<?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">AJCM</journal-id><journal-title-group><journal-title>American Journal of Computational Mathematics</journal-title></journal-title-group><issn pub-type="epub">2161-1203</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajcm.2015.52005</article-id><article-id pub-id-type="publisher-id">AJCM-56453</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  A Simple Proof of Gustafsson’s Conjecture in Case of Poisson Equation on Rectangular Domains
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>angjoon</surname><given-names>Yoon</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>Chohong</surname><given-names>Min</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="aff1"><addr-line>Institute of Mathematical Sciences, Ewha Womans University, Seoul, South Korea</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematics, Ewha Womans University, Seoul, South Korea</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>gangjoon@gmail.com(AY)</email>;<email>chohong@ewha.ac.kr(CM)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>13</day><month>05</month><year>2015</year></pub-date><volume>05</volume><issue>02</issue><fpage>75</fpage><lpage>79</lpage><history><date date-type="received"><day>6</day>	<month>March</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>17</month>	<year>May</year>	</date><date date-type="accepted"><day>20</day>	<month>May</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><html>
 <head></head>
 
  We consider the standard five-point finite difference method for solving the Poisson equation with the Dirichlet boundary condition. Its associated matrix is a typical ill-conditioned matrix whose size of the condition number is as big as 
  <img src="Edit_c31c9900-cc31-4bc0-9ac3-29fe8861d8e4.bmp" alt="" />. Among ILU, SGS, modified ILU (MILU) and other ILU-type preconditioners, Gustafson shows that only MILU achieves an enhancement of the condition number in different order as 
  <img src="Edit_0ba2485e-5970-4558-9b3a-2416cab82ec3.bmp" alt="" />. His seminal work, however, is not for the MILU but for a perturbed version of MILU and he observes that without the perurbation, it seems to reach the same result in practice. In this work, we give a simple proof of Gustafsson's conjecture on the unnecessity of perturbation in case of Poisson equation on rectangular domains. Using the Cuthill-Mckee ordering, we simplify the recursive equation in two dimensional grid nodes into a recursive one in the level that is one-dimensional. Due to the simplification, our proof is easy to follow and very short.
 
</html></p></abstract><kwd-group><kwd>Five-Point Finite Difference Method</kwd><kwd> Modified ILU Preconditioning</kwd><kwd> Condition Number</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Consider the standard five-point finite difference method for solving the Poisson equation with the Dirichlet boundary condition. Its associated matrix is a typical ill-conditioned matrix whose condition number is of size<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x7.png" xlink:type="simple"/></inline-formula>, where h is the grid size. In mitigating the large size, Dupont, Kendall and Rachfold [<xref ref-type="bibr" rid="scirp.56453-ref1">1</xref>] propose a preconditioning technique which works quite well for elliptic problems with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x8.png" xlink:type="simple"/></inline-formula> convergence rate, which is a simple modification of incomplete LU (ILU) and called the modified ILU (MILU) preconditioning techni- que. The MILU requires all the same row sums for the preconditioner and the original matrices. Also, Gusta- fsson [<xref ref-type="bibr" rid="scirp.56453-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.56453-ref3">3</xref>] shows that the MILU preconditiong reduces the size to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x9.png" xlink:type="simple"/></inline-formula>, while other popular precon- ditionings such as ILU and symmetric Gauss-Seidel (SGS) do not improve the order. Numerical study by Greenbaum and Rodrigue [<xref ref-type="bibr" rid="scirp.56453-ref4">4</xref>] indicates that further reduction is not possible with the same sparsity pattern.</p><p>The MILU preconditioing introduced by Axelsson [<xref ref-type="bibr" rid="scirp.56453-ref5">5</xref>] and developed by Gustafsson [<xref ref-type="bibr" rid="scirp.56453-ref2">2</xref>] adds some artificial diagonal perturbation on the orginal matrix. In [<xref ref-type="bibr" rid="scirp.56453-ref1">1</xref>] and [<xref ref-type="bibr" rid="scirp.56453-ref2">2</xref>] , it is found that a small positive perturbation improves the convergence rate quite well for many elliptic problems. We refer to [<xref ref-type="bibr" rid="scirp.56453-ref6">6</xref>] -[<xref ref-type="bibr" rid="scirp.56453-ref9">9</xref>] and references therein for more results and details.</p><p>The numerical experiments [<xref ref-type="bibr" rid="scirp.56453-ref10">10</xref>] with Dirichlet boundary condition, however, suggest that the perturbation is unnecessary. It is Gustafsson’s conjecture [<xref ref-type="bibr" rid="scirp.56453-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.56453-ref11">11</xref>] to prove the estimate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x10.png" xlink:type="simple"/></inline-formula> for the unperturbed MILU preconditioing. Beauwens [<xref ref-type="bibr" rid="scirp.56453-ref12">12</xref>] considers a general setting that includes the five-point method, and proves the conjecture using the matrix-graph connectivity properties (see also [<xref ref-type="bibr" rid="scirp.56453-ref13">13</xref>] ). Beauwens’ proof deals with a Stieltjes matrix under several assumptions. Notay [<xref ref-type="bibr" rid="scirp.56453-ref14">14</xref>] also obtains an upper bound <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x11.png" xlink:type="simple"/></inline-formula> for the block MILU with the line partitioning. We also refer the reader to [<xref ref-type="bibr" rid="scirp.56453-ref15">15</xref>] -[<xref ref-type="bibr" rid="scirp.56453-ref18">18</xref>] for related works on Gustafsson’s conjecture.</p><p>We introduce a novel and heuristic proof for the conjecture in case of Poisson equation with Dirichlet boundary condition on rectangular domains. The MILU preconditioner is obtained from recursively calculating the row-sum equation at each grid node in the lexicographical ordering. In the case of the five-point method, it is well known [<xref ref-type="bibr" rid="scirp.56453-ref19">19</xref>] that the same matrix can be obtained in the Cuthill-Mckee ordering. The matrix entry on the</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x12.png" xlink:type="simple"/></inline-formula>node depends only on <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x13.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x14.png" xlink:type="simple"/></inline-formula> nodes, both of which lie on the same level <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x15.png" xlink:type="simple"/></inline-formula> of the Cuthill-Mckee ordering. So we can simplify the recursive equation in two dimensional grid</p><p>nodes into a recursive one in the level that is one dimensional. Due to the simplification, our proof is easy to follow and very short.</p></sec><sec id="s2"><title>2. MILU Preconditioning</title><p>Consider the Poisson equation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x16.png" xlink:type="simple"/></inline-formula> in a rectangular domain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x17.png" xlink:type="simple"/></inline-formula> with the Dirichlet boun- dary condition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x18.png" xlink:type="simple"/></inline-formula> on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x19.png" xlink:type="simple"/></inline-formula>. The standard five-point finite difference method approximates the equation as</p><disp-formula id="scirp.56453-formula242"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x20.png"  xlink:type="simple"/></disp-formula><p>at each grid node<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x21.png" xlink:type="simple"/></inline-formula>. The approximations constitute a linear system<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x22.png" xlink:type="simple"/></inline-formula>. With the lexicographical ordering, we decompose the matrix as</p><disp-formula id="scirp.56453-formula243"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x23.png"  xlink:type="simple"/></disp-formula><p>where L, U, and D are its strictly lower and upper, and diagonal parts, respectively. MILU preconditioner is the matrix of the form<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x24.png" xlink:type="simple"/></inline-formula>, where the diagonal matrix E is obtained recursively as follows.</p><p>for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x25.png" xlink:type="simple"/></inline-formula></p><p>for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x26.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.56453-formula244"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x27.png"  xlink:type="simple"/></disp-formula><p>Here <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula> denotes the diagonal element of E corresponding to the node point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x29.png" xlink:type="simple"/></inline-formula>, i.e.<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x30.png" xlink:type="simple"/></inline-formula>. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x31.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x32.png" xlink:type="simple"/></inline-formula> denote the entry <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x33.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x34.png" xlink:type="simple"/></inline-formula>, respectively. Note that the above formula results from</p><p>the row sum property, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x35.png" xlink:type="simple"/></inline-formula>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x36.png" xlink:type="simple"/></inline-formula>. Due to the Dirichlet boundary condition, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x37.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x38.png" xlink:type="simple"/></inline-formula> are either <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x39.png" xlink:type="simple"/></inline-formula> or 0, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x40.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x41.png" xlink:type="simple"/></inline-formula> be a sequence defined recursively as</p><disp-formula id="scirp.56453-formula245"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1100421x42.png"  xlink:type="simple"/></disp-formula><p>Then we have</p><disp-formula id="scirp.56453-formula246"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x43.png"  xlink:type="simple"/></disp-formula><p>Proof. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x44.png" xlink:type="simple"/></inline-formula> be the sequence defined as (1). The lemma is shown by the mathematical induction. Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x45.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x46.png" xlink:type="simple"/></inline-formula> Then</p><disp-formula id="scirp.56453-formula247"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x47.png"  xlink:type="simple"/></disp-formula><p>and this proves the lemma.</p><p>Theorem 1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x48.png" xlink:type="simple"/></inline-formula> be the MILU preconditioner for A. Then, for every diagonal element <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x49.png" xlink:type="simple"/></inline-formula> of E corresponding to the node<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x50.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.56453-formula248"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x51.png"  xlink:type="simple"/></disp-formula><p>and, therefore,</p><disp-formula id="scirp.56453-formula249"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x52.png"  xlink:type="simple"/></disp-formula><p>Proof. We shall show that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula> by mathematical induction on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula>. Then follows the result from the previous lemma. When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x57.png" xlink:type="simple"/></inline-formula>. Assume that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x58.png" xlink:type="simple"/></inline-formula> for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x59.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x60.png" xlink:type="simple"/></inline-formula>. Then for any <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x61.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x62.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.56453-formula250"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x63.png"  xlink:type="simple"/></disp-formula><p>Now, we are ready to estimate the condition number of the MILU preconditioned matrix<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x64.png" xlink:type="simple"/></inline-formula>. The fol- lowing analysis is a standard approach, for the details see [<xref ref-type="bibr" rid="scirp.56453-ref2">2</xref>] . Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x65.png" xlink:type="simple"/></inline-formula> is similar to</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x66.png" xlink:type="simple"/></inline-formula>that is symmetric and positive definite, all the eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x67.png" xlink:type="simple"/></inline-formula> are real and positive. Moreover, the minimum and maximum eigenvalues of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x68.png" xlink:type="simple"/></inline-formula> are given as</p><disp-formula id="scirp.56453-formula251"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1100421x69.png"  xlink:type="simple"/></disp-formula><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x70.png" xlink:type="simple"/></inline-formula> is written in the form</p><disp-formula id="scirp.56453-formula252"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1100421x71.png"  xlink:type="simple"/></disp-formula><p>for the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x72.png" xlink:type="simple"/></inline-formula> (see (b) of <xref ref-type="fig" rid="fig1">Figure 1</xref> for its entries). For arbitrary<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x73.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.56453-formula253"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1100421x74.png"  xlink:type="simple"/></disp-formula><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Matrices A and R. (a) Matrix A; (b) Matrix B = M ? A.</title></caption><fig id ="fig1_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/2-1100421x75.png"/></fig></fig-group><p>Using the inequality <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x76.png" xlink:type="simple"/></inline-formula> and Theorem 1, we also have</p><disp-formula id="scirp.56453-formula254"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x77.png"  xlink:type="simple"/></disp-formula><p>Thus, we obtain the inequalities</p><disp-formula id="scirp.56453-formula255"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1100421x78.png"  xlink:type="simple"/></disp-formula><p>In summary, we have the following.</p><p>Theorem 2. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x79.png" xlink:type="simple"/></inline-formula> be an eigenvalue of the MILU preconditioned matrix, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x80.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.56453-formula256"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1100421x81.png"  xlink:type="simple"/></disp-formula><p>Proof. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x82.png" xlink:type="simple"/></inline-formula> be an eigenvalue of the MILU preconditioned matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x83.png" xlink:type="simple"/></inline-formula> From (5), we have that</p><disp-formula id="scirp.56453-formula257"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x84.png"  xlink:type="simple"/></disp-formula><p>and applying these inequalities above into (2) and (3) gives</p><disp-formula id="scirp.56453-formula258"><graphic  xlink:href="http://html.scirp.org/file/2-1100421x85.png"  xlink:type="simple"/></disp-formula><p>which shows the inequalites (6). On the other hand, the row sum property implies that 1 is an eigenvalue of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x86.png" xlink:type="simple"/></inline-formula>. Thus, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x87.png" xlink:type="simple"/></inline-formula> and we complete the proof.</p><p>Corollary 1. The ratio of the maximum and minimum eigenvalues of the MILU preconditioned matrix is bounded by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1100421x88.png" xlink:type="simple"/></inline-formula>.</p><p>Remark 1. Our analysis deals with the two dimensional Poisson equation. 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