<?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">ALAMT</journal-id><journal-title-group><journal-title>Advances in Linear Algebra &amp; Matrix Theory</journal-title></journal-title-group><issn pub-type="epub">2165-333X</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/alamt.2012.23005</article-id><article-id pub-id-type="publisher-id">ALAMT-22664</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 Modified Precondition in the Gauss-Seidel Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>limohammad</surname><given-names>Nazari</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>Sajjad</surname><given-names>Zia Borujeni</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Faculty of Science, Arak University, Arak, Iran</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>a-nazari@araku.ac.ir(LN)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>24</day><month>09</month><year>2012</year></pub-date><volume>02</volume><issue>03</issue><fpage>31</fpage><lpage>37</lpage><history><date date-type="received"><day>March</day>	<month>6,</month>	<year>2012</year></date><date date-type="rev-recd"><day>June</day>	<month>28,</month>	<year>2012</year>	</date><date date-type="accepted"><day>August</day>	<month>21,</month>	<year>2012</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 recent years, a number of preconditioners have been applied to solve the linear systems with Gauss-Seidel method (see [1-7,10-12,14-16]). In this paper we use S
  <sub>l</sub> instead of (S + S
  <sub>m</sub>) and compare with M. Morimoto’s precondition [3] and H. Niki’s precondition [5] to obtain better convergence rate. A numerical example is given which shows the preference of our method.
 
</p></abstract><kwd-group><kwd>Preconditioning; Gauss-Seidel Method; Regular Splitting; Z-Matrix; Nonnegative Matrix</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Consider the linear system</p><disp-formula id="scirp.22664-formula54741"><label>(1)</label><graphic position="anchor" xlink:href="2-2230006\b507e3af-d9ca-490d-be9c-1ded0e78874b.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="2-2230006\115a8633-3908-445f-934b-041bbb2fd3b3.jpg" /> is a known nonsingular matrix and <img src="2-2230006\3ac58f05-184e-489c-9ac1-a8b34e97137d.jpg" /> are vectors. For any splitting A = M – N with a nonsingular matrix M, the basic splitting iterative method can be expressed as</p><disp-formula id="scirp.22664-formula54742"><label>(2)</label><graphic position="anchor" xlink:href="2-2230006\f4f9aef2-70a5-462d-9699-956058d4280f.jpg"  xlink:type="simple"/></disp-formula><p>Assume that</p><p><img src="2-2230006\f2e8e432-51c3-4722-9120-8fab87b3be17.jpg" /></p><p>without loss of generality we can write</p><disp-formula id="scirp.22664-formula54743"><label>(3)</label><graphic position="anchor" xlink:href="2-2230006\99e408f1-1222-412f-9cfe-d3543d3a3bd3.jpg"  xlink:type="simple"/></disp-formula><p>where I is the identity matrix, <img src="2-2230006\9af9a74b-f9cd-442a-80c6-38f25b7093bd.jpg" />and <img src="2-2230006\63affeea-89e4-4cf2-9ccf-63c3d3c5e436.jpg" /> are strictly lower triangular and strictly upper triangular parts of<img src="2-2230006\810da9bd-9554-4678-adec-4c32dcea4a69.jpg" />, respectively. In order to accelerate the convergence of the iterative method for solving the linear system (1), the original linear system (1) is transformed into the following preconditioned linear system</p><disp-formula id="scirp.22664-formula54744"><label>(4)</label><graphic position="anchor" xlink:href="2-2230006\fa72c7db-c24a-496a-8ced-3b4f6260d7a7.jpg"  xlink:type="simple"/></disp-formula><p>where P, called a preconditioner, is a nonsingular matrix.</p><p>In 1991, Gunawardena et al. [<xref ref-type="bibr" rid="scirp.22664-ref2">2</xref>] considered the modified Gauss-Seidel method with<img src="2-2230006\78e52953-88e3-4624-a531-a036be96b7e2.jpg" />, where</p><p><img src="2-2230006\32303ba5-557d-449d-b9d2-7085ae5914ab.jpg" /></p><p>Then, the preconditioned matrix <img src="2-2230006\9f7453d1-c6af-463d-a3c7-438ebdc02f2e.jpg" /> can be written as</p><p><img src="2-2230006\66ed0912-9a83-4089-88b6-cba9cbaf7056.jpg" /></p><p>where D and E are the diagonal and strictly lower triangular parts of SL, respectively. If <img src="2-2230006\a27a6166-aab8-44ae-ac6d-c0e430470cf5.jpg" />, then <img src="2-2230006\ea119363-1cc9-433a-bc67-52f42fccaab6.jpg" /> exists. Therefore, the preconditioned Gauss-Seidel iterative matrix <img src="2-2230006\d7c9ee21-3daf-4d15-8fa5-ca17389762df.jpg" /> for <img src="2-2230006\3c3ec62d-d33c-4cb0-9d59-582d96c4c4ac.jpg" /> becomes</p><p><img src="2-2230006\9e596e4a-27c5-4cb5-892a-ad1c71c06f7d.jpg" /></p><p>which is referred to as the modified Gauss-Seidel iterative matrix. Gunawardena et al. proved the following inequality:</p><p><img src="2-2230006\ecdb2b4a-5fc9-442a-8620-847939ef67e6.jpg" /></p><p>where <img src="2-2230006\511850b0-4de9-46bb-aa5a-e8e9703d4738.jpg" /> denotes the spectral radius of the GaussSeidel iterative matrix T. Morimoto et al. [<xref ref-type="bibr" rid="scirp.22664-ref3">3</xref>] have proposed the following preconditioner,</p><p><img src="2-2230006\e254ef24-d4a5-4dc4-bfe3-09f23d64c0a5.jpg" /></p><p>In this preconditioner, <img src="2-2230006\09550818-71b9-44bf-a7ed-f1d5df60c887.jpg" />is defined by</p><p><img src="2-2230006\74ed2005-7d8f-47f5-b734-629d97faae1b.jpg" /></p><p>where <img src="2-2230006\f96cb291-2258-4ed3-ad1d-7aa17cbe2354.jpg" /> and</p><p><img src="2-2230006\05fc8845-981f-4378-b422-a55c9dd4416e.jpg" />, for</p><p><img src="2-2230006\a2da6f2a-084b-433c-a9a8-f4fa6309fe2c.jpg" />. The preconditioned matrix <img src="2-2230006\ef80dfe9-8827-43d8-bfaf-69f254c03c21.jpg" /> can then be written as</p><p><img src="2-2230006\c41503a9-9afa-43f5-a4af-80a7ba61de41.jpg" /></p><p>where<img src="2-2230006\6d9675cc-109a-4868-9e23-dec78e49953e.jpg" />, <img src="2-2230006\568b1217-b648-4090-b583-010cc70aa89c.jpg" />and <img src="2-2230006\6611e851-4c97-43d7-9001-4826fb7f8142.jpg" /> are the diagonal, strictly lower and strictly upper triangular parts of <img src="2-2230006\96164e56-d9a9-4fb4-b79f-f21533096a79.jpg" /> respectively. Assume that the following inequalities are satisfied:</p><p><img src="2-2230006\1a76c47d-00dd-41fd-b7e1-faf31b4a6760.jpg" /></p><p>Then <img src="2-2230006\7fbe8f2b-a9b2-447b-87ba-a03adf763544.jpg" /> is nonsingular. The preconditioned Gauss-Seidel iterative matrix <img src="2-2230006\16253b83-2a5d-4651-8d9a-bbbd0a3f4c9e.jpg" /> for <img src="2-2230006\d97abe2c-7af9-444b-8482-06a6875912fe.jpg" /> is then defined by</p><p><img src="2-2230006\ee89800b-1f96-448c-9207-220272f16cb6.jpg" /></p><p>Morimoto et al. [<xref ref-type="bibr" rid="scirp.22664-ref3">3</xref>] proved that<img src="2-2230006\2e128d35-42f3-4440-9baf-c42209e90468.jpg" />. To extend the preconditioning effect to the last row, Morimoto et al. [<xref ref-type="bibr" rid="scirp.22664-ref7">7</xref>] proposed the preconditioner</p><p><img src="2-2230006\1c00f2a7-f789-4b2e-8c80-429749ff3b91.jpg" /></p><p>where R is defined by</p><p><img src="2-2230006\4a523061-549c-4e5c-ac47-406a5effbb0a.jpg" /></p><p>The elements <img src="2-2230006\286d1f6c-2771-4def-8385-07ae851c5505.jpg" /> of <img src="2-2230006\4053331f-4385-4ed0-9d9a-8f950309b6bd.jpg" /> are given by</p><p><img src="2-2230006\d6b73272-4ac1-4757-9c50-ec02260a141a.jpg" /></p><p>And Morimoto et al. proved that <img src="2-2230006\6f58f5c8-6751-480f-b922-1b4a282b8cf0.jpg" /> holds, where <img src="2-2230006\07c8dab3-3d5f-4459-8b7e-bf300ba4006d.jpg" /> is the iterative matrix for<img src="2-2230006\aafefc52-dadb-404f-abee-00d60a6dd506.jpg" />. They also presented combined preconditioners, which are given by combinations of R with any upper preconditioner, and showed that the convergence rate of the combined methods are better than those of the Gauss-Seidel method applied with other upper preconditioners [<xref ref-type="bibr" rid="scirp.22664-ref7">7</xref>]. In [<xref ref-type="bibr" rid="scirp.22664-ref14">14</xref>], Niki et al. considered the preconditioner <img src="2-2230006\33fe47ee-e8e1-4d13-bc8f-e3a704991a57.jpg" /> <img src="2-2230006\55c41adc-6efb-4238-b613-98740709912b.jpg" />. Denote<img src="2-2230006\c61fa01f-ab2d-445f-ab94-eed2847bdb44.jpg" />. In [<xref ref-type="bibr" rid="scirp.22664-ref5">5</xref>], Niki et al. proved that if the following inequality is satisfied,</p><disp-formula id="scirp.22664-formula54745"><label>(5)</label><graphic position="anchor" xlink:href="2-2230006\638424da-4ca0-4e8f-b59c-7aa0375d1d60.jpg"  xlink:type="simple"/></disp-formula><p>then <img src="2-2230006\554b38f9-df0c-465d-af82-53520d662fed.jpg" /> holds, where <img src="2-2230006\11b35ab2-d7b3-477a-a28c-ada68351b16e.jpg" /> is the iterative matrix for<img src="2-2230006\6d0a2c54-f19f-43a1-a3cf-1bfb811c06b4.jpg" />. For matrices that do not satisfy Equation</p><p>(5), by putting <img src="2-2230006\0ab9ce07-a73c-440f-b9bd-0a216349e34d.jpg" /></p><p>Equation (5) is satisfied. Therefore, Niki et al. [<xref ref-type="bibr" rid="scirp.22664-ref5">5</xref>] proposed a new preconditioner<img src="2-2230006\ceae5b95-92a4-4526-aebf-308280ce5172.jpg" />, where</p><p><img src="2-2230006\98d5a842-6e2e-448d-a59c-6e69e5835b6b.jpg" /></p><p>Put<img src="2-2230006\dbc0ccee-fe4d-451a-8d43-0732c3d021d0.jpg" />, and<img src="2-2230006\4ed016ca-4524-44df-9ab7-29afc17f62dc.jpg" />.</p><p>Replacing <img src="2-2230006\2456cd48-e430-4e91-9af7-69b3087b48fd.jpg" /> by <img src="2-2230006\e2cef7d0-9175-4636-a9df-d76a52bb3b1c.jpg" /> and setting <img src="2-2230006\da2a290a-9424-47df-892d-6a5316de0783.jpg" /> the Gauss-Seidel splitting of <img src="2-2230006\0613f310-3818-43b6-be58-3d2a569a25f3.jpg" /> can be written as</p><p><img src="2-2230006\f0e8e3e2-0b85-493f-9f78-84a8df4efee5.jpg" /></p><p>where <img src="2-2230006\61f7fe16-c5ea-4235-a7f1-b6ba84238525.jpg" /> is constructed by the elements<img src="2-2230006\cae8c81c-359a-4931-b1fa-6363cd067225.jpg" />. Thus, if the preconditioner <img src="2-2230006\f2cf2ef4-6054-4394-901c-77a2f502b0d0.jpg" /> is used, then all of the rows of <img src="2-2230006\1cfaa4fb-f067-4d41-b02b-2a981a761822.jpg" /> are subject to preconditioning. Niki et al. [<xref ref-type="bibr" rid="scirp.22664-ref5">5</xref>] proved that under the condition<img src="2-2230006\dcb9ddfb-d38c-4487-a070-173b054d43f9.jpg" />, <img src="2-2230006\7f2190eb-2cce-47bd-9dfe-7ed1184458d2.jpg" />where <img src="2-2230006\ab8f773f-c16d-4da2-91a0-6a7ba460f15f.jpg" /> is the upper bound of those values of <img src="2-2230006\325686d7-c2db-47a4-b0f8-309f6a5e1b98.jpg" /> for which<img src="2-2230006\d89b969e-0488-4780-8238-3509c49b54ef.jpg" />. By setting<img src="2-2230006\9f80810e-047e-4168-89c3-dc75f0933813.jpg" />, they obtained</p><p><img src="2-2230006\82fbc173-f41d-4236-b21a-0fbf5fa8fa56.jpg" /></p><p>Niki et al. [<xref ref-type="bibr" rid="scirp.22664-ref5">5</xref>] proved that the preconditioner <img src="2-2230006\15324924-f64a-4c43-aaa2-77a6adccce13.jpg" /> satisfies the Equation (5) unconditionally. Moreover, they reported that the convergence rate of the GaussSeidel method using preconditioner <img src="2-2230006\aac43cba-68d9-49a8-80c7-ccad0d0f4832.jpg" /> is better than that of the SOR method using the optimum <img src="2-2230006\56a2196e-3814-400a-90cc-006eea54908d.jpg" /> found by numerical computation. They also reported that there is an optimum <img src="2-2230006\ce8685d1-ec9f-4c5c-a156-7b4b49bddf6a.jpg" /> in the range <img src="2-2230006\521a27d0-48cf-4bdc-b995-6eb13e541c37.jpg" /> which produces an extremely small<img src="2-2230006\fea3efce-ea83-4681-98aa-797e1fc71c51.jpg" />, where <img src="2-2230006\98dc319d-1f10-4e83-a354-4ecc95175483.jpg" /> is the upper bound of the values of <img src="2-2230006\c742763b-8d6f-4d30-bd2e-e696c41abc06.jpg" /> for which<img src="2-2230006\7e7f6c72-1ca9-4d95-ae39-2ef9c924ba38.jpg" />, for all<img src="2-2230006\63127e39-273a-4e2e-aca1-4a0f2b85f6f2.jpg" />.</p><p>In this paper we use different preconditions for solving (1) by Gauss-Siedel method, that assuming none of the components of the matrix <img src="2-2230006\f7035441-0d75-4952-b387-122c3440b130.jpg" /> to be zero. If the largest component of the column j is not <img src="2-2230006\26ac6dc1-71e2-442e-86a2-091bb3c69353.jpg" /> then the value of <img src="2-2230006\06cd4812-8f85-4db2-a5db-be7b9bc9b56b.jpg" /> will be improved.</p></sec><sec id="s2"><title>2. Main Result</title><p>In this section we replace S<sub>l</sub> by <img src="2-2230006\9c53a763-96da-4d1f-a378-c968f7b5af63.jpg" /> of Morimoto such that <img src="2-2230006\48bc80b9-5a12-4af6-bb8b-702e14014f22.jpg" /> and define <img src="2-2230006\b460ba45-7f6b-4ce7-bb1f-d023479716ff.jpg" /> by</p><p><img src="2-2230006\7a10ec86-f711-4832-a885-072a6499ce43.jpg" /></p><p>where <img src="2-2230006\4750f7ab-6789-4d7e-8173-6fe0e9bd9190.jpg" /> s.t<img src="2-2230006\c060f4a3-70b1-4c54-8969-a4d55821e5df.jpg" />, and <img src="2-2230006\1d8e04e6-b3c8-43d9-84ca-52e2ce908fda.jpg" /> has the same form as the <img src="2-2230006\2b15e96e-8a91-4768-a4ba-04bd52c3422b.jpg" /> proposed by Morimoto et al. [<xref ref-type="bibr" rid="scirp.22664-ref3">3</xref>].</p><p>The precondition Matrix <img src="2-2230006\779f5055-05a7-43de-b86d-da0f8c4d0cfb.jpg" /> can then be written as</p><p><img src="2-2230006\327d832b-456d-42f8-95ab-6debdaa6a32d.jpg" /></p><p>where <img src="2-2230006\797de99e-86ba-4232-bc88-d27191b54cfd.jpg" /> and <img src="2-2230006\a1bfa21f-882f-4beb-8545-4e67fc126c82.jpg" /> are the diagonal, strictly lower and strictly upper triangular parts of<img src="2-2230006\eee3213d-afa7-4145-aa2a-5a1e67a71e13.jpg" />, respectively. Assume that the following inequalities are satisfied:</p><disp-formula id="scirp.22664-formula54746"><label>(6)</label><graphic position="anchor" xlink:href="2-2230006\339a20b4-1081-4d62-8040-a3a578ea3978.jpg"  xlink:type="simple"/></disp-formula><p>Therefore <img src="2-2230006\48e78060-08f6-45ff-8def-9c066e27e9a0.jpg" /> exists and the preconditioned GaussSeidel iterative matrix <img src="2-2230006\49d04526-78cb-4fa6-b460-841ffbc27e40.jpg" /> for <img src="2-2230006\5f9b7f72-4e74-46ab-a55e-a87dcf2a21dd.jpg" /> is defined by</p><p><img src="2-2230006\c0e708d3-2c39-423a-94b4-6a2457533511.jpg" /></p><p>For <img src="2-2230006\16afab99-db64-45f8-a678-22a07dc83632.jpg" /> and<img src="2-2230006\3c73655f-5e9a-47ec-b9f2-0840018c047d.jpg" />, we write <img src="2-2230006\70377fed-b755-4a5f-ade2-847d82dc6674.jpg" /> whenever <img src="2-2230006\8e247f4d-b255-4450-b452-86674f01f1c6.jpg" /> holds for all <img src="2-2230006\ee1aab99-18a3-4100-bc49-4ece8a6039a4.jpg" /> A is nonnegative if <img src="2-2230006\9c5e1884-67ad-4799-8017-fc20652069dd.jpg" /> and <img src="2-2230006\018703b8-f38c-4c8f-8168-694b5724de9a.jpg" /> if and only if<img src="2-2230006\5b0755b4-37d4-4800-a869-a632d5b41d4c.jpg" />.</p><p>Definition 2.1 (Young, [<xref ref-type="bibr" rid="scirp.22664-ref15">15</xref>]). A real <img src="2-2230006\0da15cb3-0a34-48a2-adb4-be1276292c94.jpg" /> matrix <img src="2-2230006\dd4ec129-2997-4ff2-b7f9-9a09ba4d93c8.jpg" /> with <img src="2-2230006\8e827580-8883-4d60-bc09-e552749201ee.jpg" /> for all <img src="2-2230006\89de62de-d595-4b4a-8481-9bb8313aa75c.jpg" /> is called a Zmatrix.</p><p>Definition 2.2 (Varga, [<xref ref-type="bibr" rid="scirp.22664-ref16">16</xref>]). A matrix A is irreducible if the directed graph associated to A is strongly connected.</p><p>Lemma 2.3. If A is an irreducible diagonally dominant Z-matrix with unit diagonal, and if the assumption (6) holds, then the preconditioned matrix A<sub>S</sub> is a diagonally dominant Z-matrix.</p><p>Proof. The elements <img src="2-2230006\28de67db-36a6-4232-9cf3-68d7da60015e.jpg" /> of <img src="2-2230006\4190d033-b348-4501-91ba-c8ddf897d261.jpg" /> are given by</p><disp-formula id="scirp.22664-formula54747"><label>(7)</label><graphic position="anchor" xlink:href="2-2230006\10324efe-60fa-473f-84fe-0fe22846fd6c.jpg"  xlink:type="simple"/></disp-formula><p>Since A is a diagonally dominant Z-matrix, so we have</p><disp-formula id="scirp.22664-formula54748"><label>(8)</label><graphic position="anchor" xlink:href="2-2230006\8f47fcae-f0a6-4b16-8744-469aaca420ca.jpg"  xlink:type="simple"/></disp-formula><p>Therefore, the following inequalities hold:</p><p><img src="2-2230006\7578de85-0f21-48f5-a3e6-af27eb749889.jpg" /></p><p><img src="2-2230006\42975605-5371-4318-b700-c4042f5c2052.jpg" /></p><p><img src="2-2230006\a6b89e0d-aa8a-44cf-bc5f-00c1792c504a.jpg" /></p><p><img src="2-2230006\62c894c1-a1d9-4ae6-a5d8-34d747687c82.jpg" /></p><p><img src="2-2230006\83e9443a-e4b1-4204-8801-2d26deff581d.jpg" /></p><p><img src="2-2230006\3ec633cc-7f17-40bb-abe1-2b4759bb9b0d.jpg" /></p><p>We denote that <img src="2-2230006\dded4a1b-e3bd-4e1f-b037-8d74a0c406a3.jpg" /> Then the following inequality holds:</p><p><img src="2-2230006\8330b6f3-1342-4128-b5f1-66a948b046ab.jpg" /></p><p>Furthermore, if<img src="2-2230006\9d4512b8-d947-40cd-ae3c-8efc201742c4.jpg" />, and<img src="2-2230006\1a67e1fe-b12a-4e04-862d-30f3eedd30c0.jpg" />, for some<img src="2-2230006\80ca3990-6eb5-4854-af19-4a92fc4dcf25.jpg" />, then we have</p><disp-formula id="scirp.22664-formula54749"><label>(9)</label><graphic position="anchor" xlink:href="2-2230006\311e610e-da43-4f6b-afe5-51dae8fd9a67.jpg"  xlink:type="simple"/></disp-formula><p>Let<img src="2-2230006\b3b73eeb-00d8-46df-88b2-ea90389340af.jpg" />, <img src="2-2230006\7289bd65-c3a0-433a-bcaf-3d0b353d8c8b.jpg" />and <img src="2-2230006\80429491-10ba-4925-9a8a-4ebd6aa239f8.jpg" /> be the sums of the elements in row i of<img src="2-2230006\8db69178-a388-4cfb-b75b-41c419b64386.jpg" />, <img src="2-2230006\474993f6-5f66-4149-988f-0e4dcdc5d38f.jpg" />, and<img src="2-2230006\c8f301b3-e76c-466b-9f74-0d6bb254d14a.jpg" />, respectively. The following equations hold:</p><disp-formula id="scirp.22664-formula54750"><label>(10)</label><graphic position="anchor" xlink:href="2-2230006\f42c2e6d-e544-4246-afcc-d0678d1d3ada.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="2-2230006\7a003cf1-3f20-426c-adff-98069a3f9aa1.jpg" /> and <img src="2-2230006\64ca6c9e-d227-4364-bd7d-70dcce8883b6.jpg" /> are the sums of the elements in row i of L and U for<img src="2-2230006\0d17985f-7e71-47f7-9f0c-11aa2df76c91.jpg" />, respectively. Since A is a diagonally dominant Z-matrix, by (8) and by the condition (6) the following relations hold:</p><p><img src="2-2230006\49463743-d446-47e6-b91f-2cf457877c96.jpg" /></p><p><img src="2-2230006\08c0246a-9b43-42b5-90a3-00db72040291.jpg" /></p><p><img src="2-2230006\9743a758-41e1-4880-9202-2a3c0e4e2621.jpg" /></p><p>Therefore, <img src="2-2230006\4d7f3f98-6115-4dab-bd87-b3fa73fae6da.jpg" />, <img src="2-2230006\b1b20ddc-11ab-465b-9ff1-31ddf4f5feee.jpg" />, and <img src="2-2230006\ab24a6ae-11dd-413b-8e06-db6aa50af1e3.jpg" /> is a Zmatrix. Moreover, by (9) and by the assumption, we can easily obtain</p><disp-formula id="scirp.22664-formula54751"><label>(11)</label><graphic position="anchor" xlink:href="2-2230006\b23e369f-2f90-4423-96ef-79d605624248.jpg"  xlink:type="simple"/></disp-formula><p>Therefore, <img src="2-2230006\8d9e8c91-4f2d-4cd3-8d1a-421892cb6ebd.jpg" />satisfies the condition of diagonal dominance.</p><p>Lemma 2.4 [10, Lemma 2]. An upper bound on the spectral radius <img src="2-2230006\20914340-f00b-41b9-995c-3d3ccec4ad6a.jpg" /> for the Gauss-Seidel iteration matrix T is given by</p><p><img src="2-2230006\61ae3408-58cc-4fd4-94fe-85729259102c.jpg" /></p><p>where <img src="2-2230006\37fba1df-43aa-4c25-b861-a119e9e204c6.jpg" /> and <img src="2-2230006\551204c7-a988-44dc-a293-8d389172e96f.jpg" /> are the sums of the moduli of the elements in row i of the triangular matrices L and U, respectively.</p><p>Theorem 2.5. Let A be a nonsingular diagonally dominant Z-matrix with unit diagonal elements and let the condition (6) holds, then <img src="2-2230006\36d41b41-bc3a-4329-ae50-bd5fb0403935.jpg" /></p><p>Proof. From (11) and <img src="2-2230006\1b68ce39-e53b-410b-b19e-79b2c0da7024.jpg" /> we have</p><p><img src="2-2230006\49798fb4-0ab5-41b4-84fe-ea667906755c.jpg" /></p><p>This implies that</p><disp-formula id="scirp.22664-formula54752"><label>(12)</label><graphic position="anchor" xlink:href="2-2230006\6798819b-c5c0-497e-9da3-a81bd361d8c7.jpg"  xlink:type="simple"/></disp-formula><p>Hence, by Lemma (2.4) we have <img src="2-2230006\46d77310-ab42-442e-8ac6-0021b53317b4.jpg" /></p><p>Definition 2.6. Let A be an <img src="2-2230006\41d38d1c-91f5-41ca-a7b3-bdbc650250cb.jpg" /> real matrix. Then, <img src="2-2230006\0681b26a-f214-48d7-8d4a-0890f94b44df.jpg" />is referred to as:</p><p>1) a regular splitting, if M is nonsingular, <img src="2-2230006\9b2be23d-a862-4f96-805c-693c8ff61227.jpg" />and <img src="2-2230006\b73c698a-3e61-4e6d-aa47-f3e055a32146.jpg" /></p><p>2) a weak regular splitting, if M is nonsingular, <img src="2-2230006\1a12faaa-a85f-42cd-986b-8ba631cf3ddc.jpg" />and <img src="2-2230006\0026015a-84cf-49e1-bb69-1e0c8cb70edf.jpg" /></p><p>3) a convergent splitting, if <img src="2-2230006\66188c58-f219-4a01-8d75-a819dd3eb4fd.jpg" /></p><p>Lemma 2.7 (Varga, [<xref ref-type="bibr" rid="scirp.22664-ref10">10</xref>]). Let <img src="2-2230006\385d8999-c1b8-4e7e-8819-18231fccd25d.jpg" /> be a nonnegative and irreducible <img src="2-2230006\91834be9-6bbe-4ee3-92b4-9bd3f9b23b4f.jpg" /> matrix. Then 1) A has a positive real eigenvalue equal to its spectral radius<img src="2-2230006\fe20070b-ab38-45a7-9b00-c7ad8b94b1b6.jpg" />;</p><p>2) for<img src="2-2230006\d189dfff-8995-489e-b5bf-a3ba56f63749.jpg" />, there corresponds an eigenvector x &gt; 0;</p><p>3) <img src="2-2230006\43dd01f4-e7ec-4f1e-a921-c3de1137627c.jpg" />is a simple eigenvalue of A;</p><p>4) <img src="2-2230006\a1a109a6-8259-433c-89dc-a1846a09a9da.jpg" />increases whenever any entry of A increases.</p><p>Corollary 2.8 [16, Corollary 3.20]. If <img src="2-2230006\43489d1e-f4b2-41cd-b869-26618d390c6f.jpg" /> is a real, irreducibly diagonally dominant <img src="2-2230006\31e78af9-46d6-4843-af8a-d96d974b5fa0.jpg" /> matrix with <img src="2-2230006\6256203f-aefb-42b5-b042-cbd36595eea9.jpg" /> for all<img src="2-2230006\037f97e4-a426-4a7d-a52c-73df5e4b4160.jpg" />, and <img src="2-2230006\1410dc3d-5a58-494a-8cb3-7ccd02c5c221.jpg" /> for all<img src="2-2230006\80badd5c-3568-4a26-adf9-f6947ff834ab.jpg" />, then<img src="2-2230006\4dfad1a6-7a77-4480-93ee-e9ddb0da8cdb.jpg" />.</p><p>Theorem 2.9 [16, Theorem 3.29]. Let <img src="2-2230006\98e11759-4210-4c57-a945-a9ae7e66b719.jpg" /> be a regular splitting of the matrix A. Then, A is nonsingular with <img src="2-2230006\ce29dc11-1088-455e-ada3-af4d9b0a2551.jpg" /> if and only if<img src="2-2230006\1cd21fa5-0b0a-4b84-afcc-ea44f712b1a8.jpg" />, where</p><p><img src="2-2230006\922a6d16-296c-4e10-8f4c-521481eb7cf4.jpg" /></p><p>Theorem 2.10 (Gunawardena et al. [2, Theorem 2.2]). Let A be a nonnegative matrix. Then 1) If <img src="2-2230006\ffc57fea-8c54-4151-9944-f636dd555406.jpg" /> for some nonnegative vector x, <img src="2-2230006\2b31154f-685d-4922-ad01-df2647025a97.jpg" />then <img src="2-2230006\be820045-cf85-4028-947d-f20ffd6ce8c7.jpg" /></p><p>2) If <img src="2-2230006\275e6b7f-c897-4592-a8f5-4ad72a58ed47.jpg" /> for some positive vector x, then <img src="2-2230006\39ce5ce3-b539-41a7-ab42-b38dfd3f0ac8.jpg" /> Moreover, if A is irreducible and if <img src="2-2230006\56922ca7-d7af-4aea-9178-d7f2db1172e9.jpg" /> for some nonnegative vector x, then <img src="2-2230006\44c3818e-f446-49fa-91d1-d4196887fbd0.jpg" /> and <img src="2-2230006\cd468a21-d301-4729-af66-3d12b75bc41b.jpg" /> is a positive vector.</p><p>Let <img src="2-2230006\6357b236-8ab0-4c1a-b85a-b49f1797675c.jpg" /> be a real Banach space, <img src="2-2230006\4450ab43-d0c7-4b86-9c3d-2103468270ea.jpg" />its dual and <img src="2-2230006\31c3197a-5a5d-4c0a-88fc-0af299b9ef46.jpg" /> the space of all bounded linear operator mapping B into itself. We assume that B is generated by a normal cone K [<xref ref-type="bibr" rid="scirp.22664-ref17">17</xref>]. As is defined in [<xref ref-type="bibr" rid="scirp.22664-ref17">17</xref>], the operator <img src="2-2230006\90adb79d-502c-4585-a6d1-a664c9385923.jpg" /> has the property “d” if its dual <img src="2-2230006\dbc1f851-7551-4057-9a4f-8a916aa9d547.jpg" /> possesses a Frobenius eigenvector in the dual cone <img src="2-2230006\69934046-503a-41bd-b1a7-798eef177cb3.jpg" /> which is defined by</p><p><img src="2-2230006\9148ee86-c513-4535-bde6-943081e9240a.jpg" /></p><p>As is remarked in [1,17], when <img src="2-2230006\6848e3ba-cb26-41e2-ab9f-ba347ad2428f.jpg" /> and<img src="2-2230006\5b9c9c9b-fbc6-44a9-b971-ac5d75803265.jpg" />, all <img src="2-2230006\ef7056f9-e0f6-4fc2-ab7a-b2cbefcb029a.jpg" /> real matrices have the property “d”. Therefore the case are discussing fulfills the property “d”. For the space of all <img src="2-2230006\9dec1123-e289-48e4-b968-f312399ae561.jpg" /> matrices, the theorem of Marek and Szyld can be stated as follows:</p><p>Theorem 2.11 (Marek and Szyld [17, Theorem 3.15]). Let <img src="2-2230006\18ebef5c-3020-4068-aa72-4dce8214d087.jpg" /> and <img src="2-2230006\d4cc0fd0-3f2b-471d-967a-1c765bcee27d.jpg" /> be weak regular splitting with<img src="2-2230006\182d73ea-0297-4e70-b5e2-f5329959b853.jpg" />. Let <img src="2-2230006\ca9487af-535b-4921-87e7-1f5cf2eb64f8.jpg" /> be such that <img src="2-2230006\78edc91a-4b4d-47f3-b995-00b8efe0fb87.jpg" /> and<img src="2-2230006\5361cc71-453c-46a4-b582-904d2c670a77.jpg" />. If <img src="2-2230006\e5d4680c-5819-4c7e-9c8b-1fd13f9ce092.jpg" /> and if either <img src="2-2230006\bf29a690-6e49-4b62-bc61-b033cf3721f1.jpg" />or <img src="2-2230006\de4584a7-0460-4d30-8ba6-e02c6991cc0d.jpg" /> with<img src="2-2230006\661ffcc6-fa57-4b31-9739-7e9de09ac91f.jpg" />, then</p><p><img src="2-2230006\89e872ed-dab0-4f48-8369-02d2f0a51f71.jpg" /></p><p>Moreover, if <img src="2-2230006\272b3f11-831a-48a8-8f9d-6819c8489572.jpg" /> and <img src="2-2230006\65e2b5f5-ab38-464f-a255-dcb504845613.jpg" /> then</p><p><img src="2-2230006\7e86a96a-a7b9-49c7-aefb-de8ab3a015a3.jpg" /></p><p>Now in the following lemma we prove that <img src="2-2230006\b9d2e270-9aff-4bf4-9483-11846ffc575a.jpg" /> is Gauss-Seidel convergent regular splitting.</p><p>Theorem 2.12. Let A be an irreducibly diagonally dominant Z-matrix with unit diagonal, and let the condition (6) holds, then <img src="2-2230006\3f792f89-c916-4ab3-9f70-ceac79199d4c.jpg" /> is Gauss-Seidel convergent regular splitting. Moreover</p><p><img src="2-2230006\e91a20d0-b9f8-4585-8964-c9d6d1c7a305.jpg" /></p><p>Proof. If A is an irreducibly diagonally dominant Zmatrix, then by Lemma (2.3), <img src="2-2230006\874a9e82-2242-4c44-8451-cffd417e0813.jpg" />is a diagonally dominant Z -matrix. So we have<img src="2-2230006\1b4777fb-daf6-47c5-bd84-401781b3acab.jpg" />. By hypothesis we have<img src="2-2230006\bd8c430c-7efe-4966-9676-f029de7b2f32.jpg" />. Thus the strictly lower triangular matrix <img src="2-2230006\47d62fca-ef65-4e70-9063-c187c9c7fdb2.jpg" /> has nonnegative elements. By considering Neumanns series, the following inequality holds:</p><p><img src="2-2230006\68bb15ca-ec44-4a13-acca-a0a4279a689e.jpg" /></p><p>Direct calculation shows that <img src="2-2230006\b08484cb-aedc-43dd-b06c-3cb0eb08046b.jpg" /> holds. Thus, by definition (2.6) <img src="2-2230006\6cf40a34-056c-4963-9714-e4b82728cc9d.jpg" />is the Gauss-Seidel convergent regular splitting. Also in [<xref ref-type="bibr" rid="scirp.22664-ref3">3</xref>] we have <img src="2-2230006\7791d68c-b103-4fa5-b4ea-481cab6798c0.jpg" /> and</p><p><img src="2-2230006\67d73329-b6f1-4bb2-9241-17408faf499e.jpg" /></p><p>Direct comparison of the two matrix elements</p><p><img src="2-2230006\19c844a5-da78-49b2-8a65-1cba2a8455b7.jpg" />and <img src="2-2230006\34d56d3f-4e83-4e67-bd8f-8fe8b534e544.jpg" /> also <img src="2-2230006\86dbfed0-1de3-4770-a790-234dc01cf10f.jpg" /> and</p><p><img src="2-2230006\bb9ef64b-140a-4582-b32a-9e67ad26e4d9.jpg" />we obtain</p><p><img src="2-2230006\43acd39b-fcf7-4c77-b74a-864a46eb06f7.jpg" /></p><p>Thus</p><p><img src="2-2230006\a6ee8ea8-fc9d-4147-a8f5-48c7d641c8fb.jpg" /></p><p>Furthermore, since<img src="2-2230006\83dfd85e-399a-40a7-9cc8-add5a3e36459.jpg" />, we have <img src="2-2230006\8a27ac16-db9e-4543-a740-288226d54429.jpg" />. From Lemma (2.7), x is an eigenvector of <img src="2-2230006\6fe53b9c-cb90-4537-b0d6-7a2727b097b2.jpg" /> , and x is also a Perron vector of<img src="2-2230006\8bf04293-0172-4ad6-a7d8-2d7f2a79c9f6.jpg" />. Therefore, from Theorem (2.11),</p><p><img src="2-2230006\410a0a7e-f973-46bb-9a34-15b4c755fc75.jpg" /></p><p>holds.</p><p>Denote</p><p><img src="2-2230006\1d9b2789-c637-411e-b6e9-7e827468691b.jpg" /></p><p>and also let<img src="2-2230006\d258220d-7ccd-4a77-8593-45628773a91c.jpg" />, <img src="2-2230006\430bfdf2-a5c0-43df-bec3-800b9b86839e.jpg" />, <img src="2-2230006\96dc4753-af20-4183-a6c9-95ba8c641577.jpg" />and <img src="2-2230006\8b8d4aac-afeb-471e-844d-1659501d39a3.jpg" /> be the iterative matrix associated to<img src="2-2230006\87d8f2a8-8825-4659-a624-e484d79d4af6.jpg" />, <img src="2-2230006\a3b5e142-d944-48e1-a1fe-ca8025050c17.jpg" />, <img src="2-2230006\3951bf26-5204-46b9-8cb3-fb14856d87d4.jpg" />and <img src="2-2230006\2ab7cdd3-3d0f-4d18-b36d-f0df367ebd90.jpg" /> respectively. Then we can prove <img src="2-2230006\9035bf8d-93ac-43e9-babf-6a2fc1343538.jpg" /> and<img src="2-2230006\00fc9704-60bf-4a74-acf5-90b988d6bad4.jpg" />, similarly. In summary, we have the following inequalities:</p><p><img src="2-2230006\e3154181-3f8e-48c0-b2a8-0e453e0840db.jpg" /></p><p>Remark 2.13. W. Li, in [<xref ref-type="bibr" rid="scirp.22664-ref18">18</xref>] used the M-matrix instead of irreducible diagonally dominant Z-matrix, therefore we can say that the Lemma 2.3 and the Theorems 2.5 and 2.12 are hold for M-matrices.</p></sec><sec id="s3"><title>3. Numerical Results</title><p>In this section, we test a simple example to compare and contrast the characteristics of the different preconditioners. Consider the matrix</p><p><img src="2-2230006\6f15116a-9efb-4b2c-b029-f4bc42b2f8f5.jpg" /></p><p>Applying the Gauss-Seidel method, we have <img src="2-2230006\fd182c8f-a7c3-4ab3-8105-09dca1b1fd2a.jpg" /> <img src="2-2230006\938ba704-c022-498a-8f00-b97882038156.jpg" />. By using preconditioner <img src="2-2230006\d885f9d9-a527-499f-9f33-461adb4c3863.jpg" /> we find that <img src="2-2230006\24914d34-76c6-47bb-a7be-56299aff6bfa.jpg" /> and <img src="2-2230006\a90d8a48-fcfa-42a7-b7e7-2971b4691a02.jpg" /> have the following forms:</p><p><img src="2-2230006\9a4f91dd-770d-423a-9885-242c696371e9.jpg" /></p><p><img src="2-2230006\6da88322-f79e-4436-a5d4-a72bd68ef28e.jpg" /></p><p>and<img src="2-2230006\e00aa03f-ad1d-48e6-8f68-02e7515ff020.jpg" />.</p><p>Using the preconditioner <img src="2-2230006\ef68e7f1-c276-46f2-bfb1-163473d5ff05.jpg" /> we obtain</p><p><img src="2-2230006\a30ab9c1-c4b4-42e1-aabf-848106712939.jpg" /></p><p><img src="2-2230006\68ffd504-7aab-44dd-b253-d6397429da29.jpg" /></p><p>and<img src="2-2230006\c9e100a9-58fe-4891-ab5e-bc76141dfe65.jpg" />.</p><p>For<img src="2-2230006\2db18911-6f73-45b5-b4d3-41f6e9e6e254.jpg" />, we have</p><p><img src="2-2230006\0d41c62f-ca7a-4b51-8d4e-57b2c9df1d7c.jpg" /></p><p><img src="2-2230006\3e389d09-c53a-46f4-b912-38eba9b498e7.jpg" /></p><p>and<img src="2-2230006\fbf2fd07-87ba-4fe6-9e90-1d9d088452c3.jpg" />.</p><p>For<img src="2-2230006\974757d1-2278-4c35-9d00-6d02965143ea.jpg" />, we have</p><p><img src="2-2230006\ebf7351d-2060-4b75-8460-d4bd01d60a98.jpg" /></p><p><img src="2-2230006\e0a6f7b4-f19b-40c9-b176-7ad6dcf4ffdc.jpg" /></p><p>and<img src="2-2230006\a133fdb8-580e-404c-835e-4e01ef199b85.jpg" />.</p><p>For <img src="2-2230006\32519607-5296-4f6a-a6f3-65f7d174e08e.jpg" /> we have</p><p><img src="2-2230006\1c7e1b51-4d97-4b61-8773-9ee412b53276.jpg" /></p><p><img src="2-2230006\bb9a11b7-a73f-4cb4-954d-a482cbbff8bc.jpg" /></p><p>and <img src="2-2230006\f3f23b91-e180-407f-a037-a534ea1bd23a.jpg" /></p><p>From the above results, we have <img src="2-2230006\a8b613af-149b-419e-b936-9e0049652b18.jpg" />. Then <img src="2-2230006\fe35218b-3cd8-4433-8bfa-6ae7588c0328.jpg" /> and <img src="2-2230006\9f43dcde-f71b-4fea-b2d6-e8ffe816689c.jpg" /> have the forms:</p><p><img src="2-2230006\805e0790-4e79-43d9-ab3e-fea91c1361ad.jpg" /></p><p><img src="2-2230006\ddc19ed2-8c26-478e-9c1c-ea6863500ac5.jpg" /></p><p>and<img src="2-2230006\69fec903-6db7-4c6a-8947-2a7e13cecaa2.jpg" />.</p><p>For<img src="2-2230006\ecf5de32-5193-42ab-b3c1-82cd08e112c4.jpg" />, we have</p><p><img src="2-2230006\c7003e1f-974a-480a-8349-660d9fff4e4d.jpg" /></p><p><img src="2-2230006\15a1f0bd-15b7-4e63-ae19-d740cb2f8fd7.jpg" /></p><p>and <img src="2-2230006\fbe27f3b-d763-49e4-979f-8442cbeffcb0.jpg" /> Since the preconditioned matrices differ only in the values of their last rows, the related matrices also differ only in these values, as is shown in the above results. Thus the elements of new <img src="2-2230006\5a77e851-4ef4-467c-8e6d-be39cb390522.jpg" /> and <img src="2-2230006\626c0164-05f3-4bff-8454-5ce116664a9e.jpg" /> are similar to elements of <img src="2-2230006\ccb3d8d2-adae-4cd5-b196-28a5eec299f2.jpg" /> and<img src="2-2230006\d05db90f-cdda-479b-9f8b-62bcc46b8abc.jpg" />, respectively than the elements of last rows. Therefore, we hereafter show only the last row.</p><p>By putting<img src="2-2230006\31651ed8-f407-4e46-8a7d-c65ab604e77c.jpg" />, the matrices <img src="2-2230006\d3e729d8-da93-44f1-8df5-ceeb5eb1f825.jpg" /><img src="2-2230006\19985e2a-f7cd-4f88-aad0-4e2d1f987be0.jpg" /><img src="2-2230006\1e02b481-8211-4e90-b853-3565f6476449.jpg" /> and <img src="2-2230006\2e020c27-0c01-4d49-babd-fc13d8977f4b.jpg" /> have the following forms:</p><p><img src="2-2230006\29c3cc10-6043-4044-aac6-07d0d238bb9b.jpg" /></p><p>and<img src="2-2230006\93539de1-e9ad-4db6-af9f-22943413bbec.jpg" />,</p><p><img src="2-2230006\a2fbf0b6-5cc5-4efd-8610-4ce8ac5c382d.jpg" /></p><p>and<img src="2-2230006\16691acd-e115-4dac-a7d3-e0dfda65a136.jpg" />.</p><p>For <img src="2-2230006\33c67ab2-afb8-4f1f-8548-3898ba957b62.jpg" /> we have:</p><p><img src="2-2230006\6d92ea43-5cb3-4bb3-ad68-a98b0519cbb3.jpg" /></p><p>and <img src="2-2230006\32da21ed-ab30-4578-8d60-3262c488ee60.jpg" /> and</p><p><img src="2-2230006\1126bf3a-2ed7-44d0-8015-c41ffaaa870c.jpg" /></p><p>and<img src="2-2230006\ba4f7e13-3e57-4957-ac6a-8237a4268070.jpg" />.</p><p>For <img src="2-2230006\caaf58d1-7788-4da0-8251-37d0f94bf33b.jpg" /> we have:</p><p><img src="2-2230006\067f7982-c84c-4bae-b34b-b7a4e709e608.jpg" /></p><p>and <img src="2-2230006\7a09a2ca-e161-4533-8755-68787be019b2.jpg" /> and</p><p><img src="2-2230006\07168711-ecc9-4cce-9524-e97025435863.jpg" /></p><p>and<img src="2-2230006\af574e99-f258-4b13-b68a-7952b51177ee.jpg" />.</p><p>From the numerical results, we see that this method with the preconditioner <img src="2-2230006\59ebd667-3b89-411b-bd3e-46850820d8b8.jpg" /> produces a spectral radius smaller than the recent preconditioners that above was introduced.</p></sec><sec id="s4"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.22664-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">T. 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