<?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.2016.714129</article-id><article-id pub-id-type="publisher-id">AM-69827</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>
 
 
  Dirichlet Averages, Fractional Integral Operators and Solution of Euler-Darboux Equation on H&amp;ouml;lder Spaces
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>D.</surname><given-names>N. Vyas</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Basic &amp;amp; Applied Sciences, M. L. V. Textile &amp;amp; Engineering College, Bhilwara, India</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>17</day><month>08</month><year>2016</year></pub-date><volume>07</volume><issue>14</issue><fpage>1498</fpage><lpage>1503</lpage><history><date date-type="received"><day>2</day>	<month>June</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>14</month>	<year>August</year>	</date><date date-type="accepted"><day>17</day>	<month>August</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>
 
 
  In the present paper, we discuss the solution of Euler-Darboux equation in terms of Dirichlet averages of boundary conditions on H
  ?lder space and weighted H
  ?lder spaces of continuous functions using Riemann-Liouville fractional integral operators. Moreover, the results are interpreted in alternative form.
 
</p></abstract><kwd-group><kwd>Fractional Integral Operators</kwd><kwd> Dirichlet Averages</kwd><kwd> H&#246;lder Space</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The subject of Dirichlet averages has received momentum in the last decade of 20th century with reference to the solution of certain partial differential equations. Not much work has been registered in this area of Applied Mathematics except some papers devoted to evaluation of Dirichlet averages of elementary functions as well as higher treanscendental functions interpreting the results in more general special functions. The present paper is ventured to give the interpretation of solution of a typical partial differential equation and prove its inclusion properties with respect to H&#246;lder spaces. The Euler-Darboux equation (ED-equation) is a certain kind of degenerate hyperbolic partial differential equation of the type (see Nahušev [<xref ref-type="bibr" rid="scirp.69827-ref1">1</xref>] ),</p><disp-formula id="scirp.69827-formula582"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x6.png"  xlink:type="simple"/></disp-formula><p>Saigo [<xref ref-type="bibr" rid="scirp.69827-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.69827-ref4">4</xref>] considered and studied the ED-equation given by</p><disp-formula id="scirp.69827-formula583"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x7.png"  xlink:type="simple"/></disp-formula><p>which implies the Equation (1) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x8.png" xlink:type="simple"/></inline-formula> or some other degenerate hyperbolic equations described</p><p>by characteristic coordinates. The boundary conditions used for the solution of Equation (2) are</p><disp-formula id="scirp.69827-formula584"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x9.png"  xlink:type="simple"/></disp-formula><p>The solution of ED-Equation (2), due to Saigo [<xref ref-type="bibr" rid="scirp.69827-ref22">22</xref>] , is given by</p><disp-formula id="scirp.69827-formula585"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x10.png"  xlink:type="simple"/></disp-formula><p>where x and y are restricted in the domain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x11.png" xlink:type="simple"/></inline-formula>.</p><p>Srivastava and Saigo [<xref ref-type="bibr" rid="scirp.69827-ref5">5</xref>] evaluated the results on multiplication of fractional integral operators and the solution of ED-equation. Deora and Banerji [<xref ref-type="bibr" rid="scirp.69827-ref6">6</xref>] represented the solution of Equation (2) in terms of Dirichlet averages of boundary condition functions given in (3) as follows</p><disp-formula id="scirp.69827-formula586"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x12.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x13.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x14.png" xlink:type="simple"/></inline-formula> denote the single Dirichlet averages of boundary functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x15.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x16.png" xlink:type="simple"/></inline-formula>, respectively.</p><p>Kilbas et al. [<xref ref-type="bibr" rid="scirp.69827-ref7">7</xref>] studied the solution of ED-equation on H&#246;lder Space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x17.png" xlink:type="simple"/></inline-formula> or simply <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x18.png" xlink:type="simple"/></inline-formula> as well as on weighted H&#246;lder Space of continuous functions. In the present paper we discuss the Dirichlet averages on H&#246;lder Space via right-sided Riemann-Liouville fractional integral operators and prove the solution of Equation (2) to be justified on such spaces. In what follows are the preliminaries and definitions related to fractional integral operators, Dirichlet averages, and H&#246;lder spaces of continuous functions.</p></sec><sec id="s2"><title>2. H&#246;lder Spaces</title><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x19.png" xlink:type="simple"/></inline-formula> and a finite interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x20.png" xlink:type="simple"/></inline-formula> we denote by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x21.png" xlink:type="simple"/></inline-formula> the space of H&#246;lder function on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x22.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.69827-formula587"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x23.png"  xlink:type="simple"/></disp-formula><p>if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x24.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x25.png" xlink:type="simple"/></inline-formula>, i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x26.png" xlink:type="simple"/></inline-formula>is m-times differentiable function and its m-th derivative is continuous and satisfies the inequality</p><disp-formula id="scirp.69827-formula588"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x27.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x28.png" xlink:type="simple"/></inline-formula> for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x29.png" xlink:type="simple"/></inline-formula>.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x30.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x31.png" xlink:type="simple"/></inline-formula>, i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x32.png" xlink:type="simple"/></inline-formula>be the space of H&#246;lder continuous functions and</p><disp-formula id="scirp.69827-formula589"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x33.png"  xlink:type="simple"/></disp-formula><p>Then we denote by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x34.png" xlink:type="simple"/></inline-formula> the space of functions such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x35.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x36.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Dirichlet Averages</title><p>Carlson [<xref ref-type="bibr" rid="scirp.69827-ref8">8</xref>] introduced the concept of connecting elementary functions with higher transcendental functions using averaging technique. The Dirichlet average is a certain kind of integral average with respect to Dirichlet measure, which in Statistics called as beta distribution of several variables. One may refer to Banerji and Deora [<xref ref-type="bibr" rid="scirp.69827-ref9">9</xref>] , Deora and Banerji [<xref ref-type="bibr" rid="scirp.69827-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.69827-ref11">11</xref>] , Deora, Banerji and Saigo [<xref ref-type="bibr" rid="scirp.69827-ref12">12</xref>] , Gupta and Agrawal [<xref ref-type="bibr" rid="scirp.69827-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.69827-ref14">14</xref>] , Kattuveettil [<xref ref-type="bibr" rid="scirp.69827-ref15">15</xref>] , Prabhakar [<xref ref-type="bibr" rid="scirp.69827-ref16">16</xref>] , Chena Ram et al. [<xref ref-type="bibr" rid="scirp.69827-ref17">17</xref>] , Vyas [<xref ref-type="bibr" rid="scirp.69827-ref18">18</xref>] , Vyas and Banerji [<xref ref-type="bibr" rid="scirp.69827-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.69827-ref20">20</xref>] , Vyas, Banerji and Saigo [<xref ref-type="bibr" rid="scirp.69827-ref21">21</xref>] .</p><p>Standard Simplex: Denote the standard simplex in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x37.png" xlink:type="simple"/></inline-formula> by</p><disp-formula id="scirp.69827-formula590"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x38.png"  xlink:type="simple"/></disp-formula><p>Beta Function of k-variables: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x39.png" xlink:type="simple"/></inline-formula> denotes the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x40.png" xlink:type="simple"/></inline-formula> cartesian product of open right half plane and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x41.png" xlink:type="simple"/></inline-formula> is the standard simplex in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x42.png" xlink:type="simple"/></inline-formula>. The beta function of k-variables can be expressed as</p><disp-formula id="scirp.69827-formula591"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x43.png"  xlink:type="simple"/></disp-formula><p>Dirichlet Measure: The complex measure<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x44.png" xlink:type="simple"/></inline-formula>, defind on E by</p><disp-formula id="scirp.69827-formula592"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x45.png"  xlink:type="simple"/></disp-formula><p>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x46.png" xlink:type="simple"/></inline-formula>, is called the Dirichlet measure. Particularly, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x47.png" xlink:type="simple"/></inline-formula>, we write by using (3), the following:</p><disp-formula id="scirp.69827-formula593"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x48.png"  xlink:type="simple"/></disp-formula><p>Dirichlet Average: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x49.png" xlink:type="simple"/></inline-formula> be a convex set in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x50.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x51.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x52.png" xlink:type="simple"/></inline-formula> denotes a convex linear combination of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x53.png" xlink:type="simple"/></inline-formula>. Then the Dirichlet average of a holomorphic function f is defined by (See Carlson [<xref ref-type="bibr" rid="scirp.69827-ref22">22</xref>] )</p><disp-formula id="scirp.69827-formula594"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x54.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x55.png" xlink:type="simple"/></inline-formula> denotes the parameters. The convex combination is given by</p><disp-formula id="scirp.69827-formula595"><graphic  xlink:href="http://html.scirp.org/file/4-7403229x56.png"  xlink:type="simple"/></disp-formula><p>Particularly,when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x57.png" xlink:type="simple"/></inline-formula>, the Dirichlet average, so extracted out of (5), is called the single Dirichlet average of f over the line segment from 0 to 1. It is expressed as</p><disp-formula id="scirp.69827-formula596"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x58.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x59.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x60.png" xlink:type="simple"/></inline-formula>.</p><p>If we consider the continuous function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x61.png" xlink:type="simple"/></inline-formula> in H&#246;lder Space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x62.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x63.png" xlink:type="simple"/></inline-formula>, then without the loss of characteristics of such spaces, the Dirichlet average of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x64.png" xlink:type="simple"/></inline-formula> is defined by</p><disp-formula id="scirp.69827-formula597"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x65.png"  xlink:type="simple"/></disp-formula><p>and for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x66.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x67.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x68.png" xlink:type="simple"/></inline-formula>. The equation analogous to (11), is expressed as</p><disp-formula id="scirp.69827-formula598"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x69.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x70.png" xlink:type="simple"/></inline-formula> denotes the single Dirichlet average of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x71.png" xlink:type="simple"/></inline-formula> in two variables x and y in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x72.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Fractional Integral Operators</title><p>Fractional calculus is the generalization of ordinary n-times iterated integrals and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x73.png" xlink:type="simple"/></inline-formula> derivatives of continuous functions to that of any arbitrary order real or complex. The most commonly used definition of fractional integral operators of order a is due to Riemann-Liouville. A detailed account of fractional calculus is given in Samko et al. [<xref ref-type="bibr" rid="scirp.69827-ref23">23</xref>] and the applications of it are elaborated in Hilfer [<xref ref-type="bibr" rid="scirp.69827-ref24">24</xref>] and Podlubney [<xref ref-type="bibr" rid="scirp.69827-ref25">25</xref>] . Vyas [<xref ref-type="bibr" rid="scirp.69827-ref26">26</xref>] interpreted the angle of collision occurring in the study of transport properties of Noble gases at low density configuration in terms of Fractional Integral Operators.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x74.png" xlink:type="simple"/></inline-formula> be the H&#246;lderian class of continuous functions and the weighted H&#246;lder space be defined in (8). Then the right-sided Riemann-Liouville fractional integral operators are defined by</p><disp-formula id="scirp.69827-formula599"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69827-formula600"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69827-formula601"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69827-formula602"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x78.png"  xlink:type="simple"/></disp-formula><p>Proposition 1: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x79.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x80.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x81.png" xlink:type="simple"/></inline-formula>. Then for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x82.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.69827-formula603"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x83.png"  xlink:type="simple"/></disp-formula><p>Proposition 2: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x84.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x85.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x86.png" xlink:type="simple"/></inline-formula>. Then for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x87.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.69827-formula604"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x88.png"  xlink:type="simple"/></disp-formula><p>Generalization of fractional integral operators is due to Saigo [<xref ref-type="bibr" rid="scirp.69827-ref27">27</xref>] . Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x89.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x90.png" xlink:type="simple"/></inline-formula> be real numbers and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x91.png" xlink:type="simple"/></inline-formula> be the Gauss’ hypergeometric function. One may refer Erd&#233;lyi [<xref ref-type="bibr" rid="scirp.69827-ref28">28</xref>] [<xref ref-type="bibr" rid="scirp.69827-ref29">29</xref>] and Slater [<xref ref-type="bibr" rid="scirp.69827-ref30">30</xref>] . Then the fractional integral operator involving Gauss’ hypergeometric function on H&#246;lder space is defined by</p><disp-formula id="scirp.69827-formula605"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x92.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69827-formula606"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x93.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69827-formula607"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x94.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.69827-formula608"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x95.png"  xlink:type="simple"/></disp-formula><p>Proposition 3: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x96.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x97.png" xlink:type="simple"/></inline-formula>. Then for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x98.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.69827-formula609"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x99.png"  xlink:type="simple"/></disp-formula><p>Proposition 4: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x100.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x101.png" xlink:type="simple"/></inline-formula>. Then for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x102.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.69827-formula610"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x103.png"  xlink:type="simple"/></disp-formula><p>By setting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x104.png" xlink:type="simple"/></inline-formula>, the generalized fractional integral operators defined in (23) to (26) reduce to right-sided Riemann-Liouville fractional integral operators defined in (17) to (20).</p></sec><sec id="s5"><title>5. Main Results</title><p>Theorem 1: Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x105.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x106.png" xlink:type="simple"/></inline-formula>. Then the single Dirichlet average of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x107.png" xlink:type="simple"/></inline-formula> is expressed as</p><disp-formula id="scirp.69827-formula611"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x108.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x109.png" xlink:type="simple"/></inline-formula> is the right-sided Riemann-Liouville fractional integral operator defined in (17).</p><p>Proof: Using Equation (16), we write</p><disp-formula id="scirp.69827-formula612"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x110.png"  xlink:type="simple"/></disp-formula><p>Using the transformation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x111.png" xlink:type="simple"/></inline-formula> in (30) and adjusting the terms involved, we obtain</p><disp-formula id="scirp.69827-formula613"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x112.png"  xlink:type="simple"/></disp-formula><p>which upon using (17), can be expressed as</p><disp-formula id="scirp.69827-formula614"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x113.png"  xlink:type="simple"/></disp-formula><p>which, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x114.png" xlink:type="simple"/></inline-formula>, can also be put in the form</p><disp-formula id="scirp.69827-formula615"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x115.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x116.png" xlink:type="simple"/></inline-formula> denotes the new fractional operator defined by</p><disp-formula id="scirp.69827-formula616"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x117.png"  xlink:type="simple"/></disp-formula><p>Owing to the proposition 1 to proposition 4 we conclude the proof of theorem 1.</p><p>Corollary 1: If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x118.png" xlink:type="simple"/></inline-formula> and restrictions on parmeters hold true, then for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x119.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.69827-formula617"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-7403229x120.png"  xlink:type="simple"/></disp-formula><p>Proof: Invoking the proposition 1 and using the result (32), we find that the fractional integral representation of single Dirichlet average of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x121.png" xlink:type="simple"/></inline-formula>, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x122.png" xlink:type="simple"/></inline-formula> gives rise to the result (35). This justifies that the Dirichlet averages, so evaluated, belong to the H&#246;lderian class.</p><p>Theorem 2: Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula> denote the Dirichlet averages of boundary functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x126.png" xlink:type="simple"/></inline-formula>, respectively associatd with the ED-Equation (2) and if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x127.png" xlink:type="simple"/></inline-formula> denotes the solution of ED-equation, given by (5), in terms of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x128.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x129.png" xlink:type="simple"/></inline-formula>. Then, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x130.png" xlink:type="simple"/></inline-formula>, the solution belongs to the H&#246;lderian class<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403229x131.png" xlink:type="simple"/></inline-formula>.</p><p>Proof: Using Equation (5), Theorem 1 and the Corollary 1, theorem 2 can be proved easily under the proposition 4.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The author is indebted to P. K. Banerji, Jodhpur, India for fruitful discussions during the preparation of this paper. Financial support under Technical Education Quality Improvement Programme (TEQIP)-II, a programme of Ministry of Human Resource Development, Government of India is highly acknowledged. Author is also thankful to worthy refree for his/her valuable suggestions upon improvement.</p></sec><sec id="s7"><title>Cite this paper</title><p>D. N. Vyas, (2016) Dirichlet Averages, Fractional Integral Operators and Solution of Euler-Darboux Equation on H&amp;ouml;lder Spaces. Applied Mathematics,07,1498-1503. doi: 10.4236/am.2016.714129</p></sec></body><back><ref-list><title>References</title><ref id="scirp.69827-ref1"><label>1</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Nahusev</surname><given-names> A.M. </given-names></name>,<etal>et al</etal>. 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