<?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">ICA</journal-id><journal-title-group><journal-title>Intelligent Control and Automation</journal-title></journal-title-group><issn pub-type="epub">2153-0653</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ica.2014.54028</article-id><article-id pub-id-type="publisher-id">ICA-51567</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  An Optimization Problem of Boundary Type for Cooperative Hyperbolic Systems Involving Schr&amp;#246;dinger Operator
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hlam</surname><given-names>Hasan Qamlo</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 Mathematics, Faculty of Applied sciences, Umm AL-Qura University, Makkah, KSA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>drahqamlo@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>15</day><month>10</month><year>2014</year></pub-date><volume>05</volume><issue>04</issue><fpage>262</fpage><lpage>271</lpage><history><date date-type="received"><day>16</day>	<month>September</month>	<year>2014</year></date><date date-type="rev-recd"><day>10</day>	<month>October</month>	<year>2014</year>	</date><date date-type="accepted"><day>25</day>	<month>October</month>	<year>2014</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 consider cooperative hyperbolic systems involving Schr
  ?dinger operator defined on  R
  <sup>n</sup>. First we prove the existence and uniqueness of the state for these systems. Then we find the necessary and sufficient conditions of optimal control for such systems of the boundary type. We also find the necessary and sufficient conditions of optimal control for same systems when the observation is on the boundary. 
 
</p></abstract><kwd-group><kwd>Hyperbolic Systems</kwd><kwd> Schr&#246;dinger Operator</kwd><kwd> Boundary Control Problem</kwd><kwd> Boundary Observation</kwd><kwd> Cooperative</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The optimal control problems of distributed systems involving Schr&#246;dinger operator have been widely discussed in many papers. One of the first studies was introduced by Serag [<xref ref-type="bibr" rid="scirp.51567-ref1">1</xref>] , which discusses 2 &#215; 2 cooperative systems of elliptic operator. Further research in this area developed the problem by studying different operator types (el- liptic, parabolic, or hyperbolic) or higher system degree as in [<xref ref-type="bibr" rid="scirp.51567-ref2">2</xref>] - [<xref ref-type="bibr" rid="scirp.51567-ref6">6</xref>] . Many boundary control problems have been introduced in [<xref ref-type="bibr" rid="scirp.51567-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.51567-ref10">10</xref>] .</p><p>In [<xref ref-type="bibr" rid="scirp.51567-ref3">3</xref>] , we discussed distributed control problem for 2 &#215; 2 cooperative hyperbolic systems involving Schr&#246;- dinger operator.</p><p>Here, using the theory of [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] , we consider the following 2 &#215; 2 cooperative hyperbolic systems involving Schr&#246;- dinger operator:</p><disp-formula id="scirp.51567-formula100"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x6.png"  xlink:type="simple"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x7.png" xlink:type="simple"/></inline-formula>.</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x8.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x10.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x11.png" xlink:type="simple"/></inline-formula> are given numbers such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x12.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x13.png" xlink:type="simple"/></inline-formula>,</p><p>i.e. the system (1) is called cooperative (2)</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x14.png" xlink:type="simple"/></inline-formula>is a positive function and tending to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x15.png" xlink:type="simple"/></inline-formula> at infinity, (3)</p><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x16.png" xlink:type="simple"/></inline-formula> with boundary<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x17.png" xlink:type="simple"/></inline-formula>.</p><p>The model of the system (1) is given by:</p><disp-formula id="scirp.51567-formula101"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x18.png"  xlink:type="simple"/></disp-formula><p>since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x19.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x20.png" xlink:type="simple"/></inline-formula>.</p><p>We first prove the existence and uniqueness of the state for these systems, then we introduce the optimality conditions of boundary control, we also discuss them when the observation is on the boundary.</p></sec><sec id="s2"><title>2. Some Concepts and Results</title><p>Here we shall consider some results about the following eigenvalue problem which introduced in [<xref ref-type="bibr" rid="scirp.51567-ref1">1</xref>] and [<xref ref-type="bibr" rid="scirp.51567-ref12">12</xref>] :</p><disp-formula id="scirp.51567-formula102"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x21.png"  xlink:type="simple"/></disp-formula><p>The associated space is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x22.png" xlink:type="simple"/></inline-formula>, with respect to the norm:</p><disp-formula id="scirp.51567-formula103"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x23.png"  xlink:type="simple"/></disp-formula><p>Since the imbedding of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x24.png" xlink:type="simple"/></inline-formula> into <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x25.png" xlink:type="simple"/></inline-formula> is compact, then the operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x26.png" xlink:type="simple"/></inline-formula> considered as an</p><p>Operator in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x27.png" xlink:type="simple"/></inline-formula> is positive self-adjoint with compact inverse. Hence its spectrum consists of an infinite se- quence of positive eigenvalues, tending to infinity; moreover the smallest one which is called the principal ei- genvalue denoted by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x28.png" xlink:type="simple"/></inline-formula> is simple and is associated with an eigenfunction which does not change sign in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x29.png" xlink:type="simple"/></inline-formula>. It is characterized by:</p><disp-formula id="scirp.51567-formula104"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x30.png"  xlink:type="simple"/></disp-formula><p>We have:</p><disp-formula id="scirp.51567-formula105"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x31.png"  xlink:type="simple"/></disp-formula><p>which is continuous and compact.</p><p>Let us introduce the space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x32.png" xlink:type="simple"/></inline-formula> of measurable function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x33.png" xlink:type="simple"/></inline-formula> which is defined on open interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x34.png" xlink:type="simple"/></inline-formula> and the variable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x35.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x36.png" xlink:type="simple"/></inline-formula>denotes the time.</p><p>On <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x37.png" xlink:type="simple"/></inline-formula> with Lebesgue measure <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x38.png" xlink:type="simple"/></inline-formula> we have the norm:</p><disp-formula id="scirp.51567-formula106"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x39.png"  xlink:type="simple"/></disp-formula><p>and the scalar product</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x40.png" xlink:type="simple"/></inline-formula>,</p><p>the space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x41.png" xlink:type="simple"/></inline-formula> with the scalar product and the norm above is a Hilbert space.</p><p>Analogously, we can define the spaces<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x42.png" xlink:type="simple"/></inline-formula>,</p><p>with the scalar product:</p><disp-formula id="scirp.51567-formula107"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x43.png"  xlink:type="simple"/></disp-formula><p>then we have:</p><disp-formula id="scirp.51567-formula108"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x44.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. The Existence and Uniqueness for the State of the System (1)</title><p>We have the bilinear form:</p><disp-formula id="scirp.51567-formula109"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x45.png"  xlink:type="simple"/></disp-formula><p>For all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x46.png" xlink:type="simple"/></inline-formula> the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x47.png" xlink:type="simple"/></inline-formula> is measurable on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x48.png" xlink:type="simple"/></inline-formula>.</p><p>The coerciveness condition of the bilinear form (7) in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x49.png" xlink:type="simple"/></inline-formula> has been proved by Serag [<xref ref-type="bibr" rid="scirp.51567-ref1">1</xref>] , by using the</p><p>conditions for having the maximum principle for cooperative system (1) which have been obtained by Fleckinger [<xref ref-type="bibr" rid="scirp.51567-ref13">13</xref>] , and take the form:</p><disp-formula id="scirp.51567-formula110"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x50.png"  xlink:type="simple"/></disp-formula><p>that means:</p><disp-formula id="scirp.51567-formula111"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x51.png"  xlink:type="simple"/></disp-formula><p>Theorem (3.1):</p><p>Under the hypotheses (2) and (9), if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x52.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x53.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x54.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x55.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x56.png" xlink:type="simple"/></inline-formula>, then there exists a unique solution: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x57.png" xlink:type="simple"/></inline-formula>for system (1).</p><p>Proof:</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x58.png" xlink:type="simple"/></inline-formula> be a continuous linear form defined on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x59.png" xlink:type="simple"/></inline-formula> by:</p><disp-formula id="scirp.51567-formula112"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x60.png"  xlink:type="simple"/></disp-formula><p>then by Lax-Milgram lemma, there exists a unique element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x61.png" xlink:type="simple"/></inline-formula> such that:</p><disp-formula id="scirp.51567-formula113"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x62.png"  xlink:type="simple"/></disp-formula><p>Now, let us multiply both sides of first equation of system (1) by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x63.png" xlink:type="simple"/></inline-formula>, and the second equation by: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x64.png" xlink:type="simple"/></inline-formula>then integration over<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x65.png" xlink:type="simple"/></inline-formula>, we have:</p><disp-formula id="scirp.51567-formula114"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x66.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51567-formula115"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x67.png"  xlink:type="simple"/></disp-formula><p>By applying Green’s formula:</p><disp-formula id="scirp.51567-formula116"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x68.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51567-formula117"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x69.png"  xlink:type="simple"/></disp-formula><p>By sum the two equations we get:</p><disp-formula id="scirp.51567-formula118"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x70.png"  xlink:type="simple"/></disp-formula><p>by comparing the previous equation with (7), (10) and (11) we deduce that:</p><disp-formula id="scirp.51567-formula119"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x71.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.51567-formula120"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x72.png"  xlink:type="simple"/></disp-formula><p>then the proof is complete.</p></sec><sec id="s4"><title>4. Formulation of the Control Problem</title><p>The space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x73.png" xlink:type="simple"/></inline-formula> is the space of controls. For a control<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x74.png" xlink:type="simple"/></inline-formula>, the state <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x75.png" xlink:type="simple"/></inline-formula> of the system is given by the solution of</p><disp-formula id="scirp.51567-formula121"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x76.png"  xlink:type="simple"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x77.png" xlink:type="simple"/></inline-formula>.</p><p>The observation equation is given by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x78.png" xlink:type="simple"/></inline-formula>.</p><p>For a given<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x79.png" xlink:type="simple"/></inline-formula>, the cost function is given by:</p><disp-formula id="scirp.51567-formula122"><label>. (13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x80.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x81.png" xlink:type="simple"/></inline-formula> is hermitian positive definite operator:</p><disp-formula id="scirp.51567-formula123"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x82.png"  xlink:type="simple"/></disp-formula><p>The control problem then is to find <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x83.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x84.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x85.png" xlink:type="simple"/></inline-formula> is a closed con-</p><p>vex subset of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x86.png" xlink:type="simple"/></inline-formula>.</p><p>Since the cost function (14) can be written as (see [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] ):</p><disp-formula id="scirp.51567-formula124"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x87.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x88.png" xlink:type="simple"/></inline-formula> is a continuous coercive bilinear form and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x89.png" xlink:type="simple"/></inline-formula> is a continuous linear form on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x89.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x90.png" xlink:type="simple"/></inline-formula>.</p><p>Then there exists a unique optimal control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x91.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x92.png" xlink:type="simple"/></inline-formula> for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x93.png" xlink:type="simple"/></inline-formula> by using the general theory of Lions [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] . Moreover, we have the following theorem which gives the necessary and sufficient conditions of optimality:</p><p>Theorem (4.1):</p><p>Assume that (9) and (14) hold. If the cost function is given by (13), the optimal control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x94.png" xlink:type="simple"/></inline-formula> is then characterized by the following equations and inequalities:</p><disp-formula id="scirp.51567-formula125"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x95.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x96.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.51567-formula126"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x97.png"  xlink:type="simple"/></disp-formula><p>together with (12) , where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x98.png" xlink:type="simple"/></inline-formula> is the adjoint state.</p><p>Proof:</p><p>The optimal control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x99.png" xlink:type="simple"/></inline-formula> is characterized by [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>]</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x100.png" xlink:type="simple"/></inline-formula>,</p><p>Which is equivalent to:</p><disp-formula id="scirp.51567-formula127"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x101.png"  xlink:type="simple"/></disp-formula><p>i.e.</p><disp-formula id="scirp.51567-formula128"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x102.png"  xlink:type="simple"/></disp-formula><p>this inequality can be written as:</p><disp-formula id="scirp.51567-formula129"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x103.png"  xlink:type="simple"/></disp-formula><p>Now, since:</p><disp-formula id="scirp.51567-formula130"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x104.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.51567-formula131"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x105.png"  xlink:type="simple"/></disp-formula><p>by using Green formula and (12), we have:</p><disp-formula id="scirp.51567-formula132"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x106.png"  xlink:type="simple"/></disp-formula><p>then</p><disp-formula id="scirp.51567-formula133"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x107.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x108.png" xlink:type="simple"/></inline-formula></p><p>since the adjoint equation takes the form [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] : <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x109.png" xlink:type="simple"/></inline-formula></p><p>and from theorem (3.1), we have a unique solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x110.png" xlink:type="simple"/></inline-formula> which satisfies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x111.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x112.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x113.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x111.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x114.png" xlink:type="simple"/></inline-formula>.</p><p>This proves system (15).</p><p>Now, we transform (18) by using (15) as follows:</p><disp-formula id="scirp.51567-formula134"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x115.png"  xlink:type="simple"/></disp-formula><p>Using Green formula, we obtain:</p><disp-formula id="scirp.51567-formula135"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x116.png"  xlink:type="simple"/></disp-formula><p>Using (12), we have:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x117.png" xlink:type="simple"/></inline-formula>.</p><p>Thus the proof is complete.</p></sec><sec id="s5"><title>5. Formulation of the Problem When the Observation Is on the Boundary</title><p>The observation equation is given by:</p><disp-formula id="scirp.51567-formula136"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x118.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x119.png" xlink:type="simple"/></inline-formula>.</p><p>This is interpreted as follows [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] : we take the trace of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x120.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x121.png" xlink:type="simple"/></inline-formula>, which is particular in<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x122.png" xlink:type="simple"/></inline-formula>. Let this be denoted by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x123.png" xlink:type="simple"/></inline-formula>.</p><p>For a given<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x124.png" xlink:type="simple"/></inline-formula>, the cost function is given by:</p><disp-formula id="scirp.51567-formula137"><label>. (19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x125.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x126.png" xlink:type="simple"/></inline-formula> is defined as in (14).</p><p>The control problem then is to find <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x127.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x128.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x127.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x129.png" xlink:type="simple"/></inline-formula> is a closed con-</p><p>vex subset of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x130.png" xlink:type="simple"/></inline-formula>.</p><p>Since the cost function (19) can be written as [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] :</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x131.png" xlink:type="simple"/></inline-formula>,</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x132.png" xlink:type="simple"/></inline-formula> is a continuous coercive bilinear form and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x133.png" xlink:type="simple"/></inline-formula> is a continuous linear form on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x134.png" xlink:type="simple"/></inline-formula>. Then using the general theory of Lions [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] , there exists a unique optimal control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x135.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x136.png" xlink:type="simple"/></inline-formula> for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x137.png" xlink:type="simple"/></inline-formula>. Moreover, we have the following theorem which gives the necessary and suf-</p><p>ficient conditions of optimality:</p><p>Theorem (5.1):</p><p>Assume that (9) and (14) hold. If the cost function is given by (19), the optimal control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x138.png" xlink:type="simple"/></inline-formula></p><p>is then characterized by the following equations and inequalities:</p><disp-formula id="scirp.51567-formula138"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x139.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x140.png" xlink:type="simple"/></inline-formula> together with (16) and (12).</p><p>Proof:</p><p>The optimal control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x141.png" xlink:type="simple"/></inline-formula> is characterized by [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] :</p><disp-formula id="scirp.51567-formula139"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x142.png"  xlink:type="simple"/></disp-formula><p>Which is equivalent to:</p><disp-formula id="scirp.51567-formula140"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x143.png"  xlink:type="simple"/></disp-formula><p>i.e.</p><disp-formula id="scirp.51567-formula141"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x144.png"  xlink:type="simple"/></disp-formula><p>this inequality can be written as:</p><disp-formula id="scirp.51567-formula142"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/9-7900372x145.png"  xlink:type="simple"/></disp-formula><p>since the adjoint system takes the form [<xref ref-type="bibr" rid="scirp.51567-ref11">11</xref>] :</p><disp-formula id="scirp.51567-formula143"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x146.png"  xlink:type="simple"/></disp-formula><p>and from theorem (3.1), we get a unique solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x147.png" xlink:type="simple"/></inline-formula> which satisfies: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x148.png" xlink:type="simple"/></inline-formula>.</p><p>This proves system (20).</p><p>Now, we transform (22) by using (20) as follows:</p><disp-formula id="scirp.51567-formula144"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x149.png"  xlink:type="simple"/></disp-formula><p>Using Green formula, we obtain:</p><disp-formula id="scirp.51567-formula145"><graphic  xlink:href="http://html.scirp.org/file/9-7900372x150.png"  xlink:type="simple"/></disp-formula><p>Using (12), we have:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x151.png" xlink:type="simple"/></inline-formula>,</p><p>which is equivalent to:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x152.png" xlink:type="simple"/></inline-formula>.</p><p>Thus the proof is complete.</p></sec><sec id="s6"><title>6. Conclusions</title><p>In this paper, we have some important results. First of all we proved the existence and uniqueness of the state for system (1), which is (2 &#180; 2) cooperative hyperbolic system involving Schr&#246;dinger operator defined on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/9-7900372x153.png" xlink:type="simple"/></inline-formula> (Theorem 3.1). Then we found the necessary and sufficient conditions of optimality for system (1), that give the characterization of optimal control (Theorem 4.1). Finally, we also find the necessary and sufficient conditions of optimal control when the observation is on the boundary (Theorem 5.1).</p><p>Also it is evident that by modifying:</p><p>-the nature of the control (distributed, boundary(,</p><p>-the nature of the observation (distributed, boundary(,</p><p>-the initial differential system,</p><p>-the type of equation (elliptic, parabolic and hyperbolic),</p><p>-the type of system (non-cooperative, cooperative),</p><p>-the order of equation,</p><p>many of variations on the above problem are possible to study with the help of Lions formalism.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.51567-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Serag, H.M. (2000) Distributed Control for Cooperative Systems Governed by Schr&amp;#246;dinger Operator. 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