<?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">JSIP</journal-id><journal-title-group><journal-title>Journal of Signal and Information Processing</journal-title></journal-title-group><issn pub-type="epub">2159-4465</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jsip.2012.34058</article-id><article-id pub-id-type="publisher-id">JSIP-24960</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>
 
 
  Union Resolution Performance of Frequency Modulation Parameter Based on RWT for LFM Signals
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>enchen</surname><given-names>Li</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Huimin</surname><given-names>Yang</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>Hong</surname><given-names>Li</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>Mei</surname><given-names>Dan</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>Xuesong</surname><given-names>Wang</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>Shunping</surname><given-names>Xiao</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>School of Electronic Science and Engineering, National University of Defense Technology, Changsha, China</addr-line></aff><aff id="aff1"><addr-line>National Major Laboratory of Complex Electromagnetic Environmental Effects for Electronic Information System, Luoyang, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>leewench@yahoo.com.cn(EL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>11</month><year>2012</year></pub-date><volume>03</volume><issue>04</issue><fpage>457</fpage><lpage>464</lpage><history><date date-type="received"><day>July</day>	<month>22nd,</month>	<year>2012</year></date><date date-type="rev-recd"><day>August</day>	<month>24th,</month>	<year>2012</year>	</date><date date-type="accepted"><day>September</day>	<month>7th,</month>	<year>2012</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>
 
 
  Union resolution performance of FM (frequency modulation) parameter based on Radon-Wigner transform (RWT) for multi-component LFM (linear frequency modulation) signals is studied. Firstly, the RWT output expression is offered, and the independent resolution performances of initial frequency and chirp rate are analyzed. Secondly, the RWT output approximate analytic expression is given based on quadratic Taylor's series expansion, and the contour property is analyzed. Contour can be used to picture the union resolution performance of FM parameter, and 2-D resolution performance is studied based on approximate analytic expression, and the union resolution expression of FM parameter and resolution ellipse are offered. The simulation results validate the union resolution expression, and show that the union resolution can improve the resolution performance of multi-component LFM signals, contrasted with absolute resolution performance. The paper can help the study of LFM parameter estimation and resolution performance.
 
</p></abstract><kwd-group><kwd>Multi-Component LFM Signals; Radon-Wigner Transform (RWT); Resolution Ellipse; Union Resolution of FM Parameter; Half-Power Lobe Width</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The LFM signal is widely applied in domains such as radar, correspondence and sound navigation. LFM signal’s parameter estimation is an important research subject in the electronic intelligence system, target motive parameter estimation and ISAR image. There are many literatures about LFM signal parameter estimation method, such as estimation performance, the operating speed and the application, for example ML (Maximum Likelihood) method [<xref ref-type="bibr" rid="scirp.24960-ref1">1</xref>], polynomial phase transform (PPT) [2,3], Radon-Wigner transform (RWT) or the Wigner-Hough transform (WHT) [4-6], Radon-Ambiguity transform (RAT) [7,8], Fractional Fourier transform (FrFT) [<xref ref-type="bibr" rid="scirp.24960-ref9">9</xref>]. RWT or WHT are the commonly used LFM signal parameter estimation methods. RWT method searches the straight line in the Wigner-Ville time-frequency distribution plane. The cross term can be suppressed effectively through the line integral in RWT, which is used to estimate the initial frequency and chirp rate of LFM signals, ulteriorly, the amplitude and phase information can be estimated.</p><p>The research of RWT resolution for LFM signal is the foundation for multi-component signal separation. And there are quite a few literatures about the RWT resolution. Simulation results in literature [<xref ref-type="bibr" rid="scirp.24960-ref8">8</xref>] show that the RAT chirp rate resolution is <img src="4-3400231\5077172b-5974-4428-a22c-133cd5892597.jpg" /> and <img src="4-3400231\35e23590-4ad6-4697-831d-dffdd570e409.jpg" /> for the square-law and enveloping ambiguity respectively. Literature [<xref ref-type="bibr" rid="scirp.24960-ref10">10</xref>] defines the nominal resolution with the main lobe of 3 dB width (half-power width), Literature [<xref ref-type="bibr" rid="scirp.24960-ref11">11</xref>] indicates the range-velocity union resolution with the ambiguity diagram’s 3/4 interception area. In summary, the resolution definition is disparate in different literatures, and the nominal resolution can reflect the resolution performance on a certain extent, but not accurately.</p><p>The unite resolution of RWT FM parameter (initial frequency and chirp rate) for the multi-component signal is related with SNR (signal to noise ratio), signal form and processing method. Generally the system resolution performance is analyzed under the condition of great SNR and best signal processing, therefore this article analyzes the RWT resolution performance for signal with great SNR. Firstly, the RWT output expression is given, and the independent resolutions of initial frequency and chirp rate are analyzed. Secondly, the RWT output approximate analytic expression is given by Taylor series expansion. The contour line nature is analyzed and the contour line deviation caused by approximation in Taylor expansion is revised. The contour line and two-dimensional resolution have been studied based on the analytic expression. The mathematical expression of FM parameter union resolution and the resolution ellipse area are obtained. Finally, the simulation results indicate that the union resolution of FM parameter is higher than independent resolution.</p></sec><sec id="s2"><title>2. RWT FM Parameter Estimation</title><sec id="s2_1"><title>2.1. LFM Signal Model</title><p>Single LFM signal model is expressed by:</p><disp-formula id="scirp.24960-formula95540"><label>(1)</label><graphic position="anchor" xlink:href="4-3400231\4e4c3ed3-bbd7-441d-8ccc-4c8528216e4a.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-3400231\f024d402-5ad5-4a21-ac12-23d0ab42eb4a.jpg" />,<img src="4-3400231\e0ab9920-52bb-4579-9244-5cca15428153.jpg" /> are the signal scope, the phase, the initial angular frequency (or initial frequency) and the angle FM rate (or chirp rate) respectively. <img src="4-3400231\e31a8181-6881-46df-993f-2410611e1874.jpg" />is gauss white noise, whose mean is zero and variance is<img src="4-3400231\07a3967d-946b-4cc1-bc76-e9797550b951.jpg" />.</p></sec><sec id="s2_2"><title>2.2. RWT of LFM Signal</title><p>The essence of Radon transformation is to transform the straight line to the point in plane through the rotation axis projection integral, and a point coordinate corresponds the straight line slope and the slant range, then the detection and estimation are carried in this parameter spatial domain. RWT method transform the LFM signal from the time domain to the parameter spatial domain including the initial frequency and the FM rate.</p><p>The Wigner-Ville distribution [<xref ref-type="bibr" rid="scirp.24960-ref5">5</xref>] of <img src="4-3400231\79b75c32-709e-42d8-a874-95f49879138f.jpg" /> is</p><disp-formula id="scirp.24960-formula95541"><label>(2)</label><graphic position="anchor" xlink:href="4-3400231\b9d88e40-f67e-4ce1-9a10-030232af58e5.jpg"  xlink:type="simple"/></disp-formula><p>LFM signal chirp rate<img src="4-3400231\d73c7a46-47ce-4f35-836e-6b5c463552b1.jpg" />, <img src="4-3400231\c652e846-b1f6-4fd2-bb6c-9bde905faf0b.jpg" />axis intercept<img src="4-3400231\9ab605a8-68dc-4438-a268-0cd4f40216ac.jpg" />, viz. initial frequency of<img src="4-3400231\c4a376da-7289-4503-915b-a2a4846d000e.jpg" />.</p><p>According to the Wigner-Ville distribution characteristic of LFM signal, Radon straight line integral transformation is expressed by the straight line slope <img src="4-3400231\4fc012a9-d964-47e0-b902-2e8123ffa94e.jpg" /> and the axis intercept<img src="4-3400231\778729eb-4739-4990-bf7a-dc1efd1bc79d.jpg" />, the integral is done along the line<img src="4-3400231\36ee3c6d-5acd-42ab-a3e8-b6f2e1add4e8.jpg" />. Then the signal is transformed from time domain to the parameter spatial domain composed by initial frequency h and chirp rate K. The scheme of Radon transformation is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The RWT formula is expressed by:</p><disp-formula id="scirp.24960-formula95542"><label>(3)</label><graphic position="anchor" xlink:href="4-3400231\26fbd7d5-2528-4565-8864-54e48b83a49b.jpg"  xlink:type="simple"/></disp-formula><p>Using the integration variable replacement [<xref ref-type="bibr" rid="scirp.24960-ref12">12</xref>], the formula can be transformed into:</p><disp-formula id="scirp.24960-formula95543"><label>(4)</label><graphic position="anchor" xlink:href="4-3400231\b192605f-cf87-4c49-b7de-e7f6693ceec8.jpg"  xlink:type="simple"/></disp-formula><p>Namely the two-dimensional integral of RWT modeling can be transformed to the power spectrum estimation</p><p>of the time domain dechirp signal [<xref ref-type="bibr" rid="scirp.24960-ref13">13</xref>]. And the best estimation of <img src="4-3400231\17f92338-fefa-497c-87a6-455bc5d37884.jpg" /> may be determined by the maximum value position of<img src="4-3400231\f815394b-5587-4385-b6f5-c803d3a44740.jpg" />, and obtain the estimation value <img src="4-3400231\4a1abc00-94aa-4c4a-b1e8-c1ec1d2695fb.jpg" /> of <img src="4-3400231\c5e9dea3-d19a-47c9-b388-c1fcb1f6c89d.jpg" /> by the <img src="4-3400231\5a95cec6-f6db-475a-858b-231e5fc9f467.jpg" /> parameter estimation.</p></sec></sec><sec id="s3"><title>3. RWT Resolution of Initial Frequency and Chirp Rate</title><p>From formula (4), the RWT output of the noise-free LFM signal model <img src="4-3400231\aac58246-d608-461a-a7c4-f4d0e44267a8.jpg" /> is expressed by:</p><disp-formula id="scirp.24960-formula95544"><label>(5)</label><graphic position="anchor" xlink:href="4-3400231\a41b2784-c895-410d-977b-87f60cac0f4f.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.24960-formula95545"><label>(6)</label><graphic position="anchor" xlink:href="4-3400231\6affb44b-fe1c-4647-a2c2-bb7a85e6aea2.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95546"><label>(7)</label><graphic position="anchor" xlink:href="4-3400231\1740c4f5-e30d-46f4-b6bb-bccdc2a25152.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95547"><label>(8)</label><graphic position="anchor" xlink:href="4-3400231\020f2a4d-c02d-43bb-a5b8-06b3af4cfbd5.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95548"><label>(9)</label><graphic position="anchor" xlink:href="4-3400231\d994e5a7-e208-4e0a-81ec-b7743073b342.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-3400231\2ec80449-88d3-40d0-b1e3-6057e6efa306.jpg" />, <img src="4-3400231\7c91957c-da38-432f-ba2f-92785b7e1d6d.jpg" />is Fresnel cosine integral and <img src="4-3400231\a1403a11-079f-4a52-b8b4-25f7d558339b.jpg" /> is Fresnel sine integral [<xref ref-type="bibr" rid="scirp.24960-ref12">12</xref>]. <img src="4-3400231\677688d1-fa5e-4ae2-a039-0ff433aa6356.jpg" />when<img src="4-3400231\d87f9be4-6cff-49e0-a71f-decf9790c644.jpg" />,<img src="4-3400231\d8c536ce-7475-4c90-8866-b898bc802f46.jpg" />. The half-power lobe width of the RWT output function, that is<img src="4-3400231\6326261e-048e-40b4-8532-4fcc0b23b29f.jpg" />, is shown in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p><p>• When <img src="4-3400231\043b4548-45c4-4535-af88-a0c901898995.jpg" /></p><p><img src="4-3400231\0b111144-cff1-4ef4-b0a6-345473e4832f.jpg" />is obtained via interpolation method from <img src="4-3400231\e8ac1ea4-4091-438a-92cf-9e884ad2da2f.jpg" /> in <xref ref-type="fig" rid="fig2">Figure 2</xref>(a). The half-power lobe width of <img src="4-3400231\13411598-6868-4e06-8a48-f5c078bcd145.jpg" /> is:</p><disp-formula id="scirp.24960-formula95549"><label>(10)</label><graphic position="anchor" xlink:href="4-3400231\a10d7a54-7a7f-41ca-84c7-96a093ceeaa1.jpg"  xlink:type="simple"/></disp-formula><p>• When <img src="4-3400231\b6d79204-68cf-4816-8b86-cdbc80168d3e.jpg" /></p><p>Using<img src="4-3400231\f1ee5535-bd9f-4231-9273-9a5b0654c089.jpg" />, obtains:</p><disp-formula id="scirp.24960-formula95550"><label>(11)</label><graphic position="anchor" xlink:href="4-3400231\8465f8f7-bf77-469e-bd7f-ae2c0030bb03.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-3400231\674d328d-ea0a-4d65-8602-3764bbccdf16.jpg" />.<img src="4-3400231\7e989ec5-0b79-4646-a102-95448ff6338e.jpg" /> is obtained via interpolation method from <img src="4-3400231\a5a1a353-4e80-4d59-8f26-4ba09fee74a5.jpg" /> in <xref ref-type="fig" rid="fig2">Figure 2</xref>(b). The half-power lobe width of <img src="4-3400231\6373a462-4fd9-4147-a690-bd33152fb7f4.jpg" /> is:</p><disp-formula id="scirp.24960-formula95551"><label>(12)</label><graphic position="anchor" xlink:href="4-3400231\36b85da6-e777-4330-a90d-7fb948c33c84.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Taylor Formula and Character of the RWT Function</title><sec id="s4_1"><title>4.1. Taylor Formula of the RWT Function</title><p>The RWT function’s main lobe reflects the RWT union resolution of initial frequency and chirp rate. In order to</p><p>obtain the main lobe analytic expression in the different high, the RWT function is indicated with the quadratic Taylor series expansion on the point with maximum value, which is <img src="4-3400231\bcbdfc9e-ed97-4bb7-9ebb-153c1667dd79.jpg" /> and<img src="4-3400231\1c7fcf80-e3e7-4617-8739-b5f01f23c2e4.jpg" />. The Taylor expansion of <img src="4-3400231\9241127a-28dd-4312-b067-9318d29b9a0e.jpg" /> is quite complex, so this article directly calculates the quadratic Taylor series of RWT output on the maximum value using the expression of<img src="4-3400231\6bc332f9-655e-48d8-a4e9-9b66d7a5ca06.jpg" />. The quadratic Taylor formula is expressed by [<xref ref-type="bibr" rid="scirp.24960-ref12">12</xref>]:</p><disp-formula id="scirp.24960-formula95552"><label>(13)</label><graphic position="anchor" xlink:href="4-3400231\161695db-8e48-4d5c-9386-2a3237a84c42.jpg"  xlink:type="simple"/></disp-formula><p>From formula (4), when the noise-free input signal model is<img src="4-3400231\4a9626d1-9747-4012-b40b-a91465c95ce4.jpg" />, <img src="4-3400231\fe0f2a0b-0cb6-474b-80ae-b1a060bbc2ae.jpg" />, the RWT function is:</p><disp-formula id="scirp.24960-formula95553"><label>(14)</label><graphic position="anchor" xlink:href="4-3400231\1568631a-573d-4bcb-b3e1-fc21fb908d36.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.24960-formula95554"><label>(15)</label><graphic position="anchor" xlink:href="4-3400231\6330212a-6a1e-44a6-a4cc-ed06c8e27fc8.jpg"  xlink:type="simple"/></disp-formula><p>Via<img src="4-3400231\f355b09b-46fb-4c00-ab64-cfb090272a2a.jpg" />,</p><p><img src="4-3400231\305173e1-a5bb-4dfe-97eb-22ae5a056f25.jpg" />,</p><p><img src="4-3400231\63f78dd6-5f76-4228-b2a3-61ab58a7adf3.jpg" />,</p><p><img src="4-3400231\14d22bd8-04e1-4a58-924d-c7968fb8031c.jpg" />,</p><p><img src="4-3400231\e39c276f-304a-4916-be6e-c92a48e7649c.jpg" />,</p><p><img src="4-3400231\22f9246e-7b49-45cc-a2dc-c99dc03cf422.jpg" />obtains these item in formula (13) as follows:</p><disp-formula id="scirp.24960-formula95555"><label>(16)</label><graphic position="anchor" xlink:href="4-3400231\3c2c9522-421f-4f29-989c-4af221cbc636.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95556"><label>(17)</label><graphic position="anchor" xlink:href="4-3400231\a0e0d29a-2a6f-4ae5-a9f4-e95b90226565.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95557"><label>(18)</label><graphic position="anchor" xlink:href="4-3400231\65ef8046-8ec9-41ad-8cd4-070d16770db2.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95558"><label>(19)</label><graphic position="anchor" xlink:href="4-3400231\eea4dd11-d979-4e10-b9b3-e507aeaf6307.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95559"><label>(20)</label><graphic position="anchor" xlink:href="4-3400231\21bbb6c9-5eba-4688-8e49-dfa6632e696d.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95560"><label>(21)</label><graphic position="anchor" xlink:href="4-3400231\567ecac8-bba3-4215-a1c7-e93790d7c6c4.jpg"  xlink:type="simple"/></disp-formula><p>Taylor formula (13) is transformed into:</p><disp-formula id="scirp.24960-formula95561"><label>(22)</label><graphic position="anchor" xlink:href="4-3400231\6e7ad697-e7c1-4169-99c9-8d0cb212adb2.jpg"  xlink:type="simple"/></disp-formula><p>Obviously the RWT output is nonstandard quadratic surface, which can be proved to be nonstandard ellipse paraboloid.</p></sec><sec id="s4_2"><title>4.2. The Contour Line Parameter Analysis of the Quadratic Taylor Formula</title><p>The RWT output is two-dimensional function of initial frequency and chirp rate, and the greatest value is<img src="4-3400231\bdd1e88e-6c16-4ecf-b802-e8fce76fddc8.jpg" />. The lobe characteristic of the RWT output function is reflected by the contour line along <img src="4-3400231\f0bf8512-7355-4e58-8ea7-ef555c96fad7.jpg" /> and the cutting coefficient of contour line is<img src="4-3400231\e295f159-2e7f-466b-b894-4909d5438be1.jpg" />. The output result is not the standard analytic expression, therefore the RWT cutting contour line is indicated by the quadratic Taylor formula, as follows:</p><disp-formula id="scirp.24960-formula95562"><label>(23)</label><graphic position="anchor" xlink:href="4-3400231\3ac9dc26-fff7-4cf7-a75a-1ebb42b916f6.jpg"  xlink:type="simple"/></disp-formula><p>Substitutes the quadratic Taylor formula, obtains:</p><disp-formula id="scirp.24960-formula95563"><label>(24)</label><graphic position="anchor" xlink:href="4-3400231\caf6f6b7-6a98-4a4c-b0bb-a2c8fffa4b1d.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.24960-formula95564"><label>(25)</label><graphic position="anchor" xlink:href="4-3400231\f3e61e5b-ae62-4497-a335-f2cbe61f57f9.jpg"  xlink:type="simple"/></disp-formula><p>Using <img src="4-3400231\9b2b8209-4603-4ff4-b453-42b5ebd7f1c4.jpg" /> as the center, and prescribing counterclockwise is positive, the coordinate system</p><p><img src="4-3400231\3cc21684-991d-4c80-9dad-fb4b523c1153.jpg" />is counter-clockwise rotated with angle<img src="4-3400231\a8522e6a-c3a1-4a05-b677-cc555868a063.jpg" />, and the coordinate system <img src="4-3400231\e58b02d6-cb79-4023-9194-616c2a1d30f2.jpg" /> is obtained, shown in <xref ref-type="fig" rid="fig3">Figure 3</xref>.</p><disp-formula id="scirp.24960-formula95565"><label>(26)</label><graphic position="anchor" xlink:href="4-3400231\abb6afa9-7195-4356-bc9d-c0d120f9e928.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95566"><label>(27)</label><graphic position="anchor" xlink:href="4-3400231\abfc9c10-3ef6-4765-821d-65681235fa1b.jpg"  xlink:type="simple"/></disp-formula><p>In the coordinate system<img src="4-3400231\be68c919-200c-443d-a0fb-d0a93678b844.jpg" />, Equation (24) transforms into:</p><disp-formula id="scirp.24960-formula95567"><label>(28)</label><graphic position="anchor" xlink:href="4-3400231\1cb7421b-ecb9-406d-a0ec-c9edf38e2017.jpg"  xlink:type="simple"/></disp-formula><p>when the item of <img src="4-3400231\dbbc6711-ade4-44df-b589-562e608d610d.jpg" /> is zero, the equation is standard ellipse, and obtains</p><disp-formula id="scirp.24960-formula95568"><label>(29)</label><graphic position="anchor" xlink:href="4-3400231\24364eaa-8b98-4f1a-88c8-6e413603d1c8.jpg"  xlink:type="simple"/></disp-formula><p>And formula (28) is simplified to</p><disp-formula id="scirp.24960-formula95569"><label>(30)</label><graphic position="anchor" xlink:href="4-3400231\a7bd65da-c5b0-41f2-9ebc-76ed9bbf7da0.jpg"  xlink:type="simple"/></disp-formula><p>It can be proved that the equation coefficient is more than zero, that is</p><disp-formula id="scirp.24960-formula95570"><label>(31)</label><graphic position="anchor" xlink:href="4-3400231\0e961a53-d87d-4b1c-86fc-dd5afbc161ae.jpg"  xlink:type="simple"/></disp-formula><p>Therefore, the equation is the elliptic equation, the RWT quadratic surface is nonstandard ellipse paraboloid.</p></sec><sec id="s4_3"><title>4.3. Contrastive Analysis of Quadratic Taylor Formula and Actual Contour Line</title><p>In order to analyze conveniently, the performance of</p><p>RWT resolution is characterized by half-power lobe width in this article. The half-power lobe contour line, which is obtained by quadratic Taylor formula, is the RWT output amplitude<img src="4-3400231\75b505c4-cc07-4ac1-9bcd-563769e29a49.jpg" />. By</p><p><img src="4-3400231\88461295-7d59-4f98-8a1b-8c1515785301.jpg" />, the half-power lobe width of <img src="4-3400231\79cb0189-828c-41c0-af0d-34be6f9298c5.jpg" /> is:</p><disp-formula id="scirp.24960-formula95571"><label>(32)</label><graphic position="anchor" xlink:href="4-3400231\0293823b-9e09-4bdc-a9d3-8f0dbb9e6fd6.jpg"  xlink:type="simple"/></disp-formula><p>By<img src="4-3400231\2c1bdff4-2484-4357-a1f7-7e1764d2d1aa.jpg" />, the half-power lobe width of <img src="4-3400231\9b54fe7c-6500-49b4-b92f-41f5611d9fce.jpg" /> is:</p><disp-formula id="scirp.24960-formula95572"><label>(33)</label><graphic position="anchor" xlink:href="4-3400231\948304ac-ade4-4070-81f5-e09208e4ac61.jpg"  xlink:type="simple"/></disp-formula><p>The result is close with the half-power lobe width <img src="4-3400231\129955f0-ea84-4c10-a3dc-49d677c999bf.jpg" /> and<img src="4-3400231\2e27a8d8-48ce-4431-bf6d-0b55b3e692d9.jpg" />, which is obtained directly by curve simulation and interpolation. There are two main error sources: The one is abbreviate of higher item, the other is cutting departure from the spot with maximum value. The half-power lobe width of the actual RWT output can be approached by adjustment the parameter<img src="4-3400231\881ae981-cb67-40f3-ab2d-b21bcffb3b9e.jpg" />, and the best revision interception coefficient <img src="4-3400231\a4df5b7f-aeef-4228-9d3f-05c116013303.jpg" /> is:</p><disp-formula id="scirp.24960-formula95573"><label>(34)</label><graphic position="anchor" xlink:href="4-3400231\76e364eb-c92e-4b51-850c-14384e3bf5a3.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-3400231\4df4d446-21d3-40cf-87bf-dc32669e7090.jpg" /> are obtained separately by the half-power lobe width of h, K, the expression is expressed as follows:</p><disp-formula id="scirp.24960-formula95574"><label>(35)</label><graphic position="anchor" xlink:href="4-3400231\ac95e5f5-8ff7-4c34-b206-e11f84b71934.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24960-formula95575"><label>(36)</label><graphic position="anchor" xlink:href="4-3400231\99f74b0c-5d61-41b8-8bc3-d221dcdc2880.jpg"  xlink:type="simple"/></disp-formula><p>Namely, when<img src="4-3400231\41ef75a4-2801-4ef4-9836-8e8b3330ed93.jpg" />, the lobe width using the quadratic Taylor formula is able to approach the actual RWT output half-power lobe width, which is proved by the simulation result.</p></sec></sec><sec id="s5"><title>5. RWT Union Resolution of Initial Frequency and Chirp Rate</title><p>The signal resolution is analyzed usually by two signals with equi-signal length, amplitude and initial time. The multi-component signal amplitude is<img src="4-3400231\41ba6f72-9577-400a-a6d1-f41875df2254.jpg" />, the length is<img src="4-3400231\51d97e96-7388-4c8f-bc31-b18baa69314e.jpg" />, namely <img src="4-3400231\328f1425-bca6-48fb-8f2e-cbdfc5bb2aef.jpg" /> are the constants, the signal position is<img src="4-3400231\2d1849c8-7614-4550-b4f0-fea373b0b707.jpg" />, the <img src="4-3400231\9a5f332b-0459-4ff3-9a88-dff51a6e3778.jpg" />th component signal’s initial frequency is <img src="4-3400231\32effd99-c6d8-44c5-8624-952aeb286e55.jpg" /> and chirp rate respectively is<img src="4-3400231\6e1abfad-b53f-4a4d-a96b-993d20257fe5.jpg" />, its half-power cutting contour line is:</p><disp-formula id="scirp.24960-formula95576"><label>(37)</label><graphic position="anchor" xlink:href="4-3400231\d9233ad1-ad0b-46e7-bc6c-873c8027f850.jpg"  xlink:type="simple"/></disp-formula><p>This formula can be reduced to:</p><disp-formula id="scirp.24960-formula95577"><label>(38)</label><graphic position="anchor" xlink:href="4-3400231\a3fa98a2-7e79-4bc1-8e3f-911a62fa25c4.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.24960-formula95578"><label>(39)</label><graphic position="anchor" xlink:href="4-3400231\58456bae-58db-4a4b-a371-9ccfaf95683e.jpg"  xlink:type="simple"/></disp-formula><p>Defines</p><disp-formula id="scirp.24960-formula95579"><label>(40)</label><graphic position="anchor" xlink:href="4-3400231\630ab97e-5018-408e-bff0-f943dc21b19c.jpg"  xlink:type="simple"/></disp-formula><p>Obtains</p><disp-formula id="scirp.24960-formula95580"><label>(41)</label><graphic position="anchor" xlink:href="4-3400231\315d3c2e-7910-4a88-9ad1-96f239cc7f24.jpg"  xlink:type="simple"/></disp-formula><p>Therefore <img src="4-3400231\52328f38-6f82-4835-93c7-f0f605ffb6b9.jpg" /> and <img src="4-3400231\3e990163-6bfe-4938-bf34-bb7efc2c71ca.jpg" /> both have corresponding relationships, formula (37) in coordinate system <img src="4-3400231\5729c16f-4e63-4342-a45b-2f62813bc334.jpg" /> is circle equation.</p><disp-formula id="scirp.24960-formula95581"><label>(42)</label><graphic position="anchor" xlink:href="4-3400231\aa905193-3c49-4715-9176-1a3b46febde8.jpg"  xlink:type="simple"/></disp-formula><p>where, the circle point of the <img src="4-3400231\139cc0a0-4068-46bf-be2b-c41a908a07eb.jpg" />th component signal in coordinate system <img src="4-3400231\ee91218b-f7ea-4cfc-8d07-1750e7e21675.jpg" /> is<img src="4-3400231\764d0eb2-c5ab-4b65-ab3f-58317f29be73.jpg" />, <img src="4-3400231\d77d17b5-eda8-4c1b-a5b1-5c2815151166.jpg" />, and the circle track data can be generated by the circle equation, from which, we can get the corresponding contour line data <img src="4-3400231\6ecec84d-6daf-41d2-95b7-97e806b209d6.jpg" /> after the coordinate system conversion.</p><p>The two component signal’s FM parameters are<img src="4-3400231\9243d191-29ce-48f5-8047-498854991849.jpg" />, <img src="4-3400231\3163ce21-3c3f-4a74-925a-c00e3ddfa980.jpg" />respectively. According to the nominal resolution, two signals can not be distinguished if half-power contour lines have the intersection point in the coordinate system<img src="4-3400231\c98bbc04-dbc8-4759-8948-e0e3d97c96b8.jpg" />, otherwise two signals are distinguishable. In the coordinate system<img src="4-3400231\c412f524-e3bc-44ae-8570-f85f17cc8f04.jpg" />, the contour line is circle. So long as the central distances of two circles are more than 2, the two LFM signals can be distinguished. The condition is described by:</p><disp-formula id="scirp.24960-formula95582"><label>(43)</label><graphic position="anchor" xlink:href="4-3400231\7ec78f82-4d1d-45f0-ac65-783302937311.jpg"  xlink:type="simple"/></disp-formula><p>Inputting<img src="4-3400231\cf79239e-9a12-40ac-a43e-70137f452b0f.jpg" />, the formula can be reduced to:</p><disp-formula id="scirp.24960-formula95583"><label>(44)</label><graphic position="anchor" xlink:href="4-3400231\6e4253a7-5bba-4458-a6c7-2078118f0634.jpg"  xlink:type="simple"/></disp-formula><p>Inputting<img src="4-3400231\dae8b8e2-ec06-471f-a010-efd552b4a646.jpg" />, the resolution expression based on parameter is</p><disp-formula id="scirp.24960-formula95584"><label>(45)</label><graphic position="anchor" xlink:href="4-3400231\7698c36a-9b39-440f-b06c-f71bd7756e95.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-3400231\c73246db-3f77-47e0-9042-ddf3f31e0f9c.jpg" />, and multi-component signal is able to be resolved, so long as the position of FM parameter<img src="4-3400231\a23ea274-9572-4527-a122-c30bb5c5a3dc.jpg" />, <img src="4-3400231\63e2ee79-179f-4c68-b20a-8e2295bd3b42.jpg" />satisfies the above equation. Obviously in order to achieve the high resolution of initial frequency and chirp rate, the time length must be increased.</p><p>The union resolution of initial frequency and chirp rate may be indicated by the interception ellipse area.</p><disp-formula id="scirp.24960-formula95585"><label>(46)</label><graphic position="anchor" xlink:href="4-3400231\8c3c9b91-aa3e-4a34-a997-2426828f6a98.jpg"  xlink:type="simple"/></disp-formula><p>Obviously the resolution ellipse’s area is in reverse proportion with<img src="4-3400231\7d1d8302-bef1-457f-b420-e744f0e1c8d2.jpg" />, related with the interception coefficient<img src="4-3400231\2e512636-463f-444c-b4b8-cdc38a9b9d15.jpg" />.</p></sec><sec id="s6"><title>6. Simulation Results</title><sec id="s6_1"><title>6.1. The RWT Output of Single Component LFM Signal</title><p>The signal model is:</p><disp-formula id="scirp.24960-formula95586"><label>(47)</label><graphic position="anchor" xlink:href="4-3400231\271a69cd-8819-462e-a93f-013effe9ad44.jpg"  xlink:type="simple"/></disp-formula><p>The digital simulation result is given in <xref ref-type="fig" rid="fig4">Figure 4</xref>, where<img src="4-3400231\8a6c7837-37fb-48a4-847e-f9a9e5eec476.jpg" />, <img src="4-3400231\1b92dcee-7c0e-4161-90b3-210cb80c2a42.jpg" />, namely a = 0.5334, b = 0.2754, c = 0.2845, and the FM parameter sampling interval is quite small in order to study the fine characteristic of RWT output. <xref ref-type="fig" rid="fig4">Figure 4</xref>(a) is the contrast of RWT half-power contour line and the Taylor’s expansion contour line in<img src="4-3400231\9857fe5b-434a-482c-90d3-77c024afcad1.jpg" />. <xref ref-type="fig" rid="fig4">Figure 4</xref>(b) is the contour line view. It is indicated that the contour line two-dimensional superposition is very good for the two methods, therefore the RWT output half-power contour line is described well by the contour line equation in<img src="4-3400231\da807f93-78e7-4d63-a924-c5241addf7ea.jpg" />. The results indicate simultaneously that the FM parameter estimation error is very small for a single component noise-free LFM signal.</p></sec><sec id="s6_2"><title>6.2. The RWT of Multi Component LFM Signal</title><p>The signal model is:</p><disp-formula id="scirp.24960-formula95587"><label>(48)</label><graphic position="anchor" xlink:href="4-3400231\cb1a960f-3ec8-4e53-ac38-10f5735c2e42.jpg"  xlink:type="simple"/></disp-formula><p>The signal length is 1s, initial frequency independent resolution is<img src="4-3400231\487ad4c6-f864-42d5-a69c-080954be06dc.jpg" />, chirp rate independent resolution is<img src="4-3400231\05f6dfc7-8a1b-4830-8589-6f2511209c96.jpg" />. The first component is:</p><disp-formula id="scirp.24960-formula95588"><label>(49)</label><graphic position="anchor" xlink:href="4-3400231\52142166-c04a-4d6f-ae65-d3d7088daf26.jpg"  xlink:type="simple"/></disp-formula><p>The second component is:</p><disp-formula id="scirp.24960-formula95589"><label>(50)</label><graphic position="anchor" xlink:href="4-3400231\2e6776ac-bf0d-46e0-91df-36e243496f36.jpg"  xlink:type="simple"/></disp-formula><p>The RWT resolution performance of two component LFM signals is studied by changing the initial frequency and chirp rate of the second component separately in</p><p>what follows.</p><sec id="s6_2_1"><title>6.2.1. Independent Resolution of Initial Frequency and Chirp Rate</title><p>The simulation results of initial frequency and chirp rate independent resolution are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>, including contour map and projection view. Two LFM signals with same chirp rate and different initial frequency (<img src="4-3400231\95680197-95a6-4a8e-9ba3-046c36771cd2.jpg" />,<img src="4-3400231\f5005808-5824-4f88-be55-13914656f8f3.jpg" />) are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(a). Two LFM signals with same initial frequency and different chirp rate (<img src="4-3400231\19ea73dc-06ff-41df-b242-d111be370481.jpg" />,<img src="4-3400231\438f9d23-3c0e-48c7-bd8b-1870c2cd2e6a.jpg" />) are shown in <xref ref-type="fig" rid="fig5">Figure 5</xref>(b). Obviously in the RWT output two-dimensional surface of initial frequency and chirp rate, the mutual</p><p>coupling of the very near two LFM signals cause the RWT output peak position to be away from the primary position, which incurs FM parameter estimation deviation. Simultaneously the further simulation results indicate that the different phase item <img src="4-3400231\baa28748-3bf5-43ad-a50b-5a47bf4621f5.jpg" /> in the two LFM signals causes the different peak position errors, and the starting phase items of the two LFM signals affect the parameter estimation errors, but the LFM signals are distinguishable if the distinguishing condition is satisfied. Therefore the nominal resolution reflects the resolution performance to a certain extent. For single component LFM signal or multi-component LFM signal with the great FM parameter space interval in RWT, the RWT</p><p>parameter estimation error is related with SNR input. On the other hand, for the distinguishable multi-component LFM signal with the close FM parameter space interval, FM parameter estimation error is related with both SNR and other component signal’s parameter.</p></sec><sec id="s6_2_2"><title>6.2.2. Union Resolution of Initial Frequency and Chirp Rate</title><p>Union resolution of multi-component LFM signal is studied and simulation results are shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>, including contour map and projection view. (a) The second component<img src="4-3400231\931cd5c2-1e0d-4b7c-ae72-20ab86164f5d.jpg" />, <img src="4-3400231\26d19060-728d-4145-b764-6fada6f52a78.jpg" />, and the signals cannot be distinguished by RWT method; (b) The second component<img src="4-3400231\8b48142c-79d3-44bf-a7d4-bf8a5a23a856.jpg" />, <img src="4-3400231\1f88105e-a160-4921-88e1-8fd5a2e895a8.jpg" />, and the signals cannot be distinguished by RWT method; (c) The second components with the initial frequency and chirp rate are all half of independent resolution, namely <img src="4-3400231\7adb3a66-fb90-429c-aa33-be32eac086e7.jpg" /> and<img src="4-3400231\f7686f61-d2ef-45dc-861c-c1ef4d60628e.jpg" />. It is obviously the two LFM signals are distinguishable by RWT method. The simulation results confirm the superiority of the FM parameter union resolution.</p><p>As to two multi-component signals with close FM parameter space, the estimation error is big when the amplitudes are similar, and the optimum parameter estimation of various components can be obtained by Relax iteration method [<xref ref-type="bibr" rid="scirp.24960-ref14">14</xref>]. On the other hand, if the intensity difference of two signals is distinct, the strong signal suppresses the weak signal, therefore the CLEAN technology must be used to extract the signals [<xref ref-type="bibr" rid="scirp.24960-ref15">15</xref>].</p></sec></sec></sec><sec id="s7"><title>7. Conclusion</title><p>Union resolution performance of FM parameter based on RWT for multi-component LFM signals is studied in this paper. Firstly, the RWT output expression is given, and the independent resolutions of initial frequency and chirp rate are analyzed. Secondly, the RWT output approximate analytic expression is given by Taylor series expansion. The contour line property is analyzed and the contour line is deviation, which caused by approximation in Taylor expansion, is revised. Contour can be used to picture the union resolution performance of FM parameter of RWT, and 2-D resolution performance is studied based on approximate analytic expression. The union resolution expression of FM parameter and resolution ellipse area is offered. Finally the simulation results indicate that the union resolution of FM parameter is higher than independent resolution. The research in this paper can help the study of LFM parameter estimation and resolution performance.</p></sec><sec id="s8"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.24960-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">T. J. Abatzoglou, “Fast Maximum Likelihood Joint Estimation of Frequency and Frequency Rate,” IEEE Transactions on Aerospace and Electronic Systems, Vol. 22, No. 6, 1986, pp. 708-715.</mixed-citation></ref><ref id="scirp.24960-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">S. Peleg and B. Porat, “Linear FM Signal Parameter Estimation from Discrete-Time Observations,” IEEE Transactions on Aerospace and Electronic Systems, Vol. 27, No. 4, 1991, pp. 607-615. doi:10.1109/7.85033</mixed-citation></ref><ref id="scirp.24960-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">S. Peleg and B. Porat, “Estimation and Classification of Polynomial Phase Signals,” IEEE Transactions on Information Theory, Vol. 37, No. 2, 1991, pp. 423-430. 
doi:10.1109/18.75269</mixed-citation></ref><ref id="scirp.24960-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">J. C. Wood and D. T. Barry, “Radon Transformation of Time-Frequency Distributions for Analysis of Multi-Component Signals,” IEEE Transactions on Signal Processing, Vol. 42, No. 11, 1994, pp. 3166-3177. 
doi:10.1109/78.330375</mixed-citation></ref><ref id="scirp.24960-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">J. C. Wood and D. T. Barry, “Linear Signal Synthesis Using the Radon-Wigner Transform,” IEEE Transactions on Signal Processing, Vol. 42, No. 8, 1994, pp. 2105-2111. doi:10.1109/78.301845</mixed-citation></ref><ref id="scirp.24960-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">S. Barbarossa, “Analysis of Multi-Component LFM Signals by a Combined Wigner-Hough Transform,” IEEE Transactions on Signal Processing, Vol. 43, No. 6, 1995, pp. 1511-1515. doi:10.1109/78.388866</mixed-citation></ref><ref id="scirp.24960-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">M. S. Wang, A. K. Chan and C. K. Chui, “Linear Frequency-Modulated Signal Detection Using Radon-Ambiguity Transform,” IEEE Transactions on Signal Processing, Vol. 46, No. 3, 1998, pp. 571-586. 
doi:10.1109/78.661326</mixed-citation></ref><ref id="scirp.24960-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">W. C. Li, M. Dan, X. S. Wang, D. Li and G. Y. Wang, “Fast Estimation Method and Performance Analysis of Frequency Modulation Rate via RAT,” International Conference on Information and Automation, Changsha, China, 20-23 June 2008, pp. 144-147. 
doi:10.1109/ICINFA.2008.4607984</mixed-citation></ref><ref id="scirp.24960-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">L. B. Almeida, “The Fractional Fourier Transforms and Time-Frequency Representations,” IEEE Transactions on Signal Processing, Vol. 42, No. 11, 1994, pp. 3084-3091. 
doi:10.1109/78.330368</mixed-citation></ref><ref id="scirp.24960-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">M. I. Skolnik, “Radar Handbook,” 2nd Edition, McGraw-Hill Publishing Company, New York, 1990.</mixed-citation></ref><ref id="scirp.24960-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">A. W. Rihaczek, “Principles of High-Resolution Radar,” McGraw-Hill Publishing Company, New York, 1969.</mixed-citation></ref><ref id="scirp.24960-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">“Mathematics Handbook,” Higher Education Publishing Company, Beijing, 2004.</mixed-citation></ref><ref id="scirp.24960-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">W. P. Li, “Wigner Distribution Method Equivalent to Dechirp Method for Detecting a Chirp Signal,” IEEE Transactions on Acoustics, Speech, Signal Processing, Vol. 35, No. 8, 1987, pp. 1210-1211.</mixed-citation></ref><ref id="scirp.24960-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">Y. M. Zheng and Z. Bao, “Autofocusing of SAR Images Based on Relax,” IEEE International Radar Conference, Alexandria, 7-12 May 2000, pp. 533-538. 
doi:10.1109/RADAR.2000.851890</mixed-citation></ref><ref id="scirp.24960-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">J. Tsao and B. D. Steinberg, “Reduction of Side Lobe and Speckle Artifacts in Microwave Imaging: The CLEAN Technique,” IEEE Transactions on Antennas and Propagation, Vol. 36, No. 4, 1988, pp. 543-556. 
doi:10.1109/8.1144</mixed-citation></ref></ref-list></back></article>