<?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">JMF</journal-id><journal-title-group><journal-title>Journal of Mathematical Finance</journal-title></journal-title-group><issn pub-type="epub">2162-2434</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jmf.2015.54029</article-id><article-id pub-id-type="publisher-id">JMF-60999</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Business&amp;Economics</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  &lt;i&gt;H&lt;/i&gt;&lt;sub&gt;&amp;#8734&lt;/sub&gt; Optimal Control Problems for Jump
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>van</surname><given-names>G. Ivanov</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ivelin</surname><given-names>G. Ivanov</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Pedagogical College Dobrich, Shoumen University, Shoumen, Bulgaria</addr-line></aff><aff id="aff1"><addr-line>Faculty of Economics and Business Administration, Sofia University “St. Kliment Ohridski”, Sofia, Bulgaria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>i_ivanov@feb.uni-sofia.bg(VGI)</email>;<email>iwelin.ivanow@gmail.com(IGI)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>05</day><month>11</month><year>2015</year></pub-date><volume>05</volume><issue>04</issue><fpage>337</fpage><lpage>347</lpage><history><date date-type="received"><day>8</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>8</month>	<year>November</year>	</date><date date-type="accepted"><day>11</day>	<month>November</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   We consider a set of continuous algebraic Riccati equations with indefinite quadratic parts that arise in H￥ control problems. It is well known that the approach for solving such type of equations is proposed in the literature. Two matrix sequences are constructed. Three effective methods are described for computing the matrices of the second sequence, where each matrix is the stabilizing solution of the set of Riccati equations with definite quadratic parts. The acceleration modifications of the described methods are presented and applied. Computer realizations of the presented methods are numerically compared. In addition, a second iterative method is proposed. It constructs one matrix sequence which converges to the stabilizing solution to the given set of Riccati equations with indefinite quadratic parts. The convergence properties of the second method are commented. The iterative methods are numerically compared and investigated. 
 
</p></abstract><kwd-group><kwd>&lt;i&gt;H&lt;/i&gt;&lt;sub&gt;&amp;#8734&lt;/sub&gt; Optimal Control Problem</kwd><kwd> Generalized Riccati Equation</kwd><kwd> Indefinite Sign</kwd><kwd> Stabilizing Solution</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Recently the algebraic Riccati equations with indefinite quadratic part have been investigated intensively. The paper of Lanzon et al. [<xref ref-type="bibr" rid="scirp.60999-ref1">1</xref>] is the first where is investigated an algebraic Riccati equation with an indefinite quadratic part in the deterministic case. Further on, the Lanzon’s approach has been extended and applied to the algebraic Riccati equations of different types [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] -[<xref ref-type="bibr" rid="scirp.60999-ref5">5</xref>] and for the stochastic case [<xref ref-type="bibr" rid="scirp.60999-ref6">6</xref>] . Many situations in management, economics and finance [<xref ref-type="bibr" rid="scirp.60999-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.60999-ref9">9</xref>] are characterized by multiple decision makers/players who can enforce the decisions that have enduring consequences. The similar game models lead us to the solution of the Riccati equations with an indefinite quadratic part. The findings in [<xref ref-type="bibr" rid="scirp.60999-ref8">8</xref>] show how to model economic and financial applications using a discrete-time H<sub>&#165;</sub>-approach to simulate optimal solutions under a flexible choice of system parameters. Here, a continuous H<sub>&#165;</sub>-approach to jump linear equations is studied and investigated.</p><p>More precisely, how to find the stabilizing solution of the coupled algebraic Riccati equations of the optimal control problem for jump linear systems with indefinite quadratic part:</p><disp-formula id="scirp.60999-formula462"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x6.png"  xlink:type="simple"/></disp-formula><p>is considered. In the above equations the matrix coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x7.png" xlink:type="simple"/></inline-formula> are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x8.png" xlink:type="simple"/></inline-formula> real matrices, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x9.png" xlink:type="simple"/></inline-formula>are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x10.png" xlink:type="simple"/></inline-formula> real matrices, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x11.png" xlink:type="simple"/></inline-formula>is a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x12.png" xlink:type="simple"/></inline-formula> real matrix and the unknown <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x13.png" xlink:type="simple"/></inline-formula> is a symmetric <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x14.png" xlink:type="simple"/></inline-formula> matrix<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x15.png" xlink:type="simple"/></inline-formula>. The considered set of Riccati Equation (1) is connected to the stochastic controlled system with the continuous Markov process (see [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] ), which is called a <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x16.png" xlink:type="simple"/></inline-formula> control problem. The parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x17.png" xlink:type="simple"/></inline-formula> presents a level of attenuation of the corresponding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x18.png" xlink:type="simple"/></inline-formula> control problem. In order to solve a given <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x19.png" xlink:type="simple"/></inline-formula> control problem, we have to find the control <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x20.png" xlink:type="simple"/></inline-formula> which is given by</p><disp-formula id="scirp.60999-formula463"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x21.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x22.png" xlink:type="simple"/></inline-formula> is a right continuous Markov process and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x23.png" xlink:type="simple"/></inline-formula> is the stabilizing solution to (1) (see [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] ).</p><p>The stabilizing solution of the considered game theoretic Riccati equation is obtained as a limit of a sequence of approximations constructed based on stabilizing solutions of a sequence of algebraic Riccati equations of stochastic control with definite sign of the quadratic part. The main idea is to construct two matrix sequences such that the sum of corresponding matrices converges to the stabilizing solution of the set of Riccati Equation (1). Such approach is considered in [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] . The properties of this approach are considered in terms of the concept of mean square stabilizability and the assumption that the convex set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x24.png" xlink:type="simple"/></inline-formula> is not empty (see Dragan and coauthors in [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] ).</p><p>Here we introduce the sufficient conditions for the existence of stabilizing solutions of the set of Riccati Equation (1). We will prove under these conditions some convergence properties of constructed matrix sequences in terms of perturbed Lyapunov matrix equations. In addition, we introduce a second iterative method where we construct one matrix sequence. We show that the second iterative method constructs a convergent matrix sequence. Moreover, if the sufficient conditions of the first approach are satisfied then the second iterative method converges.</p></sec><sec id="s2"><title>2. Preliminary Facts</title><p>The notation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x25.png" xlink:type="simple"/></inline-formula> stands for the linear space of symmetric matrices of size n over the field of real numbers. For any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x26.png" xlink:type="simple"/></inline-formula>, we write <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x27.png" xlink:type="simple"/></inline-formula> or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x28.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x29.png" xlink:type="simple"/></inline-formula> is positive definite or <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x30.png" xlink:type="simple"/></inline-formula> is positive semidefinite.</p><p>We use notation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula>. The notations <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula> and the inequality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula> mean that for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x34.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x35.png" xlink:type="simple"/></inline-formula>, respectively. The linear space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x36.png" xlink:type="simple"/></inline-formula> is a Hilbert space with the Frobenius inner product<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x37.png" xlink:type="simple"/></inline-formula>. A linear operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x38.png" xlink:type="simple"/></inline-formula> on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x39.png" xlink:type="simple"/></inline-formula> is called asymptotically stable if the</p><p>eigenvalues to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x40.png" xlink:type="simple"/></inline-formula> lie in the open left half plane and almost asymptotically stable if the eigenvalues to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x41.png" xlink:type="simple"/></inline-formula> lie in the closed left half plane.</p><p>We denote <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x42.png" xlink:type="simple"/></inline-formula> and define the matrix function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x43.png" xlink:type="simple"/></inline-formula> as follows:</p><disp-formula id="scirp.60999-formula464"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x44.png"  xlink:type="simple"/></disp-formula><p>We will rewrite the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x45.png" xlink:type="simple"/></inline-formula> in the form:</p><disp-formula id="scirp.60999-formula465"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x46.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x47.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x48.png" xlink:type="simple"/></inline-formula></p><p>Note that transition coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x49.png" xlink:type="simple"/></inline-formula> if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x50.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x51.png" xlink:type="simple"/></inline-formula> for all i. Thus if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x52.png" xlink:type="simple"/></inline-formula>, we have<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x53.png" xlink:type="simple"/></inline-formula>.</p><p>We introduce the following perturbed Lyapunov operator</p><disp-formula id="scirp.60999-formula466"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x54.png"  xlink:type="simple"/></disp-formula><p>and will present the solvability of (1) through properties if the perturbed Lyapunov operator.</p><p>Proposition 1: [<xref ref-type="bibr" rid="scirp.60999-ref10">10</xref>] The following are equivalent:</p><p>1) The matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x55.png" xlink:type="simple"/></inline-formula> is the stabilizing solution to (1);</p><p>2) The perturbed Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x56.png" xlink:type="simple"/></inline-formula> is asymptotically stable where:</p><disp-formula id="scirp.60999-formula467"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x57.png"  xlink:type="simple"/></disp-formula><p>The above proposition presents a deterministic characterization of a stabilizing solution to set of Riccati Equation (1).</p><p>A matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x58.png" xlink:type="simple"/></inline-formula> is called stabilizing for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x59.png" xlink:type="simple"/></inline-formula> if eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x60.png" xlink:type="simple"/></inline-formula> lie in the open left half plane. In order words the stabilizing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x61.png" xlink:type="simple"/></inline-formula> to (1) stabilizes the operators<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x62.png" xlink:type="simple"/></inline-formula>.</p><p>Knowing the stabilizing solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x63.png" xlink:type="simple"/></inline-formula> to (1) we consider <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x64.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x65.png" xlink:type="simple"/></inline-formula> and therefore the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x66.png" xlink:type="simple"/></inline-formula> builds a perturbed Lyapunov operator which is asymptotically stable.</p><p>Dragan et al. [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] have introduced the following iteration scheme for finding the stabilizing solution to set of algebraic Riccati Equation (1). They construct two matrix sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x67.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x68.png" xlink:type="simple"/></inline-formula> as follows:</p><disp-formula id="scirp.60999-formula468"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x69.png"  xlink:type="simple"/></disp-formula><p>Each matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x70.png" xlink:type="simple"/></inline-formula> is computed as the stabilizing solution of the algebraic Riccati equation with definite quadratic part:</p><disp-formula id="scirp.60999-formula469"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x71.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.60999-formula470"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x72.png"  xlink:type="simple"/></disp-formula><p>However, it is not explained in [<xref ref-type="bibr" rid="scirp.60999-ref2">2</xref>] how Equation (5) has to be solved.</p><p>In our investigation we present a few iterative methods for finding the stabilizing solution to (5). Convergence</p><p>properties of the matrix sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x73.png" xlink:type="simple"/></inline-formula> will be derived. A second iterative method is derived. The</p><p>second aim of the paper is to provide a short numerically survey on iterative methods for computing the stabilizing solution to the given set of Riccati equations. Results from the numerical comparison are given on a family of numerical examples.</p><p>Lemma 1. For the map <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x74.png" xlink:type="simple"/></inline-formula> the following identities are valid:</p><p>i)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x75.png" xlink:type="simple"/></inline-formula> (6)</p><p>for any symmetric matrices<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x76.png" xlink:type="simple"/></inline-formula>.</p><p>ii)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x77.png" xlink:type="simple"/></inline-formula> (7)</p><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x78.png" xlink:type="simple"/></inline-formula></p><p>Proof. The statements of Lemma 1 are verified by direct manipulations. □</p><p>Lemma 2. Assume there exist positive definite symmetric matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x79.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x80.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x81.png" xlink:type="simple"/></inline-formula> is the stabilizing solution to</p><disp-formula id="scirp.60999-formula471"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x82.png"  xlink:type="simple"/></disp-formula><p>Then</p><p>i) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x83.png" xlink:type="simple"/></inline-formula> is asymptotically stable for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x84.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x85.png" xlink:type="simple"/></inline-formula> then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x86.png" xlink:type="simple"/></inline-formula>;</p><p>ii) if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x87.png" xlink:type="simple"/></inline-formula> then the Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x88.png" xlink:type="simple"/></inline-formula> is asymptotically stable for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x89.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. Assume the index i is fixed. We have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x90.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x91.png" xlink:type="simple"/></inline-formula>. Applying some matrix manipulations we obtain the equation:</p><disp-formula id="scirp.60999-formula472"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x92.png"  xlink:type="simple"/></disp-formula><p>Thus<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x93.png" xlink:type="simple"/></inline-formula>. The statement 1) is proved.</p><p>In order to prove the statement 2) we derive:</p><disp-formula id="scirp.60999-formula473"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x94.png"  xlink:type="simple"/></disp-formula><p>Since the matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x95.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x96.png" xlink:type="simple"/></inline-formula> are positive definite then the Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x97.png" xlink:type="simple"/></inline-formula> is asymptotically stable for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x98.png" xlink:type="simple"/></inline-formula> because Riccati Equation (8) has the stabilizing positive semidefinte solution.</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x99.png" xlink:type="simple"/></inline-formula>.</p><p>The lemma is proved.</p></sec><sec id="s3"><title>3. Iterative Methods</title><p>In this section we are proving the some convergence properties of the matrix sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x100.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x101.png" xlink:type="simple"/></inline-formula> defined by iterative loop (4)-(5). We present the main theorem where the convergence properties for matrix sequences are derived.</p><p>Theorem 1. Assume there exist symmetric matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x103.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x104.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x105.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x106.png" xlink:type="simple"/></inline-formula>, and the Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x107.png" xlink:type="simple"/></inline-formula> is asymptotically stable. Then for the matrix sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x108.png" xlink:type="simple"/></inline-formula> defined as the stabilizing solution of (5) satisfy</p><p>i) The Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x109.png" xlink:type="simple"/></inline-formula> is asymptotically stable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x110.png" xlink:type="simple"/></inline-formula>;</p><p>ii)<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x111.png" xlink:type="simple"/></inline-formula>;</p><p>iii) The Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x112.png" xlink:type="simple"/></inline-formula> is asymptotically stable where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x113.png" xlink:type="simple"/></inline-formula>;</p><p>iv) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x114.png" xlink:type="simple"/></inline-formula>for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x115.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. The algorithm begins with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x116.png" xlink:type="simple"/></inline-formula>. Then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x117.png" xlink:type="simple"/></inline-formula>. The matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x117.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x118.png" xlink:type="simple"/></inline-formula> is a solution of the Riccati equation:</p><disp-formula id="scirp.60999-formula474"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x119.png"  xlink:type="simple"/></disp-formula><p>Under the assumption the Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x120.png" xlink:type="simple"/></inline-formula> is asymptotically stable <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x121.png" xlink:type="simple"/></inline-formula>. Thus, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x122.png" xlink:type="simple"/></inline-formula>is the unique stabilizing solution of the above Riccati equation and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x123.png" xlink:type="simple"/></inline-formula>.</p><p>Using Lemma 1 1) and the fact that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x124.png" xlink:type="simple"/></inline-formula> is a solution to (9) we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x124.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x125.png" xlink:type="simple"/></inline-formula>. In addition, the operator</p><disp-formula id="scirp.60999-formula475"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x126.png"  xlink:type="simple"/></disp-formula><p>is asymptotically stable and</p><disp-formula id="scirp.60999-formula476"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x127.png"  xlink:type="simple"/></disp-formula><p>The Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x128.png" xlink:type="simple"/></inline-formula> is asymptotically stable. In addition, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x129.png" xlink:type="simple"/></inline-formula>is a solution to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x130.png" xlink:type="simple"/></inline-formula> and applying Lemma 1 we obtain:</p><disp-formula id="scirp.60999-formula477"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x131.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x132.png" xlink:type="simple"/></inline-formula> is the stabilizing solution to the latest equation, then the Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x133.png" xlink:type="simple"/></inline-formula> is asymptotically stable with</p><disp-formula id="scirp.60999-formula478"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x134.png"  xlink:type="simple"/></disp-formula><p>Thus, following Lemma 2, 1) we conclude that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x135.png" xlink:type="simple"/></inline-formula>.</p><p>Thus, the properties 1), 2), 3) and 4) are true for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x136.png" xlink:type="simple"/></inline-formula>. We compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x137.png" xlink:type="simple"/></inline-formula>.</p><p>Combining iteration (5) with equality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x138.png" xlink:type="simple"/></inline-formula> we construct the following matrix sequences:</p><disp-formula id="scirp.60999-formula479"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x139.png"  xlink:type="simple"/></disp-formula><p>we prove by induction the following for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x140.png" xlink:type="simple"/></inline-formula>:</p><p>(a<sub>k</sub>): The Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x141.png" xlink:type="simple"/></inline-formula> is asymptotically stable,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x142.png" xlink:type="simple"/></inline-formula>;</p><p>(b<sub>k</sub>):<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x143.png" xlink:type="simple"/></inline-formula>;</p><p>(g<sub>k</sub>): The Lyapunov operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x144.png" xlink:type="simple"/></inline-formula> is asymptotically stable where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x145.png" xlink:type="simple"/></inline-formula>;</p><p>(d<sub>k</sub>):<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x146.png" xlink:type="simple"/></inline-formula>.</p><p>We have seen the statements (a<sub>0</sub>), (b<sub>0</sub>), (g<sub>0</sub>) and (d<sub>0</sub>)) are true. We assume the statements (a<sub>k</sub>), (b<sub>k</sub>), (g<sub>k</sub>) and (d<sub>k</sub>) are true for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x147.png" xlink:type="simple"/></inline-formula>. We prove the same statements for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x147.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x148.png" xlink:type="simple"/></inline-formula>.</p><p>We know<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula>. We compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula>. We have to find <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x152.png" xlink:type="simple"/></inline-formula> as a unique stabilizing solution to (5) with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x153.png" xlink:type="simple"/></inline-formula>. The matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x154.png" xlink:type="simple"/></inline-formula> is positive semidefinite because <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x155.png" xlink:type="simple"/></inline-formula> is true. It remains to show that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x156.png" xlink:type="simple"/></inline-formula> is asymptotically stable<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x157.png" xlink:type="simple"/></inline-formula>.</p><p>Following Lemma 2, 2) the operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula> is asymptotically stable because <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula>. Thus the operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula> is asymptotically stable. In addition, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula>. Thus the operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x163.png" xlink:type="simple"/></inline-formula> is asymptotically stable,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x164.png" xlink:type="simple"/></inline-formula>. There exists a unique positive semidefinite solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x165.png" xlink:type="simple"/></inline-formula> to (5) with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x166.png" xlink:type="simple"/></inline-formula>. The last fact in combination of the presentation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x167.png" xlink:type="simple"/></inline-formula> from Lemma 1, 1) we conclude that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x161.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x166.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x167.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x168.png" xlink:type="simple"/></inline-formula> and moreover is positive semidefnite. The assertions (a<sub>r</sub>) and (b<sub>r</sub>) are proved.</p><p>We have to prove the operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x169.png" xlink:type="simple"/></inline-formula> is asymptotically stable and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x170.png" xlink:type="simple"/></inline-formula>. In addition, the operator <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x171.png" xlink:type="simple"/></inline-formula> is asymptotically stable because (a<sub>r</sub>). Moreover, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x172.png" xlink:type="simple"/></inline-formula> Thus the (g<sub>r</sub>) is true for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x169.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x170.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x171.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x173.png" xlink:type="simple"/></inline-formula>.</p><p>Further on, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x174.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x175.png" xlink:type="simple"/></inline-formula> and thus</p><disp-formula id="scirp.60999-formula480"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x176.png"  xlink:type="simple"/></disp-formula><p>is asymptotically stable by Lemma 2, 2) Using again Lemma 2, 1) we conclude<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x177.png" xlink:type="simple"/></inline-formula>. Hence<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x178.png" xlink:type="simple"/></inline-formula>. All statements are proved for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x179.png" xlink:type="simple"/></inline-formula>.</p><p>The theorem is proved. □</p><p>The problem is to find the stabilizing solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x180.png" xlink:type="simple"/></inline-formula> to the general equation</p><disp-formula id="scirp.60999-formula481"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x181.png"  xlink:type="simple"/></disp-formula><p>The Riccati Iterative Method. We choose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x182.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x183.png" xlink:type="simple"/></inline-formula> is the stabilizing solution to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x183.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x184.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.60999-formula482"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x185.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x186.png" xlink:type="simple"/></inline-formula> Note that the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x187.png" xlink:type="simple"/></inline-formula> is a positive semidefinite matrix for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x186.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x187.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x188.png" xlink:type="simple"/></inline-formula>.</p><p>It is well know that if the matrix pair <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x189.png" xlink:type="simple"/></inline-formula> is stabilizable and the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x190.png" xlink:type="simple"/></inline-formula> is positive semidefinite, then there exists a semidefinite solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x189.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x191.png" xlink:type="simple"/></inline-formula> to the “perturbed” Riccati Equation (10).</p><p>Based on Riccati iteration (11) we consider the improved modification given by:</p><disp-formula id="scirp.60999-formula483"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x192.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.60999-formula484"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x193.png"  xlink:type="simple"/></disp-formula><p>The Lyapunov Iterative Method. We choose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x194.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x194.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x195.png" xlink:type="simple"/></inline-formula> is the stabilizing solution to</p><disp-formula id="scirp.60999-formula485"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x196.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x197.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.60999-formula486"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x198.png"  xlink:type="simple"/></disp-formula><p>We consider the Lyapunov iteration (13) as a special case of the Lyapunov iteration introduced and investigated by Ivanov [<xref ref-type="bibr" rid="scirp.60999-ref11">11</xref>] . Following the numerical experience in [<xref ref-type="bibr" rid="scirp.60999-ref11">11</xref>] we improve iteration (13) and introduce the improved Lyapunov iteration</p><disp-formula id="scirp.60999-formula487"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x199.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.60999-formula488"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x200.png"  xlink:type="simple"/></disp-formula><p>Convergence properties of the matrix sequence defined by (14) are given with Theorem 2.1 [<xref ref-type="bibr" rid="scirp.60999-ref11">11</xref>] .</p><p>Further on, we consider an alternative iteration process where one matrix sequence is constructed. This sequence converges to the stabilizing solution of the given set of Riccati equations. We are proving that this in-</p><p>troduced iteration is equivalent to the iteration loop (4)-(5). We substitute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x201.png" xlink:type="simple"/></inline-formula> from (3) in recurrence Equation (5) and after matrix manipulations we obtain for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x201.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x202.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.60999-formula489"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x203.png"  xlink:type="simple"/></disp-formula><p>Thus, we can construct the matrix sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x204.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x205.png" xlink:type="simple"/></inline-formula> and each subsequent matrix is computed as a unique stabilizing solution to (15). In fact we just proved that the matrix sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x206.png" xlink:type="simple"/></inline-formula> defined by (15) is equivalent to the matrix sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x207.png" xlink:type="simple"/></inline-formula> defined by (4)-(5). In order to apply the iteration (15) we change the term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x208.png" xlink:type="simple"/></inline-formula> from (15) with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x204.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x205.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x206.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x207.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x208.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x209.png" xlink:type="simple"/></inline-formula>.</p><p>The unknown matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x210.png" xlink:type="simple"/></inline-formula> is a solution to the set of continuous-time algebraic Riccati equation with the independent matrix</p><disp-formula id="scirp.60999-formula490"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x211.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Numerical Simulations</title><p>We have considered two iterative methods for computing the matrix sequence<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x212.png" xlink:type="simple"/></inline-formula>: the Riccati iteration</p><p>(15) and the Lyapunov iteration (14). In the begining we remark the LMI approach for finding the stabilizing solution to (5). Following similar investigations [<xref ref-type="bibr" rid="scirp.60999-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.60999-ref13">13</xref>] we conclude that the optimization problem (for given k)</p><disp-formula id="scirp.60999-formula491"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-1490354x213.png"  xlink:type="simple"/></disp-formula><p>has a solution which is the stabilizing solution to (5).</p><p>We carry out experiments for solving a set of Riccati Equation (1). We construct two matrix sequences <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x214.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x215.png" xlink:type="simple"/></inline-formula> for each example. The first matrix sequence is computed using iterative method (4)-(5). In order to form the second matrix sequence we apply Riccati iteration (15), Lyapunov iteration (14) and LMI approach (16). In addition, we construct a matrix sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x214.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x215.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x216.png" xlink:type="simple"/></inline-formula> for each example using recurrence Equation (15) for this purpose.</p><p>The matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x217.png" xlink:type="simple"/></inline-formula> are computed in terms of the solutions of N Riccati equations for (15) and N</p><p>algebraic Lyapunov equations for (14) at each step. For this purpose the MATLAB procedure care is applied where the flops are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x218.png" xlink:type="simple"/></inline-formula> per one iteration. Lyapunov iteration (14) solves N algebraic Riccati equations at each step. The MATLAB procedure lyap is used and the flops are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x218.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x219.png" xlink:type="simple"/></inline-formula> per one iteration. In order to find the symmetric solution to (16) we adapt MATLAB’s software functions of LMI Lab.</p><p>Our experiments are executed in MATLAB on a 2.20 GHz Intel(R) Core(TM) i7-4702MQ CPU computer. We use two variables tolR and tol for small positive numbers to control the accuracy of computations. We de-</p><p>note <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x220.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x221.png" xlink:type="simple"/></inline-formula>. The iterations (15) and (14) stop when the inequality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x222.png" xlink:type="simple"/></inline-formula> is satisfied for some<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x223.png" xlink:type="simple"/></inline-formula>. That is a practical stopping criterion for (15) and (14). The variable It means the maximal number of iterations for which the inequality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x220.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x221.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x222.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x223.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x224.png" xlink:type="simple"/></inline-formula> holds. The last inequality is used as a practical stopping criterion for main iterative process (4)-(5). The tolerance tol controls accuracy of the procedure mincx which is used for numerical solution to (16).</p><p>We consider a family of examples in case <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x225.png" xlink:type="simple"/></inline-formula> for two given values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x226.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x226.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x227.png" xlink:type="simple"/></inline-formula>. The coefficient real matrices are given as follows: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x226.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x228.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x225.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x226.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x227.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x228.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x229.png" xlink:type="simple"/></inline-formula> were constructed using the MATLAB notations:</p><disp-formula id="scirp.60999-formula492"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x230.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.60999-formula493"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x231.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60999-formula494"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x232.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.60999-formula495"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x233.png"  xlink:type="simple"/></disp-formula><p>In our definitions the functions randn (p, k) and sprand (q, m, 0.3) return a p-by-k matrix of pseudorandom scalar values and a q-by-m sparse matrix respectively (for more information see the MATLAB description). The following transition probability matrix</p><disp-formula id="scirp.60999-formula496"><graphic  xlink:href="http://html.scirp.org/file/3-1490354x234.png"  xlink:type="simple"/></disp-formula><p>is applied for all examples.</p><p>For our purpose we have executed hundred examples of each value of m for all tests. <xref ref-type="table" rid="table1">Table 1</xref> reports the average number of iterations for the main iterative process “It<sub>M</sub>” and the average number of iterations for the second iterative process “It<sub>S</sub>” needed for achieving the relative accuracy for all examples of each size. The column “CPU” presents the CPU time for executing the corresponding iterations. Results from experiments are given in <xref ref-type="table" rid="table1">Table 1</xref> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x235.png" xlink:type="simple"/></inline-formula> for all tests. Results from experiments with the iteration (15) are given in <xref ref-type="table" rid="table2">Table 2</xref> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x235.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-1490354x236.png" xlink:type="simple"/></inline-formula> for all tests.</p></sec><sec id="s5"><title>5. Conclusions</title><p>We have studied two iterative processes for finding the stabilizing solution to a set of continuous-time genera-</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Results from 50 runs for each value of n</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >n</th><th align="center" valign="middle"  colspan="3"  >(4)-(5) with RI: (15)</th><th align="center" valign="middle"  colspan="3"  >(4)-(5) with LI: (14)</th><th align="center" valign="middle"  colspan="3"  >(4)-(5) with LMI: (16)</th></tr></thead><tr><td align="center" valign="middle" >It<sub>M</sub></td><td align="center" valign="middle" >It<sub>S</sub></td><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >It<sub>M</sub></td><td align="center" valign="middle" >It<sub>S</sub></td><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >It<sub>M</sub></td><td align="center" valign="middle" >It<sub>S</sub></td><td align="center" valign="middle" >CPU</td></tr><tr><td align="center" valign="middle"  colspan="10"  >Test 1: m<sub>1</sub> = 4</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >12.2</td><td align="center" valign="middle" >3.9 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >12.6</td><td align="center" valign="middle" >1.6 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >19.8</td><td align="center" valign="middle" >16.7 s</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >14.7</td><td align="center" valign="middle" >4.6 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >13.7</td><td align="center" valign="middle" >1.6 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >20.3</td><td align="center" valign="middle" >23.5 s</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >16.5</td><td align="center" valign="middle" >5.6 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >16.4</td><td align="center" valign="middle" >2.3 s</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >21.9</td><td align="center" valign="middle" >35.7 s</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >17.4</td><td align="center" valign="middle" >6.5 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >18.9</td><td align="center" valign="middle" >2.8 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >23.4</td><td align="center" valign="middle" >54.8 s</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >22.7</td><td align="center" valign="middle" >9.8 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >20.5</td><td align="center" valign="middle" >3.3 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >26.3</td><td align="center" valign="middle" >84.2 s</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >27.3</td><td align="center" valign="middle" >13.3 s</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >26.8</td><td align="center" valign="middle" >4.6 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >31.6</td><td align="center" valign="middle" >130.5 s</td></tr><tr><td align="center" valign="middle"  colspan="10"  >Test 2: m<sub>1</sub> = n</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >12.7</td><td align="center" valign="middle" >4.0 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >12.5</td><td align="center" valign="middle" >1.3 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >20.7</td><td align="center" valign="middle" >20.8 s</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >13.2</td><td align="center" valign="middle" >4.4 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >14.9</td><td align="center" valign="middle" >1.8 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >22.0</td><td align="center" valign="middle" >28.0 s</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >15.6</td><td align="center" valign="middle" >6.2 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >16.2</td><td align="center" valign="middle" >2.1 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >22.3</td><td align="center" valign="middle" >39.8 s</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >17.7</td><td align="center" valign="middle" >7.8 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >18.4</td><td align="center" valign="middle" >2.5 s</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >26.2</td><td align="center" valign="middle" >66.0 s</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >20.5</td><td align="center" valign="middle" >9.7 s</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >21.0</td><td align="center" valign="middle" >3.0 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >37.2</td><td align="center" valign="middle" >125.3 s</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >23.3</td><td align="center" valign="middle" >11.5 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >22.8</td><td align="center" valign="middle" >3.3 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >36.9</td><td align="center" valign="middle" >163.2 s</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >25.1</td><td align="center" valign="middle" >11.6 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >25.6</td><td align="center" valign="middle" >4.0 s</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >57.0</td><td align="center" valign="middle" >371.0 s</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >28.6</td><td align="center" valign="middle" >15.3 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >27.3</td><td align="center" valign="middle" >4.7 s</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >73.8</td><td align="center" valign="middle" >636.5 s</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Results from 50 runs for each value of n</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >the max number of iteration steps</th><th align="center" valign="middle" >the average number of iteration steps</th><th align="center" valign="middle" >CPU time</th></tr></thead><tr><td align="center" valign="middle"  colspan="4"  >Iteration (15) for m<sub>1</sub> = 4</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >17.0</td><td align="center" valign="middle" >1.8 s</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >38</td><td align="center" valign="middle" >18.6</td><td align="center" valign="middle" >2.1 s</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >28</td><td align="center" valign="middle" >19.7</td><td align="center" valign="middle" >2.5 s</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >58</td><td align="center" valign="middle" >23.2</td><td align="center" valign="middle" >3.1 s</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >56</td><td align="center" valign="middle" >27.5</td><td align="center" valign="middle" >4.2 s</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >61</td><td align="center" valign="middle" >31.6</td><td align="center" valign="middle" >5.2 s</td></tr><tr><td align="center" valign="middle"  colspan="4"  >Iteration (15) for m<sub>1</sub> = n</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >16.1</td><td align="center" valign="middle" >1.8 s</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >27</td><td align="center" valign="middle" >17.7</td><td align="center" valign="middle" >2.1 s</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >30</td><td align="center" valign="middle" >18.8</td><td align="center" valign="middle" >2.6 s</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >29</td><td align="center" valign="middle" >20.9</td><td align="center" valign="middle" >3.3 s</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >24.3</td><td align="center" valign="middle" >4.0 s</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >51</td><td align="center" valign="middle" >25.5</td><td align="center" valign="middle" >4.3 s</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >40</td><td align="center" valign="middle" >27.9</td><td align="center" valign="middle" >4.5 s</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >46</td><td align="center" valign="middle" >31.6</td><td align="center" valign="middle" >5.2 s</td></tr></tbody></table></table-wrap><p>lized Riccati Equation (1). We have made numerical experiments for computing this solution and we have compared the numerical results. In fact, it is a numerical survey on iterative methods for computing the stabilizing solution. We have compared the results from the experiments in regard of the number of iterations and CPU time for executing. Our numerical experiments confirm the effectiveness of proposed new method (15).</p><p>The application of all iterative methods shows that they achieve the same accuracy for different number of iterations. The executed examples have demonstrated that the two iterations “(4)-(5) with RI: (15)” and “(4)-(5) with LI: (14)” require very close average numbers of iterations (see the columns “It<sub>S</sub>” for all tests). However, the CPU time is different for these iterations. In addition, by comparing iterations based on the solution, the linear matrix Lyapunov equations shows that iteration “(4)-(5) with LI: (14)” is slightly faster than the second iteration (15). This conclusion is indicated by numerical simulations. Based on the experiments, the main conclusion is that the Lyapunov iteration is faster than the Riccati iteration because these methods carry out the same number of iterations.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The present research paper was supported in a part by the EEA Scholarship Programme BG09 Project Grant D03-91 under the European Economic Area Financial Mechanism. This support is greatly appreciated.</p></sec><sec id="s7"><title>Cite this paper</title><p>IvanG. Ivanov,Ivelin G.Ivanov, (2015) H<sub>&amp;#8734</sub> Optimal Control Problems for Jump. Journal of Mathematical Finance,05,337-347. doi: 10.4236/jmf.2015.54029</p></sec></body><back><ref-list><title>References</title><ref id="scirp.60999-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Lanzon, A., Feng, Y., Anderson, B. and Rotkowitz, M. 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