<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.77063</article-id><article-id pub-id-type="publisher-id">AM-66058</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Estimates of Approximation Error by Legendre Wavelet
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>iaoyang</surname><given-names>Zheng</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>Zhengyuan</surname><given-names>Wei</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Mathematics and Statistics, Chongqing University of Technology, Chongqing, China</addr-line></aff><pub-date pub-type="epub"><day>18</day><month>04</month><year>2016</year></pub-date><volume>07</volume><issue>07</issue><fpage>694</fpage><lpage>700</lpage><history><date date-type="received"><day>10</day>	<month>March</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>25</month>	<year>April</year>	</date><date date-type="accepted"><day>28</day>	<month>April</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>
 
  This paper first introduces Legendre wavelet bases and derives their rich properties. Then these properties are applied to estimation of approximation error upper bounded in spaces 
  <img src="Edit_bc7ea7ec-1c3a-4060-9561-8e9fe19d4219.bmp" alt="" /> and 
  <img src="Edit_7c5bec68-e19d-4908-91aa-a959a14eaa63.bmp" alt="" /> by norms 
  <img src="Edit_63e58228-d186-4ef7-bdd3-35f84524f0a8.bmp" alt="" /> and 
  <img src="Edit_3f86a762-c1c7-41e2-9927-7e3162745580.bmp" alt="" /> , respectively. These estimate results are valuable to solve integral-differential equations by Legendre wavelet method.
 
</html></p></abstract><kwd-group><kwd>Legendre Wavelet</kwd><kwd> Estimate</kwd><kwd> Exponential ?-H&#246;lder Continuity</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In recent years, an application of Legendre wavelet to solve integral-differential equations and partial differential equations is deeply considered [<xref ref-type="bibr" rid="scirp.66058-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.66058-ref9">9</xref>] . Generally, representations of function and operator by Legendre wavelet are exact up to arbitrary but finite precision, then the approximation error should be estimated. Although estimating the approximation error is a tough technique, if the wavelet satisfies certain conditions [<xref ref-type="bibr" rid="scirp.66058-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.66058-ref11">11</xref>] , then the upper bounded of the wavelet transform coefficients can be estimated. In this article, we use the rich properties of Legendre wavelet bases such as compactly supported, polynomials, orthogonality to estimate the appro- ximation error upper bounded.</p><p>In this paper, Section 2 introduces Legendre wavelet bases and its properties. Section 3 estimates the approximation error upper bounded by norms <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x10.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x11.png" xlink:type="simple"/></inline-formula> for spaces <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x12.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x13.png" xlink:type="simple"/></inline-formula>, respectively. This paper ends with brief conclusion.</p></sec><sec id="s2"><title>2. Legendre Wavelet and Its Properties</title><p>In this section, we first briefly introduce Legendre wavelet bases and our notations. Secondly, the rich properties and some important results of Legendre wavelet that will be used later are elaborated.</p><sec id="s2_1"><title>2.1. Legendre Wavelet</title><p>For level of decomposition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x14.png" xlink:type="simple"/></inline-formula> and translation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x15.png" xlink:type="simple"/></inline-formula>, we define subinterval<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x16.png" xlink:type="simple"/></inline-formula>. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x17.png" xlink:type="simple"/></inline-formula>, define <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x18.png" xlink:type="simple"/></inline-formula> as a subspace of piecewise polynomial functions satisfying</p><disp-formula id="scirp.66058-formula610"><graphic  xlink:href="http://html.scirp.org/file/11-7403145x19.png"  xlink:type="simple"/></disp-formula><p>We now start to review Legendre polynomials and Legendre wavelet bases [<xref ref-type="bibr" rid="scirp.66058-ref1">1</xref>] . Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x20.png" xlink:type="simple"/></inline-formula> denote Legendre polynomial of degree k, which is defined as follows:</p><disp-formula id="scirp.66058-formula611"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x21.png"  xlink:type="simple"/></disp-formula><p>Then, at the level of resolution<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x22.png" xlink:type="simple"/></inline-formula>, let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x23.png" xlink:type="simple"/></inline-formula> denote Legendre wavelet bases defined as</p><disp-formula id="scirp.66058-formula612"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x24.png"  xlink:type="simple"/></disp-formula><p>The whole set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x25.png" xlink:type="simple"/></inline-formula> forms an orthonormal basis for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x26.png" xlink:type="simple"/></inline-formula>.Generally, the subspace <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x27.png" xlink:type="simple"/></inline-formula> is spanned by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x28.png" xlink:type="simple"/></inline-formula> functions which are obtained from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x29.png" xlink:type="simple"/></inline-formula> by dilation and translation, i.e.,</p><disp-formula id="scirp.66058-formula613"><graphic  xlink:href="http://html.scirp.org/file/11-7403145x30.png"  xlink:type="simple"/></disp-formula><p>which forms an orthonormal basis for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x31.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x32.png" xlink:type="simple"/></inline-formula>.</p><p>Now, let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x33.png" xlink:type="simple"/></inline-formula>, then obtain six Legendre wavelet base functions which are given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x34.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x35.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x36.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x37.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x38.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x39.png" xlink:type="simple"/></inline-formula></p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x41.png" xlink:type="simple"/></inline-formula></p><p>and <xref ref-type="fig" rid="fig1">Figure 1</xref> illustrates these base function as</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The six Legendre wavelet bases with k = 0, 1, 2; n = 1.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-7403145x42.png"/></fig></fig-group></sec><sec id="s2_2"><title>2.2. Some Properties of Legendre Wavelet</title><p>It is clear that Legendre wavelet bases are compactly supported, polynomial, bounded and orthogonal on each subinterval<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x43.png" xlink:type="simple"/></inline-formula>. These properties are very useful to estimate the approximation error upper bounded.</p><p>Lemma 1. Legendre wavelet bases satisfy the results</p><disp-formula id="scirp.66058-formula614"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x44.png"  xlink:type="simple"/></disp-formula><p>Lemma 2. For any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x45.png" xlink:type="simple"/></inline-formula>, Legendre wavelet <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x46.png" xlink:type="simple"/></inline-formula> are bounded by the form</p><disp-formula id="scirp.66058-formula615"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x47.png"  xlink:type="simple"/></disp-formula><p>where k is the order of Legendre wavelet.</p><p>Proof. According to the definition of Legendre wavelet bases, Legendre wavelet defined on subinterval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x48.png" xlink:type="simple"/></inline-formula> are obtained through Legendre polynomials by dilation. With the result of Legendre polynomials<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x49.png" xlink:type="simple"/></inline-formula>, the bound of Legendre wavelet is easily proved.</p><p>Lemma 3. A relation of between Legendre wavelet and their derivative on each subinterval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x50.png" xlink:type="simple"/></inline-formula> is derived as</p><disp-formula id="scirp.66058-formula616"><label>. (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x51.png"  xlink:type="simple"/></disp-formula><p>Proof. Using the result of between Legendre polynomials and their derivative, i.e.,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x52.png" xlink:type="simple"/></inline-formula>,</p><p>we can obtain the above result.</p><p>Using this result, we can obtain</p><disp-formula id="scirp.66058-formula617"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x53.png"  xlink:type="simple"/></disp-formula><p>However, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x54.png" xlink:type="simple"/></inline-formula>, the integration is calculated as</p><disp-formula id="scirp.66058-formula618"><label>. (7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x55.png"  xlink:type="simple"/></disp-formula><p>Now, the orthogonal property of Legendre wavelet bases is given by</p><p>Lemma 4. Legendre wavelet bases defined on the interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x56.png" xlink:type="simple"/></inline-formula> are orthogonal.</p><p>Proof. According to the compactly supported of Legendre wavelet bases, we know that any two such base functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x57.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x58.png" xlink:type="simple"/></inline-formula> with the same scale index n and different<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x59.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x60.png" xlink:type="simple"/></inline-formula>are orthogonal. If any two bases functions are only different in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x61.png" xlink:type="simple"/></inline-formula>, then for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x62.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.66058-formula619"><graphic  xlink:href="http://html.scirp.org/file/11-7403145x63.png"  xlink:type="simple"/></disp-formula><p>which completes the proof.</p><p>Thus, any function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x64.png" xlink:type="simple"/></inline-formula> belonging to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x65.png" xlink:type="simple"/></inline-formula> can be expanded as</p><disp-formula id="scirp.66058-formula620"><label>, (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x66.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x67.png" xlink:type="simple"/></inline-formula> is Legendre wavelet coefficients and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x68.png" xlink:type="simple"/></inline-formula> denotes inner product. Accordingly, norm equality is given by</p><disp-formula id="scirp.66058-formula621"><label>. (9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x69.png"  xlink:type="simple"/></disp-formula><p>If approximation of the function is analyzed in the space V<sub>p</sub><sub> n</sub>, then the approximation formula is described by</p><disp-formula id="scirp.66058-formula622"><label>, (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x70.png"  xlink:type="simple"/></disp-formula><p>where S and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x71.png" xlink:type="simple"/></inline-formula> are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x72.png" xlink:type="simple"/></inline-formula> matrices and defined as, respectively</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x73.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.66058-formula623"><graphic  xlink:href="http://html.scirp.org/file/11-7403145x74.png"  xlink:type="simple"/></disp-formula><p>which makes the function approximated by arbitrary precision, when numerical computation is adopted by Legendre wavelet method.</p></sec></sec><sec id="s3"><title>3. Upper Bounded Estimates of Approximation Error by Legendre Wavelet</title><p>In this section, the preliminaries of the function spaces with respect to exponential a-H&#246;lder continuity and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x75.png" xlink:type="simple"/></inline-formula> are first introduced, respectively. Secondly, the upper bounded estimates of approximation error in the spaces by Legendre wavelet bases are derived by norms <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x76.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x76.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x77.png" xlink:type="simple"/></inline-formula>, respectively.</p><sec id="s3_1"><title>3.1. Exponential a-H&#246;lder Continuity and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x78.png" xlink:type="simple"/></inline-formula></title><p>The preliminaries of exponential a-H&#246;lder continuity <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x79.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x80.png" xlink:type="simple"/></inline-formula> spaces are defined by</p><p>Definition 1. Exponential a-H&#246;lder continuity for any a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x81.png" xlink:type="simple"/></inline-formula> denotes the function f satisfying</p><disp-formula id="scirp.66058-formula624"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x82.png"  xlink:type="simple"/></disp-formula><p>for some positive constant A.</p><p>Definition 2. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x83.png" xlink:type="simple"/></inline-formula>space denotes that all the functions f which are bounded and continuously differentiable up to N-order for any a<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x84.png" xlink:type="simple"/></inline-formula>, i.e.,</p><disp-formula id="scirp.66058-formula625"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x85.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x86.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3_2"><title>3.2. Approximation Error Estimate by Norm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x87.png" xlink:type="simple"/></inline-formula></title><p>The upper bounded of Legendre wavelet transform coefficients is estimated as:</p><p>Theorem 1. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x88.png" xlink:type="simple"/></inline-formula>, then the upper bounded estimate of Legendre wavelet transform coefficients satisfies</p><disp-formula id="scirp.66058-formula626"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x89.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x90.png" xlink:type="simple"/></inline-formula> is a constant with respect to k, f and l.</p><p>Proof. Taking advantage of the results of (6) and (7), we have</p><disp-formula id="scirp.66058-formula627"><graphic  xlink:href="http://html.scirp.org/file/11-7403145x91.png"  xlink:type="simple"/></disp-formula><p>which completes this proof.</p><p>Remark: The upper bounded of Legendre wavelet transform coefficients vanish with exponent in terms of multiplies of the scale index or exponential a-H&#246;lder continuity.</p><p>Theorem 2. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x92.png" xlink:type="simple"/></inline-formula>, suppose that wavelet has n vanishing moments, then the upper bounded estimate of wavelets <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x93.png" xlink:type="simple"/></inline-formula> transform coefficients k such that then the upper bounded estimate of Legendrewavelet transform coefficients satisfies</p><disp-formula id="scirp.66058-formula628"><label>, (14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x94.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x95.png" xlink:type="simple"/></inline-formula> is a constant with respect to k, f and l.</p><p>Proof. The proof of this theorem utilizes the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x96.png" xlink:type="simple"/></inline-formula> vanishing moments of Legendre wavelet <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x97.png" xlink:type="simple"/></inline-formula> and Taylor expansion of the function f and then is similar to that of the theorem 1.</p><p>Now, taking advantage of the results of (9), (13) and theorem 1, we can derive the upper bounded estimation by the norm<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x98.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 3. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x99.png" xlink:type="simple"/></inline-formula>, then the upper bounded estimate of approximation error by using Legendre wavelet bases satisfies</p><disp-formula id="scirp.66058-formula629"><label>, (15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x100.png"  xlink:type="simple"/></disp-formula><p>where T is a constant with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x101.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x102.png" xlink:type="simple"/></inline-formula> is an arbitrarily small positive constant.</p><p>Proof. From the equality<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x103.png" xlink:type="simple"/></inline-formula>, there exists positive integers<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x104.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x105.png" xlink:type="simple"/></inline-formula>, K, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x106.png" xlink:type="simple"/></inline-formula>and arbi-</p><p>trarily small positive constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x107.png" xlink:type="simple"/></inline-formula> satisfying</p><disp-formula id="scirp.66058-formula630"><graphic  xlink:href="http://html.scirp.org/file/11-7403145x108.png"  xlink:type="simple"/></disp-formula><p>which completes the proof.</p><p>Similarly, we can obtain the estimate of approximation error in space<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x109.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 4. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x110.png" xlink:type="simple"/></inline-formula>, the upper bounded estimate of approximation error using Legendre wavelet is described as</p><disp-formula id="scirp.66058-formula631"><label>, (16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x111.png"  xlink:type="simple"/></disp-formula><p>where T is a constant with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x112.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x113.png" xlink:type="simple"/></inline-formula> is an arbitrarily small positive constant.</p><p>These estimates of the approximation error upper bounded provide computational precision for numerical computation.</p></sec><sec id="s3_3"><title>3.3. Approximation Error Estimate by Norm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x114.png" xlink:type="simple"/></inline-formula></title><p>In this subsection, we derive the estimations of approximation error by norm<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x115.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 5. Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x116.png" xlink:type="simple"/></inline-formula>, then the estimation of the approximation error upper bounded by the norm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x117.png" xlink:type="simple"/></inline-formula> satisfies</p><disp-formula id="scirp.66058-formula632"><label>, (17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x118.png"  xlink:type="simple"/></disp-formula><p>where T is a constant with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x119.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x120.png" xlink:type="simple"/></inline-formula> is an arbitrarily small positive constant.</p><p>Proof. Taking advantage of the definition of norm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x121.png" xlink:type="simple"/></inline-formula> and using (13), it is clear that the approximation error upper bounded is estimated by</p><disp-formula id="scirp.66058-formula633"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-7403145x122.png"  xlink:type="simple"/></disp-formula><p>For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x123.png" xlink:type="simple"/></inline-formula>,the estimate technique by the norm <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x124.png" xlink:type="simple"/></inline-formula> is similar to the theorem 4 and theorem 5.</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>As all, this paper considers the compactly supported, polynomial, orthogonal and bounded properties of Legendre wavelet bases. Using these properties, the upper bounded estimates of the approximation error are presented for the function belonging to exponential a-H&#246;lder continuity and space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x125.png" xlink:type="simple"/></inline-formula> by norms <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x126.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x127.png" xlink:type="simple"/></inline-formula>, respectively.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work is funded by Fundamental and Advanced Research Project of Chongqing CSTC of China, the project No. are CSTC2013JCYJA00022 and CSTC2012jjA00018.</p></sec><sec id="s6"><title>Cite this paper</title><p>Xiaoyang Zheng,Zhengyuan Wei, (2016) Estimates of Approximation Error by Legendre Wavelet. Applied Mathematics,07,694-700. doi: 10.4236/am.2016.77063</p></sec><sec id="s7"><title>Responses to Reviewers’ Comments</title><p>Firstly, the authors are grateful to the editors and referees for their valuable comments that greatlyimprove the quality of this paper. We now present responses to the valuable comments proposed by the referees detail by detail.</p><p>Common comments proposed by the reviewers.</p></sec><sec id="s8"><title>Comment to the author</title><p>The author introduces Legendre wavelet bases and derives their rich properties.</p><p>Here are some comments to this work:</p><p>1. In the proof of Lemma 3, it is noted that it should be<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x128.png" xlink:type="simple"/></inline-formula>, but not <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x129.png" xlink:type="simple"/></inline-formula> when k = 0.</p><p>2. In the proof of Lemma 4, the author should clearly indicate why <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x130.png" xlink:type="simple"/></inline-formula> holds.</p><p>3. In page 4, is there something wrong for defining the function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x131.png" xlink:type="simple"/></inline-formula>? It is noted that the author claims that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x132.png" xlink:type="simple"/></inline-formula>. However, he also defines<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x133.png" xlink:type="simple"/></inline-formula>. Does it look like a cycle?</p><p>4. In the proof of Theorem 1, why does the author emit the part <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x134.png" xlink:type="simple"/></inline-formula> related to</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x135.png" xlink:type="simple"/></inline-formula>? Will the inequality still hold if doing so?</p></sec><sec id="s9"><title>Response</title><p>1. We discuss the situation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x136.png" xlink:type="simple"/></inline-formula>, thus it is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x137.png" xlink:type="simple"/></inline-formula>.</p><p>2. Because<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x138.png" xlink:type="simple"/></inline-formula>.</p><p>3. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x139.png" xlink:type="simple"/></inline-formula>is the wavelet coefficient and it is calculated by inner product.</p><p>4. Because<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-7403145x140.png" xlink:type="simple"/></inline-formula>.</p><p>Based on the above responses, I think there is no need to be corrected.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.66058-ref1"><label>1</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Beylkin</surname><given-names> G. </given-names></name>,<etal>et al</etal>. 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