simple"/></disp-formula><p>And finally the SNR has been just the product of this eigenvalue and the energy in the transmit waveform as follows:</p><disp-formula id="scirp.67687-formula947"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x47.png"  xlink:type="simple"/></disp-formula><p>Different methods are proposed to derive the optimum waveform for this scenario. One of them is the approach proposed in [<xref ref-type="bibr" rid="scirp.67687-ref16">16</xref>] whereby updating phase modulated waveform in such a way that the SNR at the receiver filter output is maximized and the performance of extended target detection is enhanced significantly. In this paper, we proposed a new waveform due to energy constraint and also the distribution of the target on specified bandwidth. Indeed, we are interested in waveforms which can follow the target spectrum and detect all peaks of the target in frequency domain. Regarding this assumption we defined the ESD of this waveform in such a way that is independent of noise and clutter power spectrum and only depends on the target spectrum. We name this waveform “Target Spectrum Follower (TSF)” [<xref ref-type="bibr" rid="scirp.67687-ref17">17</xref>] . Therefore, ESD of the proposed waveform is as follows:</p><disp-formula id="scirp.67687-formula948"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x48.png"  xlink:type="simple"/></disp-formula><p>where the parameter λ is found by solving:</p><disp-formula id="scirp.67687-formula949"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x49.png"  xlink:type="simple"/></disp-formula><p>The ESD obtained using this method produces a waveform that totally follows the target spectrum. The energy of transmitted waveform is allocated to the target peaks in proportion to the amount of every peak; in other words, the proposed waveform allocates its energy in all of target spectrum frequency bands. This allocation is illustrated in <xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref>(d) and <xref ref-type="fig" rid="fig4"><xref ref-type="fig" rid="fig">Figure </xref>4</xref>(d). Unlike other waveforms, this waveform can detect lower target peaks which has some advantages and disadvantages that will be discussed later. Our main purpose to design such a waveform is to show the important role of energy allocation in radar transmitted waveform and the effect of this consideration on target detection scenarios.</p><p>The waveforms discussed in this paper are: SNR-based waveform in clutter (CSNR-based) [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] , MI-based waveform without clutter (MI-based), MI-based waveform in clutter (CMI-based), target spectrum follower (TSF) and linear frequency modulation waveform (LFM).</p></sec></sec><sec id="s3"><title>3. Numerical Examples</title><sec id="s3_1"><title>3.1. Numerical Waveform Examples with Specified Gausiian Clutter</title><p>We cannot find a closed-form solution for the waveform derivations. In this section, we provide two numerical examples which can be obtained using the proposed waveforms. As it was mentioned in the previous section, target and clutter are supposed to have a Gaussian shape with the power spectrum <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x50.png" xlink:type="simple"/></inline-formula> and P<sub>c</sub>(f), respectively. Two targets for numerical examples are considered here. In example one, suppose that we have a Gaussian target and clutter shown in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref>. The ESD for CSNR-based, CMI-based, MI-based and TSF waveforms for target 1 are evaluated and shown in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref>. In the case of waveform design in signal-dependent interference, CSNR-based waveform tends to concentrate most of its energy on one dominant narrow frequency band in which the target PSD is comparable to clutter PSD putting the rest of its energy into frequency bands with great amount of target PSD. CMI-based waveform follows such a procedure with different amounts of energy allocation to each frequency band. Therefore, both waveforms place most of their energy where clutter power is low. We will briefly discuss the performance of CSNR-based waveform over CMI-based waveform later. As</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref></label><caption><title> Corresponding ESD to Different Scenarios with Target 1. (a) ESD for CSNR-based waveform; (b) ESD for MI-based waveform; (c) ESD for CMI-based Waveform; (d) ESD for TSF Waveform.</title></caption><fig id ="fig2_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x51.png"/></fig><fig id ="fig2_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x52.png"/></fig><fig id ="fig2_3"><label>(d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x53.png"/></fig><fig id ="fig2_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x54.png"/></fig></fig-group><p>shown in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref>(b) MI-based waveform without considering clutter shape puts its energy relative to the target peak values and finally TSF waveform unlike other waveforms follows all target peak energy allocation is done in each band where the target has either small or large peaks. As shown in this figure, CSNR-based waveform compared with other waveforms distributed less energy into the frequency band [−0.2, 0], where the target is comparable to the clutter and instead puts more energy into the frequency band [0.3, 0.4], where the clutter has smaller amounts of PSD compared with the target.</p><p>The target-to-noise ratio (TNR) is defined as the ratio of the area under target PSD to the area under noise PSD [<xref ref-type="bibr" rid="scirp.67687-ref17">17</xref>] , and also the ratio of the area under the clutter PSD to noise PSD is called clutter-to-noise ratio (CNR). The last ratio is TCR which is the area under the target PSD to clutter PSD. In this example, TNR, CNR and TCR are 1.66 dB, 10.94 dB and −9.29 dB, respectively. As we expected, with specified energy constraint, these waveforms which are designed in such a way to focus their energy into frequency bands; the target has the largest PSD value and the clutter has the smallest PSD value. As can be seen in <xref ref-type="fig" rid="fig2"><xref ref-type="fig" rid="fig">Figure </xref>2</xref> for target 1, the CSNR- based and CMI-based allocated most of their energy in the frequency sub-band [0.3, 0.4], where the target is comparable in terms of PSD value with clutter while this point for MI-based and TSF waveforms are not considered. We will show later that this is the main reason for the improvement of CSNR-based and CMI-based on scenarios with low values of TCR.</p><p>We repeat the experiment with target 2 and with the same clutter and noise PSD. For this target, we have TNR = 0.51 dB, CNR = 0.95 dB and TCR = −0.44 dB and corresponding waveforms for this target scenario are computed and illustrated in <xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref>. As seen in this figure, TSF waveform follows all target peaks and puts its energy due to each target peak not consider clutter and noise for this energy allocation. CMI-based and MI-based waveforms have approximately similar response to this target and just follow two great peaks of this target putting their energy equally into the corresponding frequency bands while CSNR-based puts its main energy into frequency band which has the smallest value of clutter PSD value; this could be a reason for better performance of this waveform compared with others.</p></sec><sec id="s3_2"><title>3.2. SNR and MI Comparison between Different Waveforms</title><p>As shown before, solving optimization problem requires knowledge of the target and clutter spectrum. It was shown in [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] that the probability of detection is related to the probability of false alarm by:</p><disp-formula id="scirp.67687-formula950"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x55.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x56.png" xlink:type="simple"/></inline-formula> is the cumulative density function of a chi-square random variable with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x57.png" xlink:type="simple"/></inline-formula> degrees of freedom. It has been shown that:</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3"><xref ref-type="fig" rid="fig">Figure </xref>3</xref></label><caption><title> Corresponding ESD for different scenarios with target 2. (a) ESD for CSNR-based waveform; (b) ESD for MI-based waveform; (c) ESD for CMI-based waveform. (d) ESD for TSF waveform.</title></caption><fig id ="fig3_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x58.png"/></fig><fig id ="fig3_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x59.png"/></fig><fig id ="fig3_3"><label>(d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x60.png"/></fig><fig id ="fig3_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x61.png"/></fig></fig-group><disp-formula id="scirp.67687-formula951"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x62.png"  xlink:type="simple"/></disp-formula><p>With a good approximation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-9702060x63.png" xlink:type="simple"/></inline-formula> is equal to:</p><disp-formula id="scirp.67687-formula952"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x64.png"  xlink:type="simple"/></disp-formula><p>And finally we have:</p><disp-formula id="scirp.67687-formula953"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-9702060x65.png"  xlink:type="simple"/></disp-formula><p>Using the above equation, since maximizing P<sub>D</sub> for arbitrary values of P<sub>fa</sub> depends on the values of SINR for each waveform and by maximizing SINR, we can achieve higher values of P<sub>D</sub>. Previous research has shown that SNR-based waveform and LFM waveform are compared through this method and shown that the proposed method had better performance in terms of maximizing the probability of detection. Here, we obtained different waveforms with both SNR and MI values and now we want to select the desired waveform based on achieving maximizing probability of detection for each target and clutter scenarios regarding the point that the desired waveform should have a sufficient MI value in comparison with other waveforms. MI and SINR which are defined in (14), (21) respectively, are considered as objective functions. We computed their values for three different targets.</p><p>For each target the corresponding waveform according to target, clutter and noise spectrum is generated and utilized for computing SNR and MI. Now we suppose a specific scenario with known target, clutter and noise PSDs. We are interested in investigating the effects of target, clutter and noise separately. So, we consider the scenario 1 which includes a specific Gaussian extended target, Gaussian clutter and AWGN noise with known PSDs, then compute CNR, TCR and TNR values for this scenario. Afterwards, by changing clutter (target and noise are fixed), scenario 2 is obtained and similarly scenario 3 and scenario 4 are obtained by changing the target and noise, respectively. Target, Clutter and Noise PSD for each scenario are illustrated in <xref ref-type="fig" rid="fig4"><xref ref-type="fig" rid="fig">Figure </xref>4</xref> and also their CNR, TCR and TNR values are shown in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>After defining scenarios, ESD of each waveform in accordance with each scenario is computed due to the obtained relations. Eventually for each scenario corresponding SNR and MI values for investigating the applied changes in target, clutter and noise are evaluated by Equation (15), (22) as summarized in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>As indicated in <xref ref-type="table" rid="table2">Table 2</xref>, CSNR-based waveform compared with other waveforms has greater SNR amount for each scenario, and according to (34) this waveform should have the best performance in terms of maximizing the probability of detection. The point that should be considered is its MI value which is not maximum even</p><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4"><xref ref-type="fig" rid="fig">Figure </xref>4</xref></label><caption><title> Target, clutter and noise PSD for each scenario. (a) Scenario 1; (b) Scenario 2; (c) Scenario 3; (d) Scenario 4.</title></caption><fig id ="fig4_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x66.png"/></fig><fig id ="fig4_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x67.png"/></fig><fig id ="fig4_3"><label>(d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x68.png"/></fig><fig id ="fig4_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x69.png"/></fig></fig-group><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> CNR, TCR and TNR values for different scenarios in dB</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Value(dB) Scenario</th><th align="center" valign="middle" >CNR</th><th align="center" valign="middle" >TCR</th><th align="center" valign="middle" >TNR</th></tr></thead><tr><td align="center" valign="middle" >Scenario 1</td><td align="center" valign="middle" >10.95</td><td align="center" valign="middle" >−17.37</td><td align="center" valign="middle" >−6.42</td></tr><tr><td align="center" valign="middle" >Scenario 2</td><td align="center" valign="middle" >−6.62</td><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >−6.42</td></tr><tr><td align="center" valign="middle" >Scenario 3</td><td align="center" valign="middle" >10.95</td><td align="center" valign="middle" >−11.82</td><td align="center" valign="middle" >−0.87</td></tr><tr><td align="center" valign="middle" >Scenario 4</td><td align="center" valign="middle" >20.95</td><td align="center" valign="middle" >−17.37</td><td align="center" valign="middle" >3.58</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Corresponding SNR and MI values in dB for different waveforms in each scenario</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Waveform Scenario</th><th align="center" valign="middle" >MI-based Waveform</th><th align="center" valign="middle" >CMI-based Waveform</th><th align="center" valign="middle" >CSNR-based Waveform</th><th align="center" valign="middle" >TSF Waveform</th><th align="center" valign="middle" >LFM Waveform</th></tr></thead><tr><td align="center" valign="middle" >Scenario 1</td><td align="center" valign="middle" >SNR = 17.16 MI = 16.82</td><td align="center" valign="middle" >SNR = 17.94 MI = 17.45</td><td align="center" valign="middle" >SNR = 18.09 MI = 17.1</td><td align="center" valign="middle" >SNR = 15.66 MI = 15.55</td><td align="center" valign="middle" >SNR = 8.25 MI = 8.24</td></tr><tr><td align="center" valign="middle" >Scenario 2</td><td align="center" valign="middle" >SNR = 18.16 MI = 17.75</td><td align="center" valign="middle" >SNR = 18.16 MI = 17.76</td><td align="center" valign="middle" >SNR = 18.26 MI = 15.53</td><td align="center" valign="middle" >SNR = 16.06 MI = 15.94</td><td align="center" valign="middle" >SNR = 8.34 MI = 8.34</td></tr><tr><td align="center" valign="middle" >Scenario 3</td><td align="center" valign="middle" >SNR = 19.93 MI = 19.47</td><td align="center" valign="middle" >SNR = 22.5 MI = 21.51</td><td align="center" valign="middle" >SNR = 22.87 MI = 20.67</td><td align="center" valign="middle" >SNR = 19.76 MI = 19.52</td><td align="center" valign="middle" >SNR = 13.59 MI = 13.56</td></tr><tr><td align="center" valign="middle" >Scenario 4</td><td align="center" valign="middle" >SNR = 25.26 MI = 24.03</td><td align="center" valign="middle" >SNR = 26.75 MI = 25.03</td><td align="center" valign="middle" >SNR = 27.18 MI = 24.47</td><td align="center" valign="middle" >SNR = 24.15 MI = 23.39</td><td align="center" valign="middle" >SNR = 17.63 MI = 17.53</td></tr></tbody></table></table-wrap><p>in one scenario and this is the CMI-based waveform that has greater MI amounts compared with other waveforms. As mentioned in [<xref ref-type="bibr" rid="scirp.67687-ref18">18</xref>] , LFM waveform is a good candidate for distinguishing point targets, and for an extended target case may not have good performance which we will discuss in the following paragraph.</p><p>In <xref ref-type="table" rid="table2">Table 2</xref> for scanario1, we have 9.84 dB SNR improvement for CSNR-based waveform over LFM waveform and 9.69 dB SNR improvement for CMI-based waveform over LFM waveform. This improvement for the waveform is proposed in [<xref ref-type="bibr" rid="scirp.67687-ref8">8</xref>] over LFM waveform was 3 dB and by the method proposed in [<xref ref-type="bibr" rid="scirp.67687-ref16">16</xref>] SNR of the proposed waveform was about 4 dB higher than the square pulse or the LFM pulse. For TSF waveform, we have 7.41 dB improvement which can be a good choice in some scenarios. For example, for high values of TCR, this waveform has a better performance in terms of MI and approximately the same performance in terms of SNR compared with CSNR-based waveform.</p><p>It is obvious from <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref> that by decreasing the clutter PSD, SNR and MI value will increase from one scenario to another. This idea is true for the case of increasing the amounts of target spectrum and decreasing noise PSD.</p><p>To evaluate the performance, we used receiver operating characteristic (ROC) curves corresponding to the obtained waveforms and LFM. <xref ref-type="fig" rid="fig5"><xref ref-type="fig" rid="fig">Figure </xref>5</xref> shows these ROC curves for all scenarios. As it is clear, the improvement of obtaining waveforms over LFM is shown in this <xref ref-type="fig" rid="fig">Figure </xref>for all scenarios; we see that CSNR-based and CMI-based waveforms for all scenarios have a better performance compared with other waveforms.</p></sec></sec><sec id="s4"><title>4. Providing General Result and Defining an Appropriate Closed-Loop Structure</title><sec id="s4_1"><title>4.1. Numerical Results with Different Deterministic Extended Target, Clutter and Noise</title><p>Now to better demonstrate the importance of waveform design in cognitive radar, we simulate different targets, clutters and noise realizations. To reach an aggregation, we compute SNR and MI values for each waveform by changing TCR, TNR and CNR values in a specific range. For example in <xref ref-type="fig" rid="fig">Figure </xref>6(a) and <xref ref-type="fig" rid="fig">Figure </xref>6(b), SNR and MI changes in dB versus TCR for each waveform are illustrated. It can be concluded from this figure that all waveforms have a similar SNR performance with increasing TCR and as previously discussed have a better performance over LFM waveform.</p><p>From MI consideration, as we expected, CMI-based and MI-based have better performance with a little difference compared with CSNR-based and TSF waveforms. Finally, we can conclude that indifferent values of TCR, all waveforms have 9 dB and 7 dB improvement in SNR and MI, respectively over LFM waveform.</p><p><xref ref-type="fig" rid="fig">Figure </xref>6(c) and <xref ref-type="fig" rid="fig">Figure </xref>6(d) show the SNR and MI value changes in dB for different TNR values. As indicated in this Figure, CSNR-based and CMI-based waveforms are completely similar in low TNRs but in high TNR values in terms of MI, CMI-based waveform is slightly better. TSF waveform also shows a moderate performance and better than MI-based and LFM waveforms especially in moderate TNRs.</p><p>The last case shows the SNR and MI value changes in dB for different CNRs. As indicated in <xref ref-type="fig" rid="fig">Figure </xref>6(e) and <xref ref-type="fig" rid="fig">Figure </xref>6(f) for different values of CNRs, similar to those we have for TNR and TCR values, CSNR-based and CMI-based waveforms are completely similar. A noteworthy point is that in low CNR values, MI-based waveform has a good performance but with increasing CNR, its performance declines and TSF waveform performance outperform this waveform in high CNR values. Finally, LFM waveform is fairly constant with CNR and performs the poorly as compared with other waveforms. So, according to the mentioned features for each waveform and due to each application, we should propose a good structure which considers all aspects of the problem conditions. Due to each waveform feature, it should utilize the best waveform to transmit into the environment.</p><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5"><xref ref-type="fig" rid="fig">Figure </xref>5</xref></label><caption><title> ROC curves corresponding to each waveform and each scenario. (a) Scenario 1. (b) Scenario 2. (c) Scenario 3. (d) Scenario 4.</title></caption><fig id ="fig5_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x70.png"/></fig><fig id ="fig5_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x71.png"/></fig><fig id ="fig5_3"><label>(d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x72.png"/></fig><fig id ="fig5_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x73.png"/></fig></fig-group><p>Therefore, a cognitive radar should be designed in such a way that firstly evaluates the TCR, TNR and CNR values and considering to the application and also waveform features which are mainly discussed in this paper, chooses the best waveform to transmit into the environment and achieve the maximum probable values of P<sub>D</sub>.</p></sec><sec id="s4_2"><title>4.2. Determine a New Closed-Loop Structure for Detecting Deterministic Extended Targets</title><p>In <xref ref-type="fig" rid="fig">Figure </xref>7, new closed-loop structure for detecting M targets indifferent scenarios is proposed. In this structure, SNR and MI values are considered as the cost function. This means that in the transmitter, the desired waveform are selected based on its MI and SNR values.</p><fig-group id="fig6"><label><xref ref-type="fig" rid="fig">Figure </xref>6</label><caption><title> Comparison of SNR and MI versus TCR, TNR and CNR with deterministic extended target. (a) SNR versus TCR; (b) MI versus TCR; (c) SNR versus TNR; (d) MI versus TNR; (e) SNR versus CNR; (f) MI versus CNR.</title></caption><fig id ="fig6_1"><label>(b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x74.png"/></fig><fig id ="fig6_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x75.png"/></fig><fig id ="fig6_3"><label>(d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x76.png"/></fig><fig id ="fig6_4"><label>(e)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x77.png"/></fig><fig id ="fig6_5"><label>(e)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x78.png"/></fig><fig id ="fig6_6"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x79.png"/></fig></fig-group><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig">Figure </xref>7</label><caption><title> Modelling a new structure of cognitive radar for detecting targets in different noise and clutter scenarios</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-9702060x80.png"/></fig><p>As indicated in this figure, the proposed cognitive radar structure includes an adaptive transmitter based on the feedback from the receiver and the interactions with a defined database. The radar transmitted its initial waveform into the environment. If the target is detected in the receiver, we have reached our goal; otherwise, cognitive radar loop is established using a feedback from the receiver to the transmitter and this procedure is done as long as the target of interest is identified. Surely, we can set the number of transmitting signals to a predetermined value to prevent the cognitive radar from being in an infinitive loop.</p></sec></sec><sec id="s5"><title>5. Summaryand Conclusion</title><p>In this paper, we considered a deterministic Gaussian extended target with Gaussian clutter case for our experiments. The transmitted waveform optimization is done by maximizing the signal to noise ratio and mutual information between the target frequency responses of different targets and the received signal. This helps achieve a better performance in target recognition. We derived different MI-based, SNR-based and TSF waveforms and used an approximate analytical expression for the probability of detection for different waveforms and compared the performance of these waveforms based on this idea. The remarkable features for designing these waveforms for deterministic extended targets, are energy allocation in which waveforms should allocate their energy into frequency bands where target has the greatest PSD value and clutter has the smallest PSD value. This idea will cause the product of target and transmitted waveform got the maximum amount and then the performance of target detection in the presence of clutter will increase.</p><p>The derivations of MI-based waveforms for deterministic Gaussian extended targets and in the case of Gaussian clutter are new results. Moreover, TSF waveform in signal-dependent interference is a new result derived to show that depending on the application such as deterministic extended target, energy allocation is not done well. In fact for the scenarios outlined in the text, it is better to allocate most of transmitting waveform energy into frequency bands in which target has considerable peak amount and clutter amount is negligible instead of distributing energy into all target spectrum peaks. In this paper, different values of SNR and MI are obtained in different TCR, CNR and TNR amounts and it is proven that the obtained waveforms have various performances in different TCR, CNR and TNR and in cognitive radar. We propose a new closed-loop structure considering all features discussed in this paper and for each scenario of target, clutter and noise intelligently find the optimum solution. This work just uses deterministic Gaussian targets case in Gaussian clutter. Future work will attempt to investigate methods of waveforms designing for stochastic extended targets in Gaussian and non-Gaussian environments and suggest a general method for each clutter and target scenarios.</p></sec><sec id="s6"><title>Cite this paper</title><p>Vahid Karimi,Reza Mohseni,Yaser Norouzi,Mohammad Javad Dehghani, (2016) Waveform Design for Cognitive Radar with Deterministic Extended Targets in the Presence of Clutter. International Journal of Communications, Network and System Sciences,09,250-268. doi: 10.4236/ijcns.2016.96023</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.67687-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Haykin, S. (2006) Cognitive Radar: A Way of the Future. IEEE Signal Processing Magazine, 23, 30-40.  
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