<?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">OJOp</journal-id><journal-title-group><journal-title>Open Journal of Optimization</journal-title></journal-title-group><issn pub-type="epub">2325-7105</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojop.2016.51006</article-id><article-id pub-id-type="publisher-id">OJOp-64516</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Regularized Newton Method with Correction for Unconstrained Convex Optimization
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>iming</surname><given-names>Li</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mei</surname><given-names>Qin</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>Heng</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Science, University of Shanghai for Science and Technology, Shanghai, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>usstjssx@126.com(MQ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>03</day><month>03</month><year>2016</year></pub-date><volume>05</volume><issue>01</issue><fpage>44</fpage><lpage>52</lpage><history><date date-type="received"><day>17</day>	<month>January</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>12</month>	<year>March</year>	</date><date date-type="accepted"><day>15</day>	<month>March</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, we present a regularized Newton method (M-RNM) with correction for minimizing a convex function whose Hessian matrices may be singular. At every iteration, not only a RNM step is computed but also two correction steps are computed. We show that if the objective function is 
  LC
  <sup>2</sup>, then the method posses globally convergent. Numerical results show that the new algorithm performs very well.
 
</p></abstract><kwd-group><kwd>Regularied Newton Method</kwd><kwd> Correction Technique</kwd><kwd> Trust Region Technique</kwd><kwd> Unconstrained Convex Optimization</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We consider the unconstrained optimization problem [<xref ref-type="bibr" rid="scirp.64516-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.64516-ref3">3</xref>]</p><disp-formula id="scirp.64516-formula599"><label>(1.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x7.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x8.png" xlink:type="simple"/></inline-formula> is twice continuously differentiable, whose gradient <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x9.png" xlink:type="simple"/></inline-formula> and Hessian <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x10.png" xlink:type="simple"/></inline-formula> are denoted by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x11.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x12.png" xlink:type="simple"/></inline-formula> respectively. Throughout this paper, we assume that the solution set of (1.1) is nonempty and denoted by X, and in all cases <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x13.png" xlink:type="simple"/></inline-formula> refers to the 2-norm.</p><p>It is well known that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x14.png" xlink:type="simple"/></inline-formula> is convex if and only if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x15.png" xlink:type="simple"/></inline-formula> is symmetric positive semidefinite for all<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x16.png" xlink:type="simple"/></inline-formula>. Moreover, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x17.png" xlink:type="simple"/></inline-formula> is convex, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x18.png" xlink:type="simple"/></inline-formula> if and only if x is a solution of the system of nonlinear equations</p><disp-formula id="scirp.64516-formula600"><label>(1.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x19.png"  xlink:type="simple"/></disp-formula><p>Hence, we could get the minimizer of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x20.png" xlink:type="simple"/></inline-formula> by solving (1.2) [<xref ref-type="bibr" rid="scirp.64516-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.64516-ref8">8</xref>] . The Newton method is one of efficient solution methods. At every iteration, it computes the trial step</p><disp-formula id="scirp.64516-formula601"><label>(1.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x21.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x23.png" xlink:type="simple"/></inline-formula>. As we know, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x24.png" xlink:type="simple"/></inline-formula> is Lipschitz continuous and nonsingular at the solution, then the Newton method has quadratic convergence. However, this method has an obvious disadvantage when the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x25.png" xlink:type="simple"/></inline-formula> is singular or near singular. In this case, we may compute the Moore-Penrose step [<xref ref-type="bibr" rid="scirp.64516-ref7">7</xref>] <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x26.png" xlink:type="simple"/></inline-formula>. But the computation of the singular value decomposition to obtain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x27.png" xlink:type="simple"/></inline-formula> is sometimes prohibitive. Hence, computing a direction that is close to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x28.png" xlink:type="simple"/></inline-formula> may be a good idea.</p><p>To overcome the difficulty caused by the possible singularity of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x29.png" xlink:type="simple"/></inline-formula>, [<xref ref-type="bibr" rid="scirp.64516-ref9">9</xref>] proposed a regularized Newton method, where the trial step is the solution of the linear equations</p><disp-formula id="scirp.64516-formula602"><label>(1.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x30.png"  xlink:type="simple"/></disp-formula><p>where I is the identity matrix. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x31.png" xlink:type="simple"/></inline-formula>is a positive parameter which is updated from iteration to iteration.</p><p>Now we need to consider another question, “how to choose the regularized parameter<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x32.png" xlink:type="simple"/></inline-formula>?” Yamashita and</p><p>Fukushima [<xref ref-type="bibr" rid="scirp.64516-ref10">10</xref>] chose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x33.png" xlink:type="simple"/></inline-formula> and showed that the regularized Newton method has quadratic convergence under the local error bound condition which is weaker than nonsingularity. Fan and Yuan [<xref ref-type="bibr" rid="scirp.64516-ref11">11</xref>] took <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x34.png" xlink:type="simple"/></inline-formula></p><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x35.png" xlink:type="simple"/></inline-formula> and showed that the Levenberg-Marqulardt method preserves the quadratic convergence. Numerial results ([<xref ref-type="bibr" rid="scirp.64516-ref12">12</xref>] [<xref ref-type="bibr" rid="scirp.64516-ref13">13</xref>] ) show that the choice of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x36.png" xlink:type="simple"/></inline-formula> performs more stable and preferable.</p><p>Inspired by the regularized Newton method [<xref ref-type="bibr" rid="scirp.64516-ref13">13</xref>] with correction for nonlinear equations, we propose a modified regularized Newton method in this paper. At every iteration, the modified regularized Newton method first solves the linear equations</p><disp-formula id="scirp.64516-formula603"><label>(1.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x37.png"  xlink:type="simple"/></disp-formula><p>to obtain the Newton step<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x38.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x39.png" xlink:type="simple"/></inline-formula> is updated from iteration to iteration, and solves the linear equations</p><disp-formula id="scirp.64516-formula604"><label>(1.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x40.png"  xlink:type="simple"/></disp-formula><p>to obtain the approximate Newton step<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x41.png" xlink:type="simple"/></inline-formula>.</p><p>It is easy to see</p><disp-formula id="scirp.64516-formula605"><label>(1.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x42.png"  xlink:type="simple"/></disp-formula><p>Then it solves the linear equations</p><disp-formula id="scirp.64516-formula606"><label>(1.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x43.png"  xlink:type="simple"/></disp-formula><p>to obtain the approximate Newton step<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x44.png" xlink:type="simple"/></inline-formula>.</p><p>The aim of this paper is to study the convergence properties of the above modified regularized Newton method and do a numerical experiment to test its efficiency.</p><p>The paper is organized as follows. In Section 2, we present a new regularized Newton algorithm with correction by trust region technique, and then prove the global convergence of the new algorithm under some suitable conditions. In Section 3, we test the regularized Newton algorithm with correction and compared it with a regularized Newton method. Finally, we conclude the paper in Section 4.</p></sec><sec id="s2"><title>2. The Algorithm and Its Global Convergence</title><p>In this section, we first present the new modified regularized Newton algorithm by using trust region technique, then prove the global convergence. First, we give the modified regularized Newton algorithm.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x46.png" xlink:type="simple"/></inline-formula> be given by (1.6) and (1.8), respectively. Since the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x47.png" xlink:type="simple"/></inline-formula> is symmetric and positive definite, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x48.png" xlink:type="simple"/></inline-formula>is a descent direction of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x49.png" xlink:type="simple"/></inline-formula> at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x50.png" xlink:type="simple"/></inline-formula>, however <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x51.png" xlink:type="simple"/></inline-formula> may not be. Hence we prefer to use a trust region technique.</p><p>Define the actual reduction of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x52.png" xlink:type="simple"/></inline-formula> at the kth iteration as</p><disp-formula id="scirp.64516-formula607"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x53.png"  xlink:type="simple"/></disp-formula><p>Note that the regularization step <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x54.png" xlink:type="simple"/></inline-formula> is the minimizer of the convex minimization problem</p><disp-formula id="scirp.64516-formula608"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x55.png"  xlink:type="simple"/></disp-formula><p>If we let</p><disp-formula id="scirp.64516-formula609"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x56.png"  xlink:type="simple"/></disp-formula><p>then it can be proved [<xref ref-type="bibr" rid="scirp.64516-ref4">4</xref>] that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x57.png" xlink:type="simple"/></inline-formula> is also a solution of the trust region problem</p><disp-formula id="scirp.64516-formula610"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x58.png"  xlink:type="simple"/></disp-formula><p>By the famous result given by Powell in [<xref ref-type="bibr" rid="scirp.64516-ref14">14</xref>] , we know that</p><disp-formula id="scirp.64516-formula611"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x59.png"  xlink:type="simple"/></disp-formula><p>By some simple calculations, we deduce from (1.7) that</p><disp-formula id="scirp.64516-formula612"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x60.png"  xlink:type="simple"/></disp-formula><p>so, we have</p><disp-formula id="scirp.64516-formula613"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x61.png"  xlink:type="simple"/></disp-formula><p>Similar to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x62.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x63.png" xlink:type="simple"/></inline-formula>is not only the minimizer of the problem</p><disp-formula id="scirp.64516-formula614"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x64.png"  xlink:type="simple"/></disp-formula><p>but also a solution to the trust region problem</p><disp-formula id="scirp.64516-formula615"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x65.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x66.png" xlink:type="simple"/></inline-formula>. Therefore we also have</p><disp-formula id="scirp.64516-formula616"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x67.png"  xlink:type="simple"/></disp-formula><p>Based on the inequalities (2.2), (2.3) and (2.4), it is reasonable for us to define the new predicted reduction as</p><disp-formula id="scirp.64516-formula617"><label>(2.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x68.png"  xlink:type="simple"/></disp-formula><p>which satisfies</p><disp-formula id="scirp.64516-formula618"><label>(2.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x69.png"  xlink:type="simple"/></disp-formula><p>The ratio of the actual reduction to the predicted reduction</p><disp-formula id="scirp.64516-formula619"><label>(2.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x70.png"  xlink:type="simple"/></disp-formula><p>plays a key role in deciding whether to accept the trial step and how to adjust the regularized parameter.</p><p>The regularized Newton algorithm with correction for unconstrained convex optimization problems is stated as follows.</p>Algorithm 2.1<p>Step 1. Given<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x71.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x72.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x73.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x74.png" xlink:type="simple"/></inline-formula>. Set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x75.png" xlink:type="simple"/></inline-formula>.</p><p>Step 2. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x76.png" xlink:type="simple"/></inline-formula>, then stop.</p><p>Step 3. Compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x77.png" xlink:type="simple"/></inline-formula>.</p><p>Solve</p><disp-formula id="scirp.64516-formula620"><label>(2.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x78.png"  xlink:type="simple"/></disp-formula><p>to obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x79.png" xlink:type="simple"/></inline-formula>.</p><p>Solve</p><disp-formula id="scirp.64516-formula621"><label>(2.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x80.png"  xlink:type="simple"/></disp-formula><p>to obtain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x81.png" xlink:type="simple"/></inline-formula> and set</p><disp-formula id="scirp.64516-formula622"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x82.png"  xlink:type="simple"/></disp-formula><p>Solve</p><disp-formula id="scirp.64516-formula623"><label>(2.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x83.png"  xlink:type="simple"/></disp-formula><p>to obtain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x84.png" xlink:type="simple"/></inline-formula> and set</p><disp-formula id="scirp.64516-formula624"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x85.png"  xlink:type="simple"/></disp-formula><p>Step 4. Compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x86.png" xlink:type="simple"/></inline-formula>. Set</p><disp-formula id="scirp.64516-formula625"><label>(2.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x87.png"  xlink:type="simple"/></disp-formula><p>Step 5. Choose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x88.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.64516-formula626"><label>(2.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x89.png"  xlink:type="simple"/></disp-formula><p>Set <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x90.png" xlink:type="simple"/></inline-formula> and go step 2.</p><p>Before discussing the global convergence of the algorithm above, we make the following assumption.</p><p>Assumption 2.1. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x91.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x92.png" xlink:type="simple"/></inline-formula> are both Lipschitz continuous, that is, there exists a constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x93.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x94.png" xlink:type="simple"/></inline-formula>such that</p><disp-formula id="scirp.64516-formula627"><label>(2.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x95.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.64516-formula628"><label>(2.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x96.png"  xlink:type="simple"/></disp-formula><p>It follows from (2.14) that</p><disp-formula id="scirp.64516-formula629"><label>(2.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x97.png"  xlink:type="simple"/></disp-formula><p>The following lemma given below shows the relationship between the positive semidefinite matrix and symmetric positive semidefinite matrix.</p><p>Lemma 2.1. A real-valued matrix A is positive semidefinite if and only if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x98.png" xlink:type="simple"/></inline-formula> is positive semidefinite.</p><p>Proof. See [<xref ref-type="bibr" rid="scirp.64516-ref4">4</xref>] . ♢</p><p>Next, we give the bounds of a positive definite matrix and its inverse.</p><p>Lemma 2.2. Suppose A is positive semidefinite. Then,</p><disp-formula id="scirp.64516-formula630"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x99.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.64516-formula631"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x100.png"  xlink:type="simple"/></disp-formula><p>hold for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x101.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. See [<xref ref-type="bibr" rid="scirp.64516-ref13">13</xref>] . ♢</p><p>Theorem 2.1. Under the conditions of Assumption 2.1, if f is bounded below, then Algorithm 2.1 terminates in finite iterations or satisfies</p><disp-formula id="scirp.64516-formula632"><label>(2.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x102.png"  xlink:type="simple"/></disp-formula><p>Proof. We prove by contradiction. If the theorem is not true, then there exists a positive <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x103.png" xlink:type="simple"/></inline-formula> and an integer <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x103.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x104.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.64516-formula633"><label>(2.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x105.png"  xlink:type="simple"/></disp-formula><p>Without loss of generality, we can suppose<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x106.png" xlink:type="simple"/></inline-formula>. Set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x107.png" xlink:type="simple"/></inline-formula>. Then</p><disp-formula id="scirp.64516-formula634"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x108.png"  xlink:type="simple"/></disp-formula><p>Now we will analysis in two cases whether T is finite or not.</p><p>Case (1): T is finite. Then there exists an integer <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x109.png" xlink:type="simple"/></inline-formula> such that</p><disp-formula id="scirp.64516-formula635"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x110.png"  xlink:type="simple"/></disp-formula><p>By (2.11), we have</p><disp-formula id="scirp.64516-formula636"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x111.png"  xlink:type="simple"/></disp-formula><p>Therefore by (2.12) and (2.17), we deduce</p><disp-formula id="scirp.64516-formula637"><label>(2.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x112.png"  xlink:type="simple"/></disp-formula><p>Since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x113.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x114.png" xlink:type="simple"/></inline-formula>, we get from (2.8) and (2.18) that</p><disp-formula id="scirp.64516-formula638"><label>(2.19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x115.png"  xlink:type="simple"/></disp-formula><p>Duo to (1.7), we get</p><disp-formula id="scirp.64516-formula639"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x116.png"  xlink:type="simple"/></disp-formula><p>From (2.10), we obtain</p><disp-formula id="scirp.64516-formula640"><label>(2.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x117.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x118.png" xlink:type="simple"/></inline-formula> is a positive constant.</p><p>It follows from (2.1) and (2.5) that</p><disp-formula id="scirp.64516-formula641"><label>(2.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x119.png"  xlink:type="simple"/></disp-formula><p>Moreover, from (2.6), (2.17), (2.13) and (2.19), we have</p><disp-formula id="scirp.64516-formula642"><label>(2.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x120.png"  xlink:type="simple"/></disp-formula><p>for sufficiently large k.</p><p>Duo to (2.21) and (2.22), we get</p><disp-formula id="scirp.64516-formula643"><label>(2.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x121.png"  xlink:type="simple"/></disp-formula><p>which implies that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x122.png" xlink:type="simple"/></inline-formula>. Hence, there exists positive constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x123.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x124.png" xlink:type="simple"/></inline-formula>, holds for all large k, which contradicts to (2.18).</p><p>Case (2): T is infinite. Then we have from (2.6) and (2.17) that</p><disp-formula id="scirp.64516-formula644"><label>(2.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x125.png"  xlink:type="simple"/></disp-formula><p>which implies that</p><disp-formula id="scirp.64516-formula645"><label>(2.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x126.png"  xlink:type="simple"/></disp-formula><p>The above equality together with the updating rule of (2.12) means</p><disp-formula id="scirp.64516-formula646"><label>(2.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x127.png"  xlink:type="simple"/></disp-formula><p>Similar to (2.20), it follows from (2.25) and (2.26) that</p><disp-formula id="scirp.64516-formula647"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x128.png"  xlink:type="simple"/></disp-formula><p>for some positive constant<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x129.png" xlink:type="simple"/></inline-formula>. Then we have</p><disp-formula id="scirp.64516-formula648"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x130.png"  xlink:type="simple"/></disp-formula><p>This equality together with (2.24) yields</p><disp-formula id="scirp.64516-formula649"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x131.png"  xlink:type="simple"/></disp-formula><p>which implies that</p><disp-formula id="scirp.64516-formula650"><label>(2.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x132.png"  xlink:type="simple"/></disp-formula><p>It follows from (2.8), (2.27), (2.26) and (2.20) that</p><disp-formula id="scirp.64516-formula651"><label>(2.28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x133.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x134.png" xlink:type="simple"/></inline-formula> from (2.8), we have from (2.13), (2.17) and (2.28) that</p><disp-formula id="scirp.64516-formula652"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x135.png"  xlink:type="simple"/></disp-formula><p>which means</p><disp-formula id="scirp.64516-formula653"><label>(2.29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x136.png"  xlink:type="simple"/></disp-formula><p>By the same analysis as (2.23) we know that</p><disp-formula id="scirp.64516-formula654"><label>(2.30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x137.png"  xlink:type="simple"/></disp-formula><p>Hence, there exists a positive constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x138.png" xlink:type="simple"/></inline-formula> such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x138.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x139.png" xlink:type="simple"/></inline-formula> holds for all sufficiently large k, which gives a contradiction to (2.29). The proof is completed. ♢</p></sec><sec id="s3"><title>3. Numerical Experiments</title><p>In this section, we test the performance of Algorithm 2.1 on the unconstrained nonlinear optimization problem, and compared it with a regularized Newton method without correction. The function to be minimized is</p><disp-formula id="scirp.64516-formula655"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-2730118x140.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x141.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x142.png" xlink:type="simple"/></inline-formula> are constants. It is clear that function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x143.png" xlink:type="simple"/></inline-formula> is convex and the minimizer set of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x144.png" xlink:type="simple"/></inline-formula> is</p><disp-formula id="scirp.64516-formula656"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x145.png"  xlink:type="simple"/></disp-formula><p>The Hessian <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x146.png" xlink:type="simple"/></inline-formula> is given by</p><disp-formula id="scirp.64516-formula657"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x147.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x148.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x149.png" xlink:type="simple"/></inline-formula>. Matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x150.png" xlink:type="simple"/></inline-formula> is positive semidefinite for all x, but</p><p>singular as the sum of every column is zero. Since the Hessian <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x151.png" xlink:type="simple"/></inline-formula> is always singular, the Newton method cannot be used to solve nonlinear Equations (1.2). But by using the regularization technique, both regularized Newton method and Algorithm 2.1 work quite well.</p><p>The aims of the experiments are as follows: to check whether Algorithm 2.1 converges quadratically as stated in Section 3 and also to see how well the technique of correction works. We set<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x153.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x154.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x155.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x156.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x157.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x155.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x156.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x158.png" xlink:type="simple"/></inline-formula> for Algorithm 2.1.</p><p><xref ref-type="table" rid="table1">Table 1</xref> reports the norms of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x159.png" xlink:type="simple"/></inline-formula> at every iteration when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x160.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x159.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x160.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x161.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x162.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x163.png" xlink:type="simple"/></inline-formula>. Algorithm 2.1 only take four iterations to obtain the minimizer of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x164.png" xlink:type="simple"/></inline-formula>; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x165.png" xlink:type="simple"/></inline-formula>decreases very quickly. The results show the sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x164.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x165.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x166.png" xlink:type="simple"/></inline-formula> quadratic convergence. The iteration is as follows</p><disp-formula id="scirp.64516-formula658"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x167.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64516-formula659"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x168.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64516-formula660"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x169.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64516-formula661"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x170.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64516-formula662"><graphic  xlink:href="http://html.scirp.org/file/6-2730118x171.png"  xlink:type="simple"/></disp-formula><p>We may observe that the whole sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x172.png" xlink:type="simple"/></inline-formula> converges to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x172.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x173.png" xlink:type="simple"/></inline-formula>.</p><p>We also ran the regularized Newton algorithm (RNA) without correction, that is, we do not solve the linear equations (2.9)-(2.10) and just set the solution of (2.8) to be the trial step. Then, we tested the regularized Newton algorithm without correction and Algorithm 2.1 for various of n, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula>and different choices of the starting point. The results are listed in <xref ref-type="table" rid="table2">Table 2</xref>.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula>: the selected value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula>; Dim: the dimension n of the problem;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula>: the ith element<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x178.png" xlink:type="simple"/></inline-formula>; niter: the number of iterations required;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x179.png" xlink:type="simple"/></inline-formula>: the final value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x180.png" xlink:type="simple"/></inline-formula>;<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x181.png" xlink:type="simple"/></inline-formula>: the final value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x182.png" xlink:type="simple"/></inline-formula>. We use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x174.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x175.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x176.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x177.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x178.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x179.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x180.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x181.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x182.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x183.png" xlink:type="simple"/></inline-formula> as the stopping criterion.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Results of Algorithm 2.1 to test quadratic convergence</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >k</th><th align="center" valign="middle" >0</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >5</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x184.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.8856</td><td align="center" valign="middle" >0.4890</td><td align="center" valign="middle" >0.0315</td><td align="center" valign="middle" >1.0368e−05</td><td align="center" valign="middle" >5.6523e−15</td><td align="center" valign="middle" >0</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Results of RNA and Algorithm 2.1</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x185.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x186.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x187.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >niter</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x188.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x189.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle"  rowspan="8"  >0</td><td align="center" valign="middle"  rowspan="2"  >10</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >3/1</td><td align="center" valign="middle" >1.63e−07</td><td align="center" valign="middle" >5.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >2/1</td><td align="center" valign="middle" >1.85e−06</td><td align="center" valign="middle" >0.2929</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >50</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >13/4</td><td align="center" valign="middle" >4.28e−06</td><td align="center" valign="middle" >25.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >19/6</td><td align="center" valign="middle" >4.28e−06</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >100</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >16/3</td><td align="center" valign="middle" >1.62e−06</td><td align="center" valign="middle" >50.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >5/2</td><td align="center" valign="middle" >1.15e−08</td><td align="center" valign="middle" >0.519</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >500</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >49/6</td><td align="center" valign="middle" >6.31e−07</td><td align="center" valign="middle" >250.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >18/8</td><td align="center" valign="middle" >2.08e−08</td><td align="center" valign="middle" >0.0136</td></tr><tr><td align="center" valign="middle"  rowspan="8"  >1</td><td align="center" valign="middle"  rowspan="2"  >10</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >5/1</td><td align="center" valign="middle" >2.66e−06</td><td align="center" valign="middle" >5.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >8/2</td><td align="center" valign="middle" >5.6e−12</td><td align="center" valign="middle" >0.2929</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >50</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >7/3</td><td align="center" valign="middle" >3.84e−10</td><td align="center" valign="middle" >25.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >25/14</td><td align="center" valign="middle" >4.86e−09</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >100</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >8/2</td><td align="center" valign="middle" >4.95e−06</td><td align="center" valign="middle" >50.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >11/5</td><td align="center" valign="middle" >2.30e−06</td><td align="center" valign="middle" >0.519</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >500</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >38/19</td><td align="center" valign="middle" >3.45e−07</td><td align="center" valign="middle" >250.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >11/5</td><td align="center" valign="middle" >5.48e−06</td><td align="center" valign="middle" >0.0136</td></tr><tr><td align="center" valign="middle"  rowspan="8"  >i</td><td align="center" valign="middle"  rowspan="2"  >10</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >9/4</td><td align="center" valign="middle" >9.56e−08</td><td align="center" valign="middle" >5.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >5/1</td><td align="center" valign="middle" >9.00e−06</td><td align="center" valign="middle" >0.2929</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >50</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >39/16</td><td align="center" valign="middle" >2.77e−07</td><td align="center" valign="middle" >25.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >19/10</td><td align="center" valign="middle" >3.10e−08</td><td align="center" valign="middle" >0.09</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >100</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >59/35</td><td align="center" valign="middle" >4.85e−07</td><td align="center" valign="middle" >50.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >19/10</td><td align="center" valign="middle" >2.81e−06</td><td align="center" valign="middle" >0.519</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >500</td><td align="center" valign="middle" >i</td><td align="center" valign="middle" >45/23</td><td align="center" valign="middle" >6.20e−07</td><td align="center" valign="middle" >250.5</td></tr><tr><td align="center" valign="middle" >1/i</td><td align="center" valign="middle" >19/10</td><td align="center" valign="middle" >1.56e−06</td><td align="center" valign="middle" >0.0136</td></tr></tbody></table></table-wrap><p>Moreover, we can see for the same<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x190.png" xlink:type="simple"/></inline-formula>, n and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x190.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-2730118x191.png" xlink:type="simple"/></inline-formula>, the number of iterations of Algorithm 2.1 is always less than that of RNA. And the correction term does help to improve RNA when the initial point is far away from the minimizer. These facts indicate that the introduction of correction is really useful and could accelerate the convergence of the regularized Newton method.</p></sec><sec id="s4"><title>4. Concluding Remarks</title><p>In this paper, we propose a regularized Newton method with correction for unconstrained convex optimization. At every iteration, not only a RNM step is computed but also two correction steps are computed which make use of the previous available Jacobian instead of computing the new Jacobian. Numerical experiments suggest that the introduction of correction is really useful.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This research is supported by the National Natural Science Foundation of China (11426155) and the Hujiang Foundation of China (B14005).</p></sec><sec id="s6"><title>Cite this paper</title><p>LimingLi,MeiQin,HengWang, (2016) A Regularized Newton Method with Correction for Unconstrained Convex Optimization. Open Journal of Optimization,05,44-52. doi: 10.4236/ojop.2016.51006</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.64516-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Yang, W.W., Yang, Y.T., Zhang, C.H. and Cao, M.Y. (2013) A Newton-Like Trust Region Method for Large-Scale Unconstrained Nonconvex Minimization. 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