<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2015.311163</article-id><article-id pub-id-type="publisher-id">JAMP-61112</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>
 
 
  On the Equiconvergence of the Fourier Series and Integral of Distributions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>A. Rakhimov</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 Science in Engineering, International Islamic University Malaysia (IIUM), Kuala Lumpur, Malaysia</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>abdumalik@iium.edu.my</email></corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>11</month><year>2015</year></pub-date><volume>03</volume><issue>11</issue><fpage>1361</fpage><lpage>1366</lpage><history><date date-type="received"><day>14</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>13</month>	<year>November</year>	</date><date date-type="accepted"><day>16</day>	<month>November</month>	<year>2015</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>
 
 
  We prove equiconvergence of the Bochner-Riesz means of the Fourier series and integral of distributions with compact support from the Liouville spaces.
 
</p></abstract><kwd-group><kwd>Bochner-Riesz Means</kwd><kwd> Fourier Series</kwd><kwd> Fourier Integrals</kwd><kwd> Distributions</kwd><kwd> Equiconvergence</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Convergence of the Fourier series and integral of integrable functions of one variable at certain point depends only from the values of the function in the small neighbourhood of this point (localizations principles). More- over, the difference of the partial sums of the Fourier series and integral of a function uniformly converge to zero, which means both expansions converge or diverge at the same time (equiconvergence).</p><p>In N-dimensional case, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x6.png" xlink:type="simple"/></inline-formula>, localization principles, as well as equiconvergence, for the Fourier series and integral is not valid by the Pringsheim convergence [<xref ref-type="bibr" rid="scirp.61112-ref1">1</xref>] . In [<xref ref-type="bibr" rid="scirp.61112-ref2">2</xref>] it is given a review of recent results on equiconvergence of expansions in multiple trigonometric Fourier series and integral in the case of summation over rectangles. In [<xref ref-type="bibr" rid="scirp.61112-ref3">3</xref>] the problem of equiconvergence for expansions in a triple trigonometric Fourier series and a Fourier integral of continuous functions with a certain modulus of continuity in the case of a lacunary sequence of partial sums is studied.</p><p>In [<xref ref-type="bibr" rid="scirp.61112-ref4">4</xref>] equiconvergence of the Fourier interals and expansions associated with a Schrodinger operator is studied. In [<xref ref-type="bibr" rid="scirp.61112-ref5">5</xref>] the author obtained sufficient conditions on the potential under which uniform equiconvergence holds for the expansion of a integrable function in the system of eigenfunctions and associated functions of corresponding Sturm-Liouville operator and its Fourier sine series expansion (in [<xref ref-type="bibr" rid="scirp.61112-ref6">6</xref>] potential is a distribution). In [<xref ref-type="bibr" rid="scirp.61112-ref7">7</xref>] a comparison theorem on equiconvergence of the Fourier Jacobi series with certain trigonometric Fourier series is proved.</p><p>In this paper we study equiconvergence of the Fourier series and integral of the linear continuous functionals (distributions) in the case of spherical summation. Localiation of spectral expansions of distributions for the first time was studied by Sh.A. Alimov [<xref ref-type="bibr" rid="scirp.61112-ref8">8</xref>] . Further results in [<xref ref-type="bibr" rid="scirp.61112-ref8">8</xref>] expanded to the more general spectral expansions in [<xref ref-type="bibr" rid="scirp.61112-ref9">9</xref>] - [<xref ref-type="bibr" rid="scirp.61112-ref14">14</xref>] .</p></sec><sec id="s2"><title>2. Preliminaries</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x7.png" xlink:type="simple"/></inline-formula> be the space of infinitely differentiable functions<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x8.png" xlink:type="simple"/></inline-formula>, with the locally convex topology produced from the system of the semi-norms</p><disp-formula id="scirp.61112-formula24"><graphic  xlink:href="http://html.scirp.org/file/1-1720374x9.png"  xlink:type="simple"/></disp-formula><p>where K is a compact subset of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x10.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x12.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x11.png" xlink:type="simple"/></inline-formula>is a non negative integer number, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x13.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x14.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x15.png" xlink:type="simple"/></inline-formula></p><p>Recall <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x16.png" xlink:type="simple"/></inline-formula> the space of distributions on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x17.png" xlink:type="simple"/></inline-formula>, i.e. the space of all continuous linear functionals on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x18.png" xlink:type="simple"/></inline-formula>. In fact any element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x19.png" xlink:type="simple"/></inline-formula> has a compact support in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x20.png" xlink:type="simple"/></inline-formula> and can be represented as the weakly convergent Fourier series</p><disp-formula id="scirp.61112-formula25"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x21.png"  xlink:type="simple"/></disp-formula><p>where its Fourier coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x22.png" xlink:type="simple"/></inline-formula> defined as the value of f on the test function on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x23.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x24.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x25.png" xlink:type="simple"/></inline-formula> is the set of all N-tuples with integer coordinates.</p><p>The Riesz means of order s, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x26.png" xlink:type="simple"/></inline-formula>of the spherical partial sums of the Fourier series (1) define by</p><disp-formula id="scirp.61112-formula26"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x27.png"  xlink:type="simple"/></disp-formula><p>Now, let us extend f from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x28.png" xlink:type="simple"/></inline-formula> to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x29.png" xlink:type="simple"/></inline-formula> by zero and leave the same notation for f. Then recall the Bochner- Riesz means of order s of the Fourier integral of f</p><disp-formula id="scirp.61112-formula27"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x30.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x31.png" xlink:type="simple"/></inline-formula> is the Fourier transformation of the distribution f evaluated as its action on the test function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x32.png" xlink:type="simple"/></inline-formula> with respect to the variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x33.png" xlink:type="simple"/></inline-formula>.</p><p>In this paper we shall be studying a relation between expansions (2) and (3) for some values of the summation index s depending on the power of singularity of f. In fact we will prove uniform equiconvergence of the Riesz means of the Fourier series and the Fourier integral expansion.</p><p>However, a behaviour of spherical means for the Fourier series and the Fourier integral expansion can be es</p><p>sentially different. The first results on the different behaviour of the Riesz means of critical index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x34.png" xlink:type="simple"/></inline-formula></p><p>of the Fourier integral and the Fourier series in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x35.png" xlink:type="simple"/></inline-formula> found by S. Bochner [<xref ref-type="bibr" rid="scirp.61112-ref15">15</xref>] , where it is proved that the localization of the means (3) holds and for the means (2) the localization fails. In the same paper [<xref ref-type="bibr" rid="scirp.61112-ref15">15</xref>] it is proved va-</p><p>lidity of localization principle in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x36.png" xlink:type="simple"/></inline-formula> for both expansions in the critical index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x37.png" xlink:type="simple"/></inline-formula> E. Stein [<xref ref-type="bibr" rid="scirp.61112-ref16">16</xref>] proved that if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x38.png" xlink:type="simple"/></inline-formula> the localization principle for the means (2) remain valid in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x39.png" xlink:type="simple"/></inline-formula> (consequently in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x40.png" xlink:type="simple"/></inline-formula>).</p><p>In [<xref ref-type="bibr" rid="scirp.61112-ref17">17</xref>] B.M. Levitan reported the first result on the uniform equisummability of the Riesz means</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x41.png" xlink:type="simple"/></inline-formula>expansions associated with the Laplace operator. The Riesz equisummability below critical index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x42.png" xlink:type="simple"/></inline-formula> studied by V.A. Il’in [<xref ref-type="bibr" rid="scirp.61112-ref18">18</xref>] .</p></sec><sec id="s3"><title>3. Main Results</title><p>For any real number <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x43.png" xlink:type="simple"/></inline-formula> by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x44.png" xlink:type="simple"/></inline-formula> denote the Liouville space of distributions</p><disp-formula id="scirp.61112-formula28"><graphic  xlink:href="http://html.scirp.org/file/1-1720374x45.png"  xlink:type="simple"/></disp-formula><p>Theorem 1 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x46.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x47.png" xlink:type="simple"/></inline-formula> Then for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x48.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.61112-formula29"><graphic  xlink:href="http://html.scirp.org/file/1-1720374x49.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x50.png" xlink:type="simple"/></inline-formula> a norm in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x51.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.61112-formula30"><graphic  xlink:href="http://html.scirp.org/file/1-1720374x52.png"  xlink:type="simple"/></disp-formula><p>Note, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x53.png" xlink:type="simple"/></inline-formula>, then for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x54.png" xlink:type="simple"/></inline-formula> there exist a distribution from <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x55.png" xlink:type="simple"/></inline-formula> such that it is coin-</p><p>cides with zero in some neighbourhood of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x56.png" xlink:type="simple"/></inline-formula> and the means <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x57.png" xlink:type="simple"/></inline-formula> (the same for the means <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x58.png" xlink:type="simple"/></inline-formula> diverges [<xref ref-type="bibr" rid="scirp.61112-ref8">8</xref>] . Thus, formula (4) provides precise result on the uniform equiconvergence of the Riesz means of the Fourier Integral and Series.</p><p>The illustration of the domains of convergence in the Theorem 1 given in <xref ref-type="fig" rid="fig1">Figure 1</xref> below and equiconver</p><p>gence summation domain for the Dirac delta function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x59.png" xlink:type="simple"/></inline-formula> given in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec><sec id="s4"><title>4. Estimation of the Direchlet Kernel</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x60.png" xlink:type="simple"/></inline-formula> be the Riesz means of the partial sums of the Fourier series of the Dirac delta function, which is well known as the Direchlet kernel:</p><disp-formula id="scirp.61112-formula31"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x61.png"  xlink:type="simple"/></disp-formula><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Localization of the Fourier Integral and Series</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1720374x62.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Localization domain for the Delta function</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/1-1720374x63.png"/></fig><p>Then for any distribution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x64.png" xlink:type="simple"/></inline-formula> Formula (2) can be expressed as</p><disp-formula id="scirp.61112-formula32"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x65.png"  xlink:type="simple"/></disp-formula><p>where f is acting to the test function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x66.png" xlink:type="simple"/></inline-formula> by the variable y.</p><p>Similarly, for the Fourier integral (3) we write</p><disp-formula id="scirp.61112-formula33"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x67.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x68.png" xlink:type="simple"/></inline-formula> the Bochner-Riesz means of the Fourier integral of the Dirac delta function:</p><disp-formula id="scirp.61112-formula34"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x69.png"  xlink:type="simple"/></disp-formula><p>Lemma 1 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x70.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x71.png" xlink:type="simple"/></inline-formula> be the Fourier transformation of the Riesz-Bochner kernel</p><p>(8). Then</p><disp-formula id="scirp.61112-formula35"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61112-formula36"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x73.png"  xlink:type="simple"/></disp-formula><p>Proof. From the definition of the kernel <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x74.png" xlink:type="simple"/></inline-formula> obviously obtain</p><disp-formula id="scirp.61112-formula37"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x75.png"  xlink:type="simple"/></disp-formula><p>Then estimate (9) immediately follows from (11). The estimate (10) follows from (8) and the estimate for the Bessel functions:</p><disp-formula id="scirp.61112-formula38"><graphic  xlink:href="http://html.scirp.org/file/1-1720374x76.png"  xlink:type="simple"/></disp-formula><p>Lemma 1 proved.</p><p>Note, that if a function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x77.png" xlink:type="simple"/></inline-formula> and its Fourier transformation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x78.png" xlink:type="simple"/></inline-formula> satisfy the estimates (9) and (10), then the Poisson formula for summation is valid:</p><disp-formula id="scirp.61112-formula39"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x79.png"  xlink:type="simple"/></disp-formula><p>Thus from Lemma 1 applying (12) for the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x80.png" xlink:type="simple"/></inline-formula> obtain</p><disp-formula id="scirp.61112-formula40"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x81.png"  xlink:type="simple"/></disp-formula><p>Then from (5) and (11) we have</p><disp-formula id="scirp.61112-formula41"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x82.png"  xlink:type="simple"/></disp-formula><p>In the sum of right hand side in (13) by separation term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x83.png" xlink:type="simple"/></inline-formula> obtain</p><disp-formula id="scirp.61112-formula42"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x84.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x85.png" xlink:type="simple"/></inline-formula> defined as</p><disp-formula id="scirp.61112-formula43"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x86.png"  xlink:type="simple"/></disp-formula><p>Then from Lemma 1 immediately follows:</p><p>Lemma 2 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x87.png" xlink:type="simple"/></inline-formula> Then uniformly in any compact set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x88.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.61112-formula44"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x89.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Proof of the Theorem 1</title><p>From the Formula (15) obtain</p><disp-formula id="scirp.61112-formula45"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x90.png"  xlink:type="simple"/></disp-formula><p>Then the statement of the Theorem 1 follows from the lemma below and equality (17):</p><p>Lemma 3 Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x91.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x92.png" xlink:type="simple"/></inline-formula> and let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x93.png" xlink:type="simple"/></inline-formula></p><p>Then</p><disp-formula id="scirp.61112-formula46"><graphic  xlink:href="http://html.scirp.org/file/1-1720374x94.png"  xlink:type="simple"/></disp-formula><p>uniformly in any compact set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x95.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. For any proper domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x96.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.61112-formula47"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x97.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x98.png" xlink:type="simple"/></inline-formula> means a norm in the space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x99.png" xlink:type="simple"/></inline-formula> taken with respect to the variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x100.png" xlink:type="simple"/></inline-formula>.</p><p>Note if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x101.png" xlink:type="simple"/></inline-formula>, then [<xref ref-type="bibr" rid="scirp.61112-ref19">19</xref>]</p><disp-formula id="scirp.61112-formula48"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x102.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x103.png" xlink:type="simple"/></inline-formula> means a norm in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-1720374x104.png" xlink:type="simple"/></inline-formula>.</p><p>Then the statement of the Lemma 4 follows from (19) and</p><disp-formula id="scirp.61112-formula49"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-1720374x105.png"  xlink:type="simple"/></disp-formula></sec><sec id="s6"><title>6. Conclusion</title><p>Equiconvergence of the Fourier series and integral of distributions depends on singularity of the distribution and power of regularisation as found in the main theorem. Obtained in Theorem 1 a relation for the singularity and summability index is accurate. However, to prove sharp result for the Reisz means below critical index for the smooth functions meets with some difficulties. This circumstance appears due to not applicability of the Poisson formula of summation.</p></sec><sec id="s7"><title>Acknowledgements</title><p>Ongoing research on the topics of the paper supported by IIUM FRGS 14 142 0383.</p></sec><sec id="s8"><title>Cite this paper</title><p>A. A. Rakhimov, (2015) On the Equiconvergence of the Fourier Series and Integral of Distributions. 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