<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2016.44067</article-id><article-id pub-id-type="publisher-id">JAMP-65442</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 Note on Parameterized Preconditioned Method for Singular Saddle Point Problems
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yueyan</surname><given-names>Lv</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>Naimin</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematics and Information Science, Wenzhou University, Wenzhou, China</addr-line></aff><pub-date pub-type="epub"><day>13</day><month>04</month><year>2016</year></pub-date><volume>04</volume><issue>04</issue><fpage>608</fpage><lpage>613</lpage><history><date date-type="received"><day>3</day>	<month>December</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>6</month>	<year>April</year>	</date><date date-type="accepted"><day>13</day>	<month>April</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>
 
 
   Recently, some authors (Li, Yang and Wu, 2014) studied the parameterized preconditioned HSS (PPHSS) method for solving saddle point problems. In this short note, we further discuss the PPHSS method for solving singular saddle point problems. We prove the semi-convergence of the PPHSS method under some conditions. Numerical experiments are given to illustrate the efficiency of the method with appropriate parameters. 
 
</p></abstract><kwd-group><kwd>Singular Saddle Point Problems</kwd><kwd> Hermitian and Skew-Hermitian Splitting</kwd><kwd> Preconditioning</kwd><kwd>  Iteration Methods</kwd><kwd> Semi-Convergence</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We consider the iterative solution of the following linear system:</p><disp-formula id="scirp.65442-formula167"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x5.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x6.png" xlink:type="simple"/></inline-formula> is Hermitian positive definite, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x7.png" xlink:type="simple"/></inline-formula>is rank-deficient, i.e., <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x8.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x9.png" xlink:type="simple"/></inline-formula>denotes the conjugate transpose of E, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x10.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x11.png" xlink:type="simple"/></inline-formula>. Linear systems of the form (1) are called saddle point problems. They arise in many application areas, including computational fluid dynamics, constrained optimization and weighted least-squares problem, see, e.g., [<xref ref-type="bibr" rid="scirp.65442-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.65442-ref2">2</xref>].</p><p>We review the Hermitian and skew-Hermitian splitting (HSS) [<xref ref-type="bibr" rid="scirp.65442-ref3">3</xref>] of coefficient matrix A:</p><disp-formula id="scirp.65442-formula168"><graphic  xlink:href="http://html.scirp.org/file/65442x12.png"  xlink:type="simple"/></disp-formula><p>where</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x13.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x14.png" xlink:type="simple"/></inline-formula>.</p><p>The PPHSS Iteration Method ([<xref ref-type="bibr" rid="scirp.65442-ref4">4</xref>]): Denote<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x15.png" xlink:type="simple"/></inline-formula>. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x16.png" xlink:type="simple"/></inline-formula> be an arbitrary initial guess, compute <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x17.png" xlink:type="simple"/></inline-formula> for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x18.png" xlink:type="simple"/></inline-formula> by the following iteration scheme until <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x19.png" xlink:type="simple"/></inline-formula> converges,</p><disp-formula id="scirp.65442-formula169"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x20.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x21.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x22.png" xlink:type="simple"/></inline-formula>are given positive constants and</p><disp-formula id="scirp.65442-formula170"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x23.png"  xlink:type="simple"/></disp-formula><p>matrix C is Hermitian positive definite.</p><p>Evidently, the iteration scheme (2) of PPHSS method can be rewritten as</p><disp-formula id="scirp.65442-formula171"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x24.png"  xlink:type="simple"/></disp-formula><p>here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x25.png" xlink:type="simple"/></inline-formula>is the iteration matrix of the PPHSS method. In fact, Equation (4) may also result from the splitting</p><disp-formula id="scirp.65442-formula172"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x26.png"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.65442-formula173"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x27.png"  xlink:type="simple"/></disp-formula><p>Evidently, the matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x28.png" xlink:type="simple"/></inline-formula> can act as a preconditioner for solving the linear system (1), which is called the PPHSS preconditioner. The PPHSS method is a special case of the generalized preconditioned HSS (GHSS) method [<xref ref-type="bibr" rid="scirp.65442-ref5">5</xref>]. When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x29.png" xlink:type="simple"/></inline-formula>, we can obtain a special case of the PPHSS (SPPHSS) method. In order to analyze the semi-convergence of the PPHSS iteration, we let</p><disp-formula id="scirp.65442-formula174"><graphic  xlink:href="http://html.scirp.org/file/65442x30.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x31.png" xlink:type="simple"/></inline-formula> is the identity matrix of order p and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x32.png" xlink:type="simple"/></inline-formula>. In the same way, we denote</p><disp-formula id="scirp.65442-formula175"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x33.png"  xlink:type="simple"/></disp-formula><p>Owing to the similarity of the matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x34.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x35.png" xlink:type="simple"/></inline-formula>, we only need to study the spectral properties of matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x36.png" xlink:type="simple"/></inline-formula> in order to analyze the semi-convergence of the PPHSS iteration.</p></sec><sec id="s2"><title>2. The Semi-Convergence of the PPHSS Method</title><p>As the coefficient matrix A is singular, then the iteration matrix T has eigenvalue 1, and the spectral radius of matrix T cannot be small than 1. For the iteration matrix T of the singular linear systems, we introduce its pseudo-spectral radius <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x37.png" xlink:type="simple"/></inline-formula> by follows,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x38.png" xlink:type="simple"/></inline-formula>,</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x39.png" xlink:type="simple"/></inline-formula> is the set of eigenvalues of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x40.png" xlink:type="simple"/></inline-formula>.</p><p>For a matrix<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x41.png" xlink:type="simple"/></inline-formula>, the smallest nonnegative integer i such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x42.png" xlink:type="simple"/></inline-formula> is called the index of K, and we denote it by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x43.png" xlink:type="simple"/></inline-formula>. In fact, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x44.png" xlink:type="simple"/></inline-formula>is the size of the largest Jordan block corresponding to the zero eigenvalue of K.</p><p>Lemma 2.1 ([<xref ref-type="bibr" rid="scirp.65442-ref6">6</xref>]). The iterative method (4) is semi-convergent, if and only if,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x45.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x46.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 2.2 ([<xref ref-type="bibr" rid="scirp.65442-ref7">7</xref>]).<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x47.png" xlink:type="simple"/></inline-formula>, if and only if, for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x48.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x49.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 2.3. Assume that B and C be Hermitian positive definite, E be of rank-deficient. Then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x50.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. The proof is similar to the proof of Lemma 2.8 in [<xref ref-type="bibr" rid="scirp.65442-ref8">8</xref>], here is omitted.</p><p>Lemma 2.4 ([<xref ref-type="bibr" rid="scirp.65442-ref4">4</xref>]). Let B and C be Hermitian positive definite, E be of rank-deficient. Assume that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x51.png" xlink:type="simple"/></inline-formula>. Then, we can partition <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x52.png" xlink:type="simple"/></inline-formula> in Equation (7) as</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x53.png" xlink:type="simple"/></inline-formula>.</p><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x54.png" xlink:type="simple"/></inline-formula> be the singular value decomposition [<xref ref-type="bibr" rid="scirp.65442-ref9">9</xref>] of E, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x55.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x56.png" xlink:type="simple"/></inline-formula> are unitary matrices, and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x57.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x58.png" xlink:type="simple"/></inline-formula>are the singular values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x59.png" xlink:type="simple"/></inline-formula>.</p><p>Lemma 2.5. The eigenvalues of the iteration matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x60.png" xlink:type="simple"/></inline-formula> of PPHSS iteration method are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x61.png" xlink:type="simple"/></inline-formula> with multiplicity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x62.png" xlink:type="simple"/></inline-formula>, and the roots of quadratic equation</p><p><img data-original="http://html.scirp.org/file/65442x63.png" />,<img data-original="http://html.scirp.org/file/65442x64.png" /> (8)</p><p>Proof. Notice the similarity of matrices <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x65.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x66.png" xlink:type="simple"/></inline-formula>. The proof is essentially analogous to the proof of Lemma 2.3 in [<xref ref-type="bibr" rid="scirp.65442-ref4">4</xref>] with only technical modifications. So, it is omitted.</p><p>Lemma 2.6. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula>, then the eigenvalue <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x68.png" xlink:type="simple"/></inline-formula> of the iteration matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x69.png" xlink:type="simple"/></inline-formula> satisfies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x70.png" xlink:type="simple"/></inline-formula>; if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x71.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x72.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x73.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x74.png" xlink:type="simple"/></inline-formula>, we give the proof by contradiction. By Lemma 2.5, obviously, when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x75.png" xlink:type="simple"/></inline-formula>, it can not be equal to 1. We assume<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x75.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x76.png" xlink:type="simple"/></inline-formula>, by some algebra, it can be reduced to</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x77.png" xlink:type="simple"/></inline-formula>,</p><p>here, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x78.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x79.png" xlink:type="simple"/></inline-formula>. It is equivalent to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x80.png" xlink:type="simple"/></inline-formula>, so<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x81.png" xlink:type="simple"/></inline-formula>, which is in contradiction with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x82.png" xlink:type="simple"/></inline-formula>.</p><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x83.png" xlink:type="simple"/></inline-formula>, we have <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x84.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x85.png" xlink:type="simple"/></inline-formula>, which finishes the proof.</p><p>Lemma 2.7 ([<xref ref-type="bibr" rid="scirp.65442-ref10">10</xref>]). Both roots of the real quadratic equation are less than one in modulus if and only if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x86.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x87.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 2.8. If the iteration parameters <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x88.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x89.png" xlink:type="simple"/></inline-formula></p><p><img data-original="http://html.scirp.org/file/65442x90.png" />,<img data-original="http://html.scirp.org/file/65442x91.png" /> (9)</p><p>then, the pseudo-spectral radius of the PPHSS method satisfies<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x92.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. Using condition (9), it follows that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x93.png" xlink:type="simple"/></inline-formula>. According to Lemma 2.5, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x94.png" xlink:type="simple"/></inline-formula>, we can obtain that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x95.png" xlink:type="simple"/></inline-formula>,</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x96.png" xlink:type="simple"/></inline-formula>.</p><p>By Lemma 2.7, for the eigenvalues <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x97.png" xlink:type="simple"/></inline-formula> of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x98.png" xlink:type="simple"/></inline-formula>, it holds<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x99.png" xlink:type="simple"/></inline-formula>.</p><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x100.png" xlink:type="simple"/></inline-formula>, by Lemma 2.6, the eigenvalues of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x101.png" xlink:type="simple"/></inline-formula>, except 1 are<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x102.png" xlink:type="simple"/></inline-formula>. According to the definition of pseudo-spectral, we get<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x103.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 2.9. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x104.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x105.png" xlink:type="simple"/></inline-formula>. Then, the optimal value of the iteration parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x106.png" xlink:type="simple"/></inline-formula> for the SPPHSS iteration method is given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x107.png" xlink:type="simple"/></inline-formula>,</p><p>and correspondingly,</p><disp-formula id="scirp.65442-formula176"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/65442x108.png"  xlink:type="simple"/></disp-formula><p>Proof. According to Lemma 2.5 and Lemma 2.6, we know that the eigenvalues of the iteration matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x109.png" xlink:type="simple"/></inline-formula> are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x110.png" xlink:type="simple"/></inline-formula> with multiplicity p, and</p><p><img data-original="http://html.scirp.org/file/65442x111.png" />,<img data-original="http://html.scirp.org/file/65442x112.png" /> (11)</p><p>If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x113.png" xlink:type="simple"/></inline-formula>, the eigenvalues with the form of Equation (11) are 1, which can not affect the value of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x114.png" xlink:type="simple"/></inline-formula>. Therefore, without loss of generality, here we only need to discuss the case<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x115.png" xlink:type="simple"/></inline-formula>. The rest is similar to that of the proof of Theorem 3.1 in [<xref ref-type="bibr" rid="scirp.65442-ref4">4</xref>], here is omitted.</p></sec><sec id="s3"><title>3. Numerical Results</title><p>In this section, we use an example to demonstrate the numerical results of the PPHSS method as a solver by comparing its iteration steps (IT), elapsed CPU time in seconds (CPU) and relative residual error (RES) with other methods. The iteration is terminated once the current iterate satisfies <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x116.png" xlink:type="simple"/></inline-formula> or the number of the prescribed iteration steps <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x116.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x117.png" xlink:type="simple"/></inline-formula> are exceeded. All the computations are implemented in MATLAB on a PC computer with Intel (R) Celeron (R) CPU 1000M @ 1.80 GHz, and 2.00 GB memory.</p><p>Example 3.1 ([<xref ref-type="bibr" rid="scirp.65442-ref11">11</xref>]). Consider the saddle point problem (1), with the following block form of coefficient matrix:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x118.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x118.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x119.png" xlink:type="simple"/></inline-formula>,</p><p>where symbol <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x120.png" xlink:type="simple"/></inline-formula> denotes the Kronecker product, and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x121.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x122.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x123.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x121.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x122.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x123.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x124.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x125.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x126.png" xlink:type="simple"/></inline-formula> ,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x125.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x126.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x127.png" xlink:type="simple"/></inline-formula> ,</p><p>the right-hand side vector b is chosen by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x128.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x129.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x130.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x128.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x129.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x130.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x131.png" xlink:type="simple"/></inline-formula>.</p><p>For the Example 3.1, we choose <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x132.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x133.png" xlink:type="simple"/></inline-formula> is the block diagonal matrix of B. In <xref ref-type="table" rid="table1">Table 1</xref>, it is</p><p>clear to see that the pseudo-spectral radius of the PPHSS and the SPPHSS methods are much smaller than of the PHSS method when the optimal parameters are employed. In <xref ref-type="table" rid="table2">Table 2</xref>, we list numerical results with respect to</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The optimal iteration parameters and pseudo-spectral radius</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Method</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x134.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >8</th><th align="center" valign="middle" >16</th><th align="center" valign="middle" >24</th><th align="center" valign="middle" >32</th></tr></thead><tr><td align="center" valign="middle"  rowspan="2"  >PHSS</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x135.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.6328</td><td align="center" valign="middle" >2.1999</td><td align="center" valign="middle" >2.6511</td><td align="center" valign="middle" >3.0367</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x136.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.6756</td><td align="center" valign="middle" >0.8112</td><td align="center" valign="middle" >0.8667</td><td align="center" valign="middle" >0.8969</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >SPPHSS</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x137.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.0216</td><td align="center" valign="middle" >1.0059</td><td align="center" valign="middle" >1.0027</td><td align="center" valign="middle" >1.0015</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x138.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.4947</td><td align="center" valign="middle" >0.4985</td><td align="center" valign="middle" >0.4993</td><td align="center" valign="middle" >0.4996</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >PPHSS</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x139.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.9815</td><td align="center" valign="middle" >2.6990</td><td align="center" valign="middle" >2.5976</td><td align="center" valign="middle" >2.9953</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x140.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.6853</td><td align="center" valign="middle" >0.7845</td><td align="center" valign="middle" >1.0336</td><td align="center" valign="middle" >1.1234</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x141.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.5209</td><td align="center" valign="middle" >0.5258</td><td align="center" valign="middle" >0.5340</td><td align="center" valign="middle" >0.5452</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> IT, CPU and RES for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x142.png" xlink:type="simple"/></inline-formula></title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Method</th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x143.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >8</th><th align="center" valign="middle" >16</th><th align="center" valign="middle" >24</th><th align="center" valign="middle" >32</th></tr></thead><tr><td align="center" valign="middle"  rowspan="3"  >PHSS</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >37</td><td align="center" valign="middle" >47</td><td align="center" valign="middle" >54</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >0.399</td><td align="center" valign="middle" >1.548</td><td align="center" valign="middle" >7.286</td><td align="center" valign="middle" >27.178</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x144.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >6.6914</td><td align="center" valign="middle" >7.2250</td><td align="center" valign="middle" >7.3711</td><td align="center" valign="middle" >9.3294</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >SPPHSS</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >26</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >1.075</td><td align="center" valign="middle" >1.583</td><td align="center" valign="middle" >4.879</td><td align="center" valign="middle" >8.610</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x145.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >5.3781</td><td align="center" valign="middle" >6.7198</td><td align="center" valign="middle" >7.0689</td><td align="center" valign="middle" >7.2124</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >PPHSS</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >0.220</td><td align="center" valign="middle" >1.008</td><td align="center" valign="middle" >3.620</td><td align="center" valign="middle" >12.558</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x146.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >7.8783</td><td align="center" valign="middle" >7.6704</td><td align="center" valign="middle" >7.7535</td><td align="center" valign="middle" >8.1446</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >GMRES</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >883</td><td align="center" valign="middle" >2560</td><td align="center" valign="middle" >5450</td><td align="center" valign="middle" >10376</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >0.524</td><td align="center" valign="middle" >3.179</td><td align="center" valign="middle" >12.572</td><td align="center" valign="middle" >16.264</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x147.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >9.8243</td><td align="center" valign="middle" >9.9925</td><td align="center" valign="middle" >9.9903</td><td align="center" valign="middle" >9.9950</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >PHSS-GMRES</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >22</td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >44</td><td align="center" valign="middle" >50</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >0.111</td><td align="center" valign="middle" >0.467</td><td align="center" valign="middle" >1.649</td><td align="center" valign="middle" >3.751</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x148.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >9.6710</td><td align="center" valign="middle" >8.0874</td><td align="center" valign="middle" >9.3990</td><td align="center" valign="middle" >9.8588</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >SPPHSS-GMRES</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >14</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >0.082</td><td align="center" valign="middle" >0.372</td><td align="center" valign="middle" >1.831</td><td align="center" valign="middle" >3.892</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x149.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >4.7178</td><td align="center" valign="middle" >6.7487</td><td align="center" valign="middle" >6.2498</td><td align="center" valign="middle" >4.2212</td></tr><tr><td align="center" valign="middle"  rowspan="3"  >PPHSS-GMRES</td><td align="center" valign="middle" >IT</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle" >CPU</td><td align="center" valign="middle" >0.070</td><td align="center" valign="middle" >0.428</td><td align="center" valign="middle" >1.564</td><td align="center" valign="middle" >3.366</td></tr><tr><td align="center" valign="middle" >RES (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x150.png" xlink:type="simple"/></inline-formula>)</td><td align="center" valign="middle" >5.4534</td><td align="center" valign="middle" >2.3975</td><td align="center" valign="middle" >9.8449</td><td align="center" valign="middle" >9.8690</td></tr></tbody></table></table-wrap><p>IT, CPU and RES of the texting methods with different problem sizes l. We see that the PPHSS and SPPHSS methods with appropriate parameters always outperforms the PHSS method both as a solver and as a preconditioner for GMRES in iteration steps and CPU times. Notice</p><disp-formula id="scirp.65442-formula177"><graphic  xlink:href="http://html.scirp.org/file/65442x151.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x152.png" xlink:type="simple"/></inline-formula>. To compute the matrix-vector products with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x153.png" xlink:type="simple"/></inline-formula>, we make incomplete LU factorization of B and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/65442x154.png" xlink:type="simple"/></inline-formula> with drop tolerance 0.001. In the two tables, we use restarted GMRES (18) and preconditioned GMRES (18).</p></sec><sec id="s4"><title>Cite this paper</title><p>Yueyan Lv,Naimin Zhang, (2016) A Note on Parameterized Preconditioned Method for Singular Saddle Point Problems. 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