<?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.2016.42049</article-id><article-id pub-id-type="publisher-id">JAMP-63982</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>
 
 
  The Exact Solutions of Such Coupled Linear Matrix Fractional Differential Equations of Diagonal Unknown Matrices by Using Hadamard Product
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ayed</surname><given-names>Al-Zuhiri</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>Zeyad</surname><given-names>Al-Zhour</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Khaled</surname><given-names>Jaber</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Basic Sciences and Humanities, College of Engineering, University of Dammam, Dammam, Saudi Arabia</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematics, Faculty of Science and Information Technology, Zarqa University, Zarqa, Jordan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>khaledjaber4@yahoo.com(KJ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>17</day><month>02</month><year>2016</year></pub-date><volume>04</volume><issue>02</issue><fpage>432</fpage><lpage>442</lpage><history><date date-type="received"><day>6</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>26</month>	<year>February</year>	</date><date date-type="accepted"><day>29</day>	<month>February</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we present the general exact solutions of such coupled system of matrix fractional differential equations for diagonal unknown matrices in Caputo sense by using vector extraction operators and Hadamard product. Some illustrated examples are also given to show our new approach.
 
</p></abstract><kwd-group><kwd>Fractional Operators</kwd><kwd> Matrix Fractional Differential Equations</kwd><kwd> Hadamard Product</kwd><kwd> Vector Extraction Operator</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Fractional calculus attracted the attention of researchers because of its application in physics as the nonlinear oscillation of earthquake can be modeled with fractional derivatives [<xref ref-type="bibr" rid="scirp.63982-ref1">1</xref>] , and the fluid-dynamic traffic model with fractional derivatives [<xref ref-type="bibr" rid="scirp.63982-ref2">2</xref>] can eliminate the deficiency arising from the assumption of continuum traffic flow. Based on experimental data fractional, partial differential equations for seepage flow in porous media are suggested in [<xref ref-type="bibr" rid="scirp.63982-ref3">3</xref>] , and differential equations with fractional order have recently proved to be valuable tools to the modeling of many physical phenomena [<xref ref-type="bibr" rid="scirp.63982-ref4">4</xref>] . A review of some applications of fractional derivatives in continuum and statistical mechanics is given by Mainardi [<xref ref-type="bibr" rid="scirp.63982-ref5">5</xref>] . The analytic results on the existence and uniqueness of solutions of the fractional differential equations have been investigated by many authors see as an example [<xref ref-type="bibr" rid="scirp.63982-ref6">6</xref>] . During the last decades, several methods have been used to solve fractional differential equations, fractional partial differential equations, fractional integro-differential equations and dynamic systems containing fractional derivatives, such as Adomian’s decomposition method [<xref ref-type="bibr" rid="scirp.63982-ref7">7</xref>] , variational iteration method [<xref ref-type="bibr" rid="scirp.63982-ref8">8</xref>] - [<xref ref-type="bibr" rid="scirp.63982-ref11">11</xref>] , homotopy perturbation method [<xref ref-type="bibr" rid="scirp.63982-ref12">12</xref>] , homotopy analysis method [<xref ref-type="bibr" rid="scirp.63982-ref13">13</xref>] , spectral methods [<xref ref-type="bibr" rid="scirp.63982-ref14">14</xref>] , and other methods [<xref ref-type="bibr" rid="scirp.63982-ref15">15</xref>] .</p><p>Recently, Wang [<xref ref-type="bibr" rid="scirp.63982-ref16">16</xref>] studied the synchronized motions in a star network of coupled fractional order systems in which the major element is coupled to each of the non-interacting individual elements and Kilicman and Al- Zhour [<xref ref-type="bibr" rid="scirp.63982-ref17">17</xref>] studied several operational matrices for fractional integration and differentiation and expanded the Kronecker convolution product to the Riemann-Liouville fractional integral of matrices. Al-Zhour [<xref ref-type="bibr" rid="scirp.63982-ref18">18</xref>] introduced the exact solution of coupled fractional order systems by using Kronecker structure.</p><p>In the present paper, the exact solutions of coupled and uncoupled systems of matrix fractional differential equations for diagonal unknown matrices are presented by using a new attractive method and some illustrated examples are also given to show our new approach.</p></sec><sec id="s2"><title>2. Basic Results and Preliminaries</title><p>In this section, we recall some basic results and definitions associated to Hadamard product, Mittage-Leffler function and Caputo fractional derivative that will be used to get our results later.</p><p>Definition 2.1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x6.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x7.png" xlink:type="simple"/></inline-formula>.Then the Hadamard product of A and B is defined by [<xref ref-type="bibr" rid="scirp.63982-ref19">19</xref>] - [<xref ref-type="bibr" rid="scirp.63982-ref26">26</xref>] .</p><disp-formula id="scirp.63982-formula846"><label>(2-1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x8.png"  xlink:type="simple"/></disp-formula><p>Definition 2.2. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x9.png" xlink:type="simple"/></inline-formula> be a diagonal matrix. Then the diagonal extraction operator of A is defined by [<xref ref-type="bibr" rid="scirp.63982-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.63982-ref23">23</xref>] .</p><disp-formula id="scirp.63982-formula847"><label>(2-2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x10.png"  xlink:type="simple"/></disp-formula><p>Theorem 2.3. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x11.png" xlink:type="simple"/></inline-formula> be diagonal matrices. Then</p><disp-formula id="scirp.63982-formula848"><label>(2-3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x12.png"  xlink:type="simple"/></disp-formula><p>Definition 2.4. The one parameter Mittage-Leffler functions and Mittage-Leffler matrix functions of matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x13.png" xlink:type="simple"/></inline-formula> are defined, respectively, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x14.png" xlink:type="simple"/></inline-formula> by [<xref ref-type="bibr" rid="scirp.63982-ref18">18</xref>] .</p><disp-formula id="scirp.63982-formula849"><label>(2-4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x15.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula850"><label>. (2-5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x16.png"  xlink:type="simple"/></disp-formula><p>Note that the Mittage-Leffler matrix function of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x17.png" xlink:type="simple"/></inline-formula> can be represented by using spectral decomposition method by [<xref ref-type="bibr" rid="scirp.63982-ref18">18</xref>] .</p><disp-formula id="scirp.63982-formula851"><label>(2-6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x18.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x19.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x20.png" xlink:type="simple"/></inline-formula> are the eigenvectors corresponding to the eigenvalue <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x21.png" xlink:type="simple"/></inline-formula> of A and A<sup>T</sup>, respectively.</p><p>Theorem 2.5. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x22.png" xlink:type="simple"/></inline-formula> is a diagonal matrix and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x23.png" xlink:type="simple"/></inline-formula>. Then [<xref ref-type="bibr" rid="scirp.63982-ref18">18</xref>]</p><disp-formula id="scirp.63982-formula852"><label>(2-7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x24.png"  xlink:type="simple"/></disp-formula><p>Definition 2.6. The Caputo fractional derivative of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x25.png" xlink:type="simple"/></inline-formula> with order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x26.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x27.png" xlink:type="simple"/></inline-formula>, is defined by [<xref ref-type="bibr" rid="scirp.63982-ref18">18</xref>] -[<xref ref-type="bibr" rid="scirp.63982-ref20">20</xref>] .</p><disp-formula id="scirp.63982-formula853"><label>(2-8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x28.png"  xlink:type="simple"/></disp-formula><p>Theorem 2.7. The relationship between the Mittage-Leffler function and Caputo derivative are given by:</p><p>a)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x29.png" xlink:type="simple"/></inline-formula> (2.9)</p><p>b)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x30.png" xlink:type="simple"/></inline-formula> (2.10)</p></sec><sec id="s3"><title>3. Main Results</title><p>In this section, we present the general exact solutions of the coupled and uncoupled system of fractional differential equations for diagonal unknown matrices by using the using vector extraction operators and Hadamard product.</p><p>Lemma 3.1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x31.png" xlink:type="simple"/></inline-formula> be a given scalar matrix, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x32.png" xlink:type="simple"/></inline-formula>be a given scalar vector,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x33.png" xlink:type="simple"/></inline-formula> be a given vector function and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x34.png" xlink:type="simple"/></inline-formula> be an unknown vector function to be solved. Then the exact solution of the following non-homogenous linear fractional system of order <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x35.png" xlink:type="simple"/></inline-formula> is given by [<xref ref-type="bibr" rid="scirp.63982-ref18">18</xref>] -[<xref ref-type="bibr" rid="scirp.63982-ref20">20</xref>] .</p><disp-formula id="scirp.63982-formula854"><label>(3-1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x36.png"  xlink:type="simple"/></disp-formula><p>is given by:</p><disp-formula id="scirp.63982-formula855"><label>(3-2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x37.png"  xlink:type="simple"/></disp-formula><p>Theorem 3.2. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x38.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x39.png" xlink:type="simple"/></inline-formula> be given diagonal scalar matrices, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x40.png" xlink:type="simple"/></inline-formula>be a given diagonal matrix function and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x41.png" xlink:type="simple"/></inline-formula> be an unknown diagonal matrix function. Then the general vector extraction solution of the following non-homogeneous matrix fractional differential equation</p><disp-formula id="scirp.63982-formula856"><label>(3-3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x42.png"  xlink:type="simple"/></disp-formula><p>is given by:</p><disp-formula id="scirp.63982-formula857"><label>(3-4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x43.png"  xlink:type="simple"/></disp-formula><p>Proof. By using (2-3), then (3.3) can be represented by:</p><disp-formula id="scirp.63982-formula858"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x44.png"  xlink:type="simple"/></disp-formula><p>Hence, the vector extraction solution of (3.3) is given by:</p><disp-formula id="scirp.63982-formula859"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x45.png"  xlink:type="simple"/></disp-formula><p>Theorem 3.3. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x46.png" xlink:type="simple"/></inline-formula> be given diagonal scalar matrices, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x47.png" xlink:type="simple"/></inline-formula> be an unknown diagonal matrix functions. Then the general vector extraction solution of the following general system of linear matrix fractional differential equations of order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x48.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63982-formula860"><label>(3-5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x49.png"  xlink:type="simple"/></disp-formula><p>is given by:</p><disp-formula id="scirp.63982-formula861"><label>(3-6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x50.png"  xlink:type="simple"/></disp-formula><p>Proof. By using (2-3), then (3.5) can be represented by:</p><disp-formula id="scirp.63982-formula862"><label>(3-7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x51.png"  xlink:type="simple"/></disp-formula><p>Now by letting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x52.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.63982-formula863"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x53.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x54.png" xlink:type="simple"/></inline-formula>. Then (3.7) can be written as:</p><disp-formula id="scirp.63982-formula864"><label>(3-8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x55.png"  xlink:type="simple"/></disp-formula><p>Hence by using Lemma 3.1 and simple computations, then we get the solution as in (3-6).</p><p>Below we will discuss some important special cases of the general system as in Theorem 3.3.</p><p>Theorem 3.4. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x56.png" xlink:type="simple"/></inline-formula> be given scalar diagonal matrices, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x57.png" xlink:type="simple"/></inline-formula>be diagonal matrix functions, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x58.png" xlink:type="simple"/></inline-formula> be unknown diagonal matrix functions. Then the general solutions of the following coupled matrix fractional differential equations of order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x59.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63982-formula865"><label>(3-9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x60.png"  xlink:type="simple"/></disp-formula><p>are given by:</p><disp-formula id="scirp.63982-formula866"><label>(3.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x61.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula867"><label>(3.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x62.png"  xlink:type="simple"/></disp-formula><p>Proof. By multiplying the second equation in (3-9) by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x63.png" xlink:type="simple"/></inline-formula>, we get:</p><disp-formula id="scirp.63982-formula868"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x64.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula869"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x65.png"  xlink:type="simple"/></disp-formula><p>Then (3-9) can be written as</p><disp-formula id="scirp.63982-formula870"><label>(3-12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x66.png"  xlink:type="simple"/></disp-formula><p>Now, by using <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x67.png" xlink:type="simple"/></inline-formula> of (3.12), then we get the following equivalent system:</p><disp-formula id="scirp.63982-formula871"><label>(3.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x68.png"  xlink:type="simple"/></disp-formula><p>Now by using (3-6), then the solution of (3.13) is given by:</p><disp-formula id="scirp.63982-formula872"><label>(3.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x69.png"  xlink:type="simple"/></disp-formula><p>Now we deal with</p><disp-formula id="scirp.63982-formula873"><label>(3.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x70.png"  xlink:type="simple"/></disp-formula><p>Since</p><disp-formula id="scirp.63982-formula874"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x71.png"  xlink:type="simple"/></disp-formula><p>Then</p><disp-formula id="scirp.63982-formula875"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x72.png"  xlink:type="simple"/></disp-formula><p>But</p><disp-formula id="scirp.63982-formula876"><label>(3.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x73.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.63982-formula877"><label>(3-17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x74.png"  xlink:type="simple"/></disp-formula><p>So,</p><disp-formula id="scirp.63982-formula878"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x75.png"  xlink:type="simple"/></disp-formula><p>(3.18)</p><p>Similarly,</p><disp-formula id="scirp.63982-formula879"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x76.png"  xlink:type="simple"/></disp-formula><p>(3.19)</p><p>Now from (3-13), (3-18) and (3-19), we get</p><disp-formula id="scirp.63982-formula880"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula881"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x78.png"  xlink:type="simple"/></disp-formula><p>Since,</p><disp-formula id="scirp.63982-formula882"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x79.png"  xlink:type="simple"/></disp-formula><p>Then, we get the vector extraction solution as in (3-11).</p><p>Corollary 3.5. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x80.png" xlink:type="simple"/></inline-formula> be given scalar diagonal matrices and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x81.png" xlink:type="simple"/></inline-formula> be an unknown diagonal matrix functions. Then the general vector extraction solutions of the following coupled matrix fractional differential equations of order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x82.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63982-formula883"><label>(3.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x83.png"  xlink:type="simple"/></disp-formula><p>are given by:</p><disp-formula id="scirp.63982-formula884"><label>(3.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x84.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula885"><label>(3.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x85.png"  xlink:type="simple"/></disp-formula><p>Proof. The proof is straightforward by applying Theorem 3.4 by letting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x86.png" xlink:type="simple"/></inline-formula> and by using the following fact:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x87.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Illustrated Examples</title><p>In the section, we give some illustrated examples to show our new approach as discussed in above section.</p><p>Example 4.1. Consider the following matrix linear fractional differential equation:</p><disp-formula id="scirp.63982-formula886"><label>(4-1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x88.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x89.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x90.png" xlink:type="simple"/></inline-formula> is diagonal matrix. Then the exact solution of (4-1) by applying Theorem 3.2 is given by:</p><disp-formula id="scirp.63982-formula887"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x91.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x92.png" xlink:type="simple"/></inline-formula>.</p><p>Example 4.2. Consider the following system of order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x93.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63982-formula888"><label>(4-2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x94.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x95.png" xlink:type="simple"/></inline-formula>. Then the system (4-2) can be rewritten as:</p><disp-formula id="scirp.63982-formula889"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x96.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula890"><label>(4-3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x97.png"  xlink:type="simple"/></disp-formula><p>Now the exact solution of (4-3) by applying Theorem 3.2 is given by:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x98.png" xlink:type="simple"/></inline-formula>.</p><p>Example 4.3. Consider the following matrix fractional differential equation:</p><disp-formula id="scirp.63982-formula891"><label>(4-4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x99.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x100.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x101.png" xlink:type="simple"/></inline-formula> is diagonal matrix. Then the exact solution of (4-4) by applying Theorem 3.2 is given by:</p><disp-formula id="scirp.63982-formula892"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x102.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x103.png" xlink:type="simple"/></inline-formula>.</p><p>Example 4.4. Consider the following matrix fractional differential equations of order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x104.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.63982-formula893"><label>(4-5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x105.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x106.png" xlink:type="simple"/></inline-formula> are diagonal matrices. So</p><disp-formula id="scirp.63982-formula894"><label>. (4-6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x107.png"  xlink:type="simple"/></disp-formula><p>Then the exact solution of (4-5) by applying Corollary 3.5 is given by:</p><disp-formula id="scirp.63982-formula895"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x108.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula896"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x109.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula897"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x110.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/20-1720366x111.png" xlink:type="simple"/></inline-formula>.</p><p>Example 4.5. Consider the following coupled matrix fractional differential equations:</p><disp-formula id="scirp.63982-formula898"><label>. (4-7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/20-1720366x112.png"  xlink:type="simple"/></disp-formula><p>Then the exact solution by applying Corollary 3.5 is given by:</p><disp-formula id="scirp.63982-formula899"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x113.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.63982-formula900"><graphic  xlink:href="http://html.scirp.org/file/20-1720366x114.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Conclusion</title><p>The general exact solutions of coupled system of matrix fractional differential equations with diagonal matrices coefficients by using vector extraction operators and Hadamard product in Caputo sense are presented with some illustrated examples. How to find the complexity of this method requires further research.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors express their sincere thanks to referees for very careful reading and helpful suggestion of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>ZayedAl-Zuhiri,ZeyadAl-Zhour,KhaledJaber, (2016) The Exact Solutions of Such Coupled Linear Matrix Fractional Differential Equations of Diagonal Unknown Matrices by Using Hadamard Product. Journal of Applied Mathematics and Physics,04,432-442. doi: 10.4236/jamp.2016.42049</p></sec></body><back><ref-list><title>References</title><ref id="scirp.63982-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">He, J. (1998) Nonlinear Oscillation with Fractional Derivative and Its Applications. 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