<?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.2016.71006</article-id><article-id pub-id-type="publisher-id">JSIP-63986</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>
 
 
  Sparse Representation by Frames with Signal Analysis
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hristopher</surname><given-names>Baker</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of EE &amp;amp; CS, University of Wisconsin-Milwaukee, Milwaukee, WI, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>cabaker2@uwm.edu</email></corresp></author-notes><pub-date pub-type="epub"><day>15</day><month>02</month><year>2016</year></pub-date><volume>07</volume><issue>01</issue><fpage>39</fpage><lpage>48</lpage><history><date date-type="received"><day>3</day>	<month>February</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>26</month>	<year>February</year>	</date><date date-type="accepted"><day>29</day>	<month>February</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><html>
 <head></head>
 
  The use of frames is analyzed in Compressed Sensing (CS) through proofs and experiments. First, a new generalized Dictionary-Restricted Isometry Property (D-RIP) sparsity bound constant for CS is established. Second, experiments with a tight frame to analyze sparsity and reconstruction quality using several signal and image types are shown. The constant 
  <img src="Edit_5bc9b7a7-718a-4884-9975-7aab342695fc.bmp" alt="" /> is used in fulfilling the definition of D-RIP. It is proved that k-sparse signals can be reconstructed if 
  <img src="Edit_1e2fb150-c793-49e6-947b-ac2f588f5931.bmp" alt="" /> by using a concise and transparent argument1. The approach could be extended to obtain other D-RIP bounds (i.e. 
  <img src="Edit_794ae530-738b-4ab7-9bc7-ba1c04c602d7.bmp" alt="" />). Experiments contrast results of a Gabor tight frame with Total Variation minimization. In cases of practical interest, the use of a Gabor dictionary performs well when achieving a highly sparse representation and poorly when this sparsity is not achieved.
 
</html></p></abstract><kwd-group><kwd>Compressed Sensing</kwd><kwd> Total Variation Minimization</kwd><kwd> l&lt;sub&gt;1&lt;/sub&gt;-Analysis</kwd><kwd> D-Restricted Isometry Property</kwd><kwd> Tight Frames</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x10.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x11.png" xlink:type="simple"/></inline-formula> be a signal such that</p><disp-formula id="scirp.63986-formula55"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x12.png"  xlink:type="simple"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x13.png" xlink:type="simple"/></inline-formula>. In compressed sensing, one can find a good stable approximation (in terms of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x14.png" xlink:type="simple"/></inline-formula> and the tail of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x15.png" xlink:type="simple"/></inline-formula> consisting of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x16.png" xlink:type="simple"/></inline-formula> smallest entries) of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x17.png" xlink:type="simple"/></inline-formula> from the measurement matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x18.png" xlink:type="simple"/></inline-formula> and the measurement y through solving an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x19.png" xlink:type="simple"/></inline-formula>-minimization, provided that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x20.png" xlink:type="simple"/></inline-formula> belongs to a family of well behaved matrices. A subclass of this family of matrices can be characterized by the well known Restrictive Isometry Property (RIP) of Cand&#232;s, Romberg, and Tao, [<xref ref-type="bibr" rid="scirp.63986-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.63986-ref4">4</xref>] . This property requires the following relation for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x21.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.63986-formula56"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x22.png"  xlink:type="simple"/></disp-formula><p>for every k-sparse vector c (namely, c has at most k non-zero components), for some small constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x23.png" xlink:type="simple"/></inline-formula>. Some bounds on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x24.png" xlink:type="simple"/></inline-formula> have been determined in previous publications [<xref ref-type="bibr" rid="scirp.63986-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.63986-ref6">6</xref>] . Notably, Cai and Zhang have established</p><p>several sharp RIP bounds that cover the most interesting cases of δ<sub>k</sub> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x25.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.63986-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.63986-ref8">8</xref>] showing<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x26.png" xlink:type="simple"/></inline-formula>.</p><p>A key requirement in this setting is a signal being sparse or approximately sparse. Indeed, Many families of integrating signals have sparse representations under suitable bases. Recently, an interesting sparsifying scheme was proposed by Cand&#232;s et al. [<xref ref-type="bibr" rid="scirp.63986-ref9">9</xref>] . In their scheme, instead of bases, tight frames are used to sparsify signals.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x27.png" xlink:type="simple"/></inline-formula> (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x28.png" xlink:type="simple"/></inline-formula>) be a tight frame and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x29.png" xlink:type="simple"/></inline-formula>. Cand&#232;s et al. [<xref ref-type="bibr" rid="scirp.63986-ref9">9</xref>] suggests that one use the following optimization to approximate the signal<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x30.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63986-formula57"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x31.png"  xlink:type="simple"/></disp-formula><p>The traditional RIP is no longer effective in the generalized setting. Cand&#232;s et al. defined the D-restricted isometry property which extends RIP [<xref ref-type="bibr" rid="scirp.63986-ref9">9</xref>] . Here the formulation of D-RIP is used as in Lin et al. [<xref ref-type="bibr" rid="scirp.63986-ref10">10</xref>] .</p><p>Definition 1. The measurement matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x32.png" xlink:type="simple"/></inline-formula> obeys the D-RIP with constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x33.png" xlink:type="simple"/></inline-formula> if</p><disp-formula id="scirp.63986-formula58"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x34.png"  xlink:type="simple"/></disp-formula><p>holds for all k-sparse vectors<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x35.png" xlink:type="simple"/></inline-formula>.</p><p>The RIP is now a special case of D-RIP (when the dictionary D is the identity matrix). For D being a tight frame, Cand&#232;s et al. [<xref ref-type="bibr" rid="scirp.63986-ref9">9</xref>] , proved that if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x36.png" xlink:type="simple"/></inline-formula>, then if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x37.png" xlink:type="simple"/></inline-formula> is approximately k-sparse, the solution to (3) is a good approximation of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x38.png" xlink:type="simple"/></inline-formula>. Lin et al. [<xref ref-type="bibr" rid="scirp.63986-ref10">10</xref>] , improved this result to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x39.png" xlink:type="simple"/></inline-formula> by using some techniques developed by Cand&#232;s et al. [<xref ref-type="bibr" rid="scirp.63986-ref3">3</xref>] .</p>Contribution<p>The proof in Section 2 establishes an improved D-RIP bound which states that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x40.png" xlink:type="simple"/></inline-formula>. This result was</p><p>previously available [<xref ref-type="bibr" rid="scirp.63986-ref1">1</xref>] and it has been improved on by Wu and Li [<xref ref-type="bibr" rid="scirp.63986-ref2">2</xref>] . The main ingredient of the proof in Section 2 is a tool developed by Xu et al. [<xref ref-type="bibr" rid="scirp.63986-ref11">11</xref>] . This approach takes its inspiration from the clever ideas of Cai and Zhang [<xref ref-type="bibr" rid="scirp.63986-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.63986-ref8">8</xref>] .</p><p>The practical application of this proof consists of experiments targeting the theory of using tight frames in this CS setting satisfying D-RIP. Similar experimental methods to those used by Cand&#232;s et al. are followed [<xref ref-type="bibr" rid="scirp.63986-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.63986-ref12">12</xref>] . However, an expanded variety of relevant sparse and non-sparse signals are used to test the robustness of the Gabor transform. Additionally, these experiments analyze sparsity in the coefficient domain and show that a highly sparse representation is a good indicator of reconstruction quality. These results are contrasted with a commonly used CS approach of Total Variation (TV) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x41.png" xlink:type="simple"/></inline-formula>minimization.</p><p>This paper is organized into four main sections. Background information is presented in Section 1. Section 2 describes a proof of an improved D-RIP sparsity bound by using a concise and transparent approach. Section 3 details the methods of experimentation used to apply the tight frame in practical applications of signals and image recovery. Section 4 shows and discusses the reconstruction simulation results with an analysis of the robustness and shortcomings of using tight frames in CS.</p></sec><sec id="s2"><title>2. New D-RIP Bounds</title><p>Theorem 2. Let D be an arbitrary tight frame and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x42.png" xlink:type="simple"/></inline-formula> be a measurement matrix satisfying D-RIP with</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x43.png" xlink:type="simple"/></inline-formula>. Then the solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x44.png" xlink:type="simple"/></inline-formula> to (3) satisfies</p><disp-formula id="scirp.63986-formula59"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x45.png"  xlink:type="simple"/></disp-formula><p>where the constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x46.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x47.png" xlink:type="simple"/></inline-formula> depend on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x48.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x49.png" xlink:type="simple"/></inline-formula>is the vector <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x50.png" xlink:type="simple"/></inline-formula> with all but the k largest</p><p>components (in magnitude) set to zero.</p><p>Before proving this theorem, some remarks are helpful. Firstly, Cai and Zhang have obtained a sharp bound</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x51.png" xlink:type="simple"/></inline-formula>for the case <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x52.png" xlink:type="simple"/></inline-formula> [<xref ref-type="bibr" rid="scirp.63986-ref8">8</xref>] . Their work inspired pursuit of the bound in this proof. Secondly, following</p><p>the ideas of Cai and Zhang [<xref ref-type="bibr" rid="scirp.63986-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.63986-ref8">8</xref>] , more general results (other D-RIP bounds) can be obtained in parallel.</p><p>In order to prove Theorem 2, the following <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x53.png" xlink:type="simple"/></inline-formula>-norm invariant convex k-sparse decomposition by Xu and Xu [<xref ref-type="bibr" rid="scirp.63986-ref11">11</xref>] , and Cai and Zhang [<xref ref-type="bibr" rid="scirp.63986-ref8">8</xref>] are needed.</p><p>The following description is taken from Xu et al. [<xref ref-type="bibr" rid="scirp.63986-ref11">11</xref>] .</p><p>Lemma 1. For positive integers<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x54.png" xlink:type="simple"/></inline-formula>, and positive constant C, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x55.png" xlink:type="simple"/></inline-formula> be a vector with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x56.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x57.png" xlink:type="simple"/></inline-formula>. Then there are k-sparse vectors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x58.png" xlink:type="simple"/></inline-formula> with</p><disp-formula id="scirp.63986-formula60"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x59.png"  xlink:type="simple"/></disp-formula><p>such that</p><disp-formula id="scirp.63986-formula61"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x60.png"  xlink:type="simple"/></disp-formula><p>for some nonnegative real numbers <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x61.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x62.png" xlink:type="simple"/></inline-formula>.</p><p>Now Theorem 2 is proven.</p><p>Proof. This proof follows some ideas in the proofs of Theorems 1.1 and 2.1 by Cai et al. [<xref ref-type="bibr" rid="scirp.63986-ref8">8</xref>] , incorporating some simplified steps. Some strategies from Cai et al. [<xref ref-type="bibr" rid="scirp.63986-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.63986-ref13">13</xref>] are also used. This proof deals only with the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x63.png" xlink:type="simple"/></inline-formula> case so that the key ideas can be conveyed clearly.</p><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x64.png" xlink:type="simple"/></inline-formula>.</p><p>For a subset<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x65.png" xlink:type="simple"/></inline-formula>, denoted by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x66.png" xlink:type="simple"/></inline-formula> the matrix D is restricted to the columns indexed by S (and replacing other columns by zero vectors). Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x67.png" xlink:type="simple"/></inline-formula> denote the index set of the largest k components of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x68.png" xlink:type="simple"/></inline-formula> (in</p><p>magnitude), i.e.,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x69.png" xlink:type="simple"/></inline-formula>. With this notation there is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x70.png" xlink:type="simple"/></inline-formula>. As in Cand&#232;s et al.</p><p>[<xref ref-type="bibr" rid="scirp.63986-ref9">9</xref>] , one can easily verify the following:</p><disp-formula id="scirp.63986-formula62"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x71.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula63"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x72.png"  xlink:type="simple"/></disp-formula><p>Denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x73.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x74.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x75.png" xlink:type="simple"/></inline-formula> is the i-th column of D, then</p><disp-formula id="scirp.63986-formula64"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x76.png"  xlink:type="simple"/></disp-formula><p>By rearranging the columns of D if necessary, assume<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x77.png" xlink:type="simple"/></inline-formula>. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x78.png" xlink:type="simple"/></inline-formula>. In this case, have</p><disp-formula id="scirp.63986-formula65"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x79.png"  xlink:type="simple"/></disp-formula><p>Assume that the tight frame D is normalized, i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x80.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x81.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x82.png" xlink:type="simple"/></inline-formula>. Thus there is the following useful relation:</p><disp-formula id="scirp.63986-formula66"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x83.png"  xlink:type="simple"/></disp-formula><p>From the facts <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x84.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x85.png" xlink:type="simple"/></inline-formula>, the relation</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x86.png" xlink:type="simple"/></inline-formula>yields</p><disp-formula id="scirp.63986-formula67"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x87.png"  xlink:type="simple"/></disp-formula><p>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x88.png" xlink:type="simple"/></inline-formula>, use Lemma 1 to get the following <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x89.png" xlink:type="simple"/></inline-formula>-invariant convex</p><p>k-sparse decomposition of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x90.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63986-formula68"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x91.png"  xlink:type="simple"/></disp-formula><p>with each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x92.png" xlink:type="simple"/></inline-formula> being k-sparse, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x93.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x94.png" xlink:type="simple"/></inline-formula>. From this and the</p><p>Cauchy-Schwartz inequality, there is</p><disp-formula id="scirp.63986-formula69"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x95.png"  xlink:type="simple"/></disp-formula><p>By the triangle inequality, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x96.png" xlink:type="simple"/></inline-formula>holds and thus</p><disp-formula id="scirp.63986-formula70"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x97.png"  xlink:type="simple"/></disp-formula><p>Note that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x98.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x99.png" xlink:type="simple"/></inline-formula>. In order to prove</p><p>the theorem, it suffices to show that there are constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x100.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.63986-formula71"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x101.png"  xlink:type="simple"/></disp-formula><p>In fact, assuming (17) there is</p><disp-formula id="scirp.63986-formula72"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x102.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula73"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x103.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula74"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x104.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula75"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x105.png"  xlink:type="simple"/></disp-formula><p>Now moving to the proof of (17). Denote</p><disp-formula id="scirp.63986-formula76"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x106.png"  xlink:type="simple"/></disp-formula><p>First, as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x107.png" xlink:type="simple"/></inline-formula> is k sparse, hence 2k sparse. There is</p><disp-formula id="scirp.63986-formula77"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x108.png"  xlink:type="simple"/></disp-formula><p>On the other hand, as each <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x109.png" xlink:type="simple"/></inline-formula> is 2k sparse, there is</p><disp-formula id="scirp.63986-formula78"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x110.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula79"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x111.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula80"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x112.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula81"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x113.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula82"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x114.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula83"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x115.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula84"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x116.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula85"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x117.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula86"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x118.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63986-formula87"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x119.png"  xlink:type="simple"/></disp-formula><p>Combining this with (23) shows</p><disp-formula id="scirp.63986-formula88"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x120.png"  xlink:type="simple"/></disp-formula><p>By making a perfect square, there is</p><disp-formula id="scirp.63986-formula89"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x121.png"  xlink:type="simple"/></disp-formula><p>which implies that</p><disp-formula id="scirp.63986-formula90"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x122.png"  xlink:type="simple"/></disp-formula><p>and finally have (17):</p><disp-formula id="scirp.63986-formula91"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x123.png"  xlink:type="simple"/></disp-formula><p>This demonstrates the use of Lemma 1 to get a good result. This could be pursued further to general cases for an even better bound. Indeed, this has been done recently by Wu and Li [<xref ref-type="bibr" rid="scirp.63986-ref2">2</xref>] to improve the result of this proof which has been available previously [<xref ref-type="bibr" rid="scirp.63986-ref1">1</xref>] .</p></sec><sec id="s3"><title>3. Experiments</title><p>The focus in these experiments is to show practical applications of a sparsifying frame that satisfies the new lower bound proven in the previous section. A time-frequency Gabor dictionary is used as a sparsifying trans- form in re-weighted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x124.png" xlink:type="simple"/></inline-formula> minimization [<xref ref-type="bibr" rid="scirp.63986-ref12">12</xref>] . The Gabor dictionary fulfills the requirements of D-RIP because it is a tight frame.</p><p>One of the advantages of a Gabor dictionary is its characteristic of translational invariance both in time and frequency. In a similar context, a translational invariant wavelet transform was used with good results in MRI reconstruction [<xref ref-type="bibr" rid="scirp.63986-ref14">14</xref>] . Invariance in the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x125.png" xlink:type="simple"/></inline-formula> minimization penalty term is advantageous for its ability to represent different signals sparsely.</p><p>Here comparison measurements of sparsity in Gabor and TV Coefficients of various signals are used to verify if good and robust results can be achieved. A selection of 5 different real valued signals and/or images with variants are used to simulate the complexity of practical signals.</p><p>・ Sinusoidal pulses (GHz range)</p><p>・ Shepp-Logan phantom image</p><p>・ Penguin image</p><p>・ T1 weighted MRI image</p><p>・ Time of Flight (TOF) Maximum Intensity Projection (MIP) MRI image</p><p>The original images and signals are sized to be a total length of 16k values-for images, this is a 128 &#215; 128 gray-scale image, shown in part (a) of each figure. These signals are not sparse in their native domain, but can become sparse when a transform is applied.</p><p>The use of the Gabor dictionary to reconstruct these signals utilizes a core optimization algorithm solver for the primal-dual interior point method provided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x126.png" xlink:type="simple"/></inline-formula>-Magic [<xref ref-type="bibr" rid="scirp.63986-ref15">15</xref>] . The redundancy of the Gabor transform coefficients compared to the original signal is about 43 times. These results are compared to reconstructions of the same input signal using another CS optimization algorithm solver, TV minimization with quadratic con- straint, which is also provided by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x127.png" xlink:type="simple"/></inline-formula>-Magic. These algorithms operate on the full sized image (or signal) without breaking up the data into segments. In both settings, the same under-sampling is performed by using a pseudo-random Gaussian measurement matrix with a factor of 2.</p><p>In <xref ref-type="table" rid="table1">Table 1</xref>, there is a comparison of two measures for this analysis, the Mean Square Error (MSE) and</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Sparsity and compressed Sensing reconstruction errors of various signals (L-Linear, G-Gabor, TV-Total Variation, MSE-Mean Square Error)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Test</th><th align="center" valign="middle" >L MSE</th><th align="center" valign="middle" >G MSE</th><th align="center" valign="middle" >TV MSE</th><th align="center" valign="middle" >%G Sparse</th><th align="center" valign="middle" >%TV Sparse</th></tr></thead><tr><td align="center" valign="middle" >1 (Pulse 1)</td><td align="center" valign="middle" >0.7045</td><td align="center" valign="middle" >0.0195</td><td align="center" valign="middle" >0.9411</td><td align="center" valign="middle" >99.5</td><td align="center" valign="middle" >0.19</td></tr><tr><td align="center" valign="middle" >2 (Pulse 2)</td><td align="center" valign="middle" >0.7075</td><td align="center" valign="middle" >0.0192</td><td align="center" valign="middle" >0.8023</td><td align="center" valign="middle" >94.8</td><td align="center" valign="middle" >2.6</td></tr><tr><td align="center" valign="middle" >3 (Shepp-Logan)</td><td align="center" valign="middle" >0.7062</td><td align="center" valign="middle" >0.2697</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >54.7</td><td align="center" valign="middle" >91.7</td></tr><tr><td align="center" valign="middle" >4 (Penguin)</td><td align="center" valign="middle" >0.7077</td><td align="center" valign="middle" >0.3011</td><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >54.1</td><td align="center" valign="middle" >87.6</td></tr><tr><td align="center" valign="middle" >5 (Pulse + Shepp-Logan)</td><td align="center" valign="middle" >0.7101</td><td align="center" valign="middle" >0.2541</td><td align="center" valign="middle" >0.2141</td><td align="center" valign="middle" >54.4</td><td align="center" valign="middle" >2.2</td></tr><tr><td align="center" valign="middle" >6 (T1 MRI)</td><td align="center" valign="middle" >0.7013</td><td align="center" valign="middle" >0.1445</td><td align="center" valign="middle" >0.0637</td><td align="center" valign="middle" >82.9</td><td align="center" valign="middle" >7.8</td></tr><tr><td align="center" valign="middle" >7 (TOF MRI)</td><td align="center" valign="middle" >0.7012</td><td align="center" valign="middle" >0.2555</td><td align="center" valign="middle" >0.1369</td><td align="center" valign="middle" >68.4</td><td align="center" valign="middle" >13.3</td></tr></tbody></table></table-wrap><p>Sparsity. Measurements of normalized MSE are taken, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x128.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x129.png" xlink:type="simple"/></inline-formula> are the original and reconstructed image.</p><disp-formula id="scirp.63986-formula92"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-3400447x130.png"  xlink:type="simple"/></disp-formula><p>A Linear (L) MSE of the reconstruction is used as a reference, shown as (b) in each figure. This is calculated by the transpose of the measurement matrix as the pseudo inverse. Gabor (G) MSE identifies the error in the use of that dictionary in the CS reconstruction, shown in parts (c) of the figures. TV MSE is a measure of the error when TV weighted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x131.png" xlink:type="simple"/></inline-formula> minimization is performed and is shown in part (d) of each figure.</p><p>Sparsity measurements taken in the coefficient domain are based on a ratio of the count of values that are less than 1/256 of the maximum coefficient, divided by the total number of the coefficients. This ratio then is a percentage of sparsity. Two sparsity measures are taken:</p><p>・ % G Sparse-Sparsity of the Gabor transform coefficients of the fully sampled signal</p><p>・ % TV Sparse-Sparsity of the TV calculation of the fully sampled signal</p></sec><sec id="s4"><title>4. Results and Discussion</title><p>The goal is to show how well a sparse tight frame representation of various signals performs in CS recon- struction. Analysis is done of the Gabor dictionary as a sparsifying transform on non-sparse signals and images. A large range of reconstruction errors and sparsity levels are observed for different image types and signals. The use of the Gabor frame with a reference of TV weighted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x132.png" xlink:type="simple"/></inline-formula> minimization in compressed sensing reconstruction is compared. <xref ref-type="table" rid="table1">Table 1</xref> quantifies MSE and sparsity for each reconstruction test. Figures 1-8 are the corres- ponding image and signal reconstructions.</p><p>According to these measurements, sparsity in the coefficient domain will correlate to image reconstruction</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Signal reconstruction test 1, one long pulse (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig1_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x133.png"/></fig></fig-group><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Reconstruction test 2, 20 short pulses (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig2_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x134.png"/></fig></fig-group><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Reconstruction test 3, Shepp-Logan phantom (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig3_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x135.png"/></fig></fig-group><fig-group id="fig4"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Reconstruction test 4, penguin (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig4_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x136.png"/></fig></fig-group><fig-group id="fig5"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Signal reconstruction test 5, one long pulse + Shepp-Logan phantom (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig5_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x137.png"/></fig></fig-group><fig-group id="fig6"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Image reconstruction test 5, one long pulse + Shepp-Logan phantom (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig6_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x138.png"/></fig></fig-group><fig-group id="fig7"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Reconstruction test 6, T1 MRI, (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig7_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x139.png"/></fig></fig-group><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Reconstruction test 7, MIP MRI, (a) original; (b) linear pseudo inverse; (c) CS Gabor; (d) CS TV.</title></caption><fig id ="fig8_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-3400447x140.png"/></fig></fig-group><p>success. For example, test 1 measures a Gabor coefficient sparsity of over 99% and a reconstruction success which reduces the MSE by 36 times compared to the linear reconstruction. Whereas, with the same signal, which is not sparse at all in the TV domain, TV minimization actually increases the MSE when compared with the linear reconstruction, see <xref ref-type="fig" rid="fig1">Figure 1</xref>. It is important to note that the sparsity calculated on the Gabor coefficient set is on a much larger set of redundant coefficients than the non-redundant TV coefficients.</p><p>In test 2, the complexity and sparsity are adjusted by adding additional sinusoidal pulses which may overlap. The complexity of the pulses significantly increases to 20 pulses and the Gabor dictionary is able to sparsely represent the signal very well compared to TV minimization, see <xref ref-type="fig" rid="fig2">Figure 2</xref>. Similar to the results in test 1, the reconstruction MSE is reduced by 36 times.</p><p>In tests 3 and 4, images are chosen which are sparse in the TV domain but not in the Gabor domain. The TV reconstruction reduces the MSE to zero compared to the Gabor reconstruction reducing by only a factor of 2.6 and 2.4 respectively. The penguin image is an example with a different background magnitude from the Shepp-Logan phantom, see <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref>.</p><p>The signal in test 5 is a combination of a pulse from test 1 with the Shepp-Logan image from test 3. The same signal is plotted in the time domain for <xref ref-type="fig" rid="fig5">Figure 5</xref> and in the image domain for <xref ref-type="fig" rid="fig6">Figure 6</xref>. Although both Gabor and TV CS reconstructions improve the result over the linear calculation, the error still remains quite large. It is noteworthy that the sparsity percentages are much lower for this case in both the TV and Gabor domains. This underscores the important connection between having a sparse representation and making a good reconstruction.</p><p>In the last experiments, tests 6 and 7, MRI images of the brain as either T1 weighted or TOF MIP are used. They appear not to be sparsely represented in either the Gabor domain or in TV. The MSE result is poor in both reconstruction algorithms, see <xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref>. It is important to note that under-sampling is in the image domain and not in the native MRI signal domain of k-space. However, this is still an equivalent comparison for cases when the under-sampled k-space produces artifacts that are incoherent as in this experiment. A require- ment of CS reconstruction is that artifacts due to sampling are similar to uniform noise with an even distribution across the image.</p><p>It is also important to point out that the linear reconstructions, calculated with a pseudo-inverse, have a consistent MSE for all experiments, see L MSE in <xref ref-type="table" rid="table1">Table 1</xref>. This is not the case for this tight frame. These findings show remarkably good results for some periodic signals. However, the Gabor tight frame does not appear to be advantageous for the images investigated here. The ability of the sparsifying transform to produce a high percentage of sparsity contributes greatly to the reduction of reconstruction error. When using CS in these cases, it is vital to pick a dictionary which will effectively and sparsely represent the signal of interest.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The use of a new D-RIP sparsity bound constant for compressed sensing is proven using a transparent and concise approach. Practical numerical experiments for this setting are performed. The use of a Gabor tight frame in CS is contrasted with TV weighted <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-3400447x141.png" xlink:type="simple"/></inline-formula> minimization by simulation. Measurements of reconstruction error and coefficient sparsity in each domain are presented and analyzed. Sparse representation by frames does provide good results when the dictionary is chosen appropriately. Care must be taken to assure high levels of sparsity are achieved in the coefficient domain. Otherwise, poor fidelity in reconstruction may occur.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The author wishes to thank several people: Academic supervisor, Professor Guangwu Xu, for his assistance in the proofs of the results in Section 2, suggestions in setting up experiments, and help with analysis. Bing Gao, for pointing out an error in the earlier version of the proof [<xref ref-type="bibr" rid="scirp.63986-ref1">1</xref>] . Dr. Kevin King, from GE Healthcare for providing the MRI images and suggestions for improvement. Dr. Michael Wakin [<xref ref-type="bibr" rid="scirp.63986-ref12">12</xref>] , who provided some code useful for experiment comparison.</p></sec><sec id="s7"><title>Cite this paper</title><p>ChristopherBaker, (2016) Sparse Representation by Frames with Signal Analysis. 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