<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2012.36094</article-id><article-id pub-id-type="publisher-id">AM-20290</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>
 
 
  Bounds for the Second Largest Eigenvalue of Real 3 &#215; 3 Symmetric Matrices with Entries Symmetric about the Origin
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>arini</surname><given-names>Geoffrey</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>Kivunge</surname><given-names>Benard</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jotham</surname><given-names>Akanga</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Pure and Applied Mathematics, Jomo Kenyatta University of Agriculture and Technology, Nairobi, Kenya</addr-line></aff><aff id="aff2"><addr-line>Department of Pure and Applied Mathematics, Kenya Polytechnic University College, Nairobi, Kenya</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>geoffreyonkundi@yahoo.com(AG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>21</day><month>06</month><year>2012</year></pub-date><volume>03</volume><issue>06</issue><fpage>606</fpage><lpage>609</lpage><history><date date-type="received"><day>April</day>	<month>3,</month>	<year>2012</year></date><date date-type="rev-recd"><day>May</day>	<month>3,</month>	<year>2012</year>	</date><date date-type="accepted"><day>May</day>	<month>10,</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>
 
 
  Let 
  A<sub>S</sub><sub>n</sub>
  <sub>[a,b]</sub> denote a set of all real nxn symmetric matrices with entries in the interval [
  a,
  b]. In this article, we present bounds for the second largest eigenvalue 
  λ
  <sub>2</sub>(
  A) of a real symmetric matrix 
  <b>A</b>, such that 
  A∈
  A<sub>S<sub></sub></sub>
  <sub>3</sub> [-b,b].
 
</p></abstract><kwd-group><kwd>Bounds; Determinant; Eigenvalues; Trace</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Throughout this article, <img src="19-7400795\4032fe16-d710-4739-9f14-1f5711f96be7.jpg" />denotes a set of <img src="19-7400795\b95a46f6-0262-4241-976c-49e67fc0bd18.jpg" /> real symmetric matrices whose entries are in the interval<img src="19-7400795\8619d96f-5e3c-49d3-9ae2-42f7cd45ee09.jpg" />. Eigenvalues of any real <img src="19-7400795\969b867d-c21e-474e-9679-e8fa294dcff6.jpg" /> symmetric matrix A, will be represented by</p><disp-formula id="scirp.20290-formula46907"><label>(1.1)</label><graphic position="anchor" xlink:href="19-7400795\1670c34d-c1af-437a-a3d6-d8ca7a92f63e.jpg"  xlink:type="simple"/></disp-formula><p>The smallest <img src="19-7400795\a547df4b-7b70-49e9-9747-325f4c26570a.jpg" /> and the largest <img src="19-7400795\17031329-6921-4451-a7d4-771b10901808.jpg" /> eigenvalues have been studied extensively in the recent decades. Recently, many researchers have turned attention to the second largest eigenvalue <img src="19-7400795\d1c53e51-d7f5-4935-a58e-5faf14e9f867.jpg" /> due to its applications in science and engineering. For example, thesecond largest eigenvalue governs the rate at which the statistics of the Markov chain converge to equilibrium. Here, we investigate bounds for <img src="19-7400795\d1f356f8-7af0-4994-b28a-bcf1c7d937dd.jpg" /> when entries of A vary in the interval<img src="19-7400795\df8f71ef-df2f-40f2-a674-d3c23844b6bc.jpg" />.</p><p>In 1985, Constantine [<xref ref-type="bibr" rid="scirp.20290-ref1">1</xref>] showed that if<img src="19-7400795\99dbd3cc-4135-4672-be1d-1858dc35f555.jpg" />, then</p><disp-formula id="scirp.20290-formula46908"><label>(1.2)</label><graphic position="anchor" xlink:href="19-7400795\454fcbb4-4ca1-4558-bf8d-83b50a33f2a2.jpg"  xlink:type="simple"/></disp-formula><p>if n is even and odd respectively. Similar results are presented in [<xref ref-type="bibr" rid="scirp.20290-ref2">2</xref>]. In [<xref ref-type="bibr" rid="scirp.20290-ref3">3</xref>], Zhan gave bounds for both the largest eigenvalue <img src="19-7400795\2311fc34-66fb-46fb-b5db-f5f8f2c726b1.jpg" /> and the smallest eigenvalue <img src="19-7400795\ef96cc7e-4487-4958-b729-3248bd23c3a1.jpg" /> when entries of A are in a general interval<img src="19-7400795\a9df4857-ec5c-4398-af36-6522c75d770f.jpg" />. In the same paper [<xref ref-type="bibr" rid="scirp.20290-ref3">3</xref>], Zhan posed the following problem: For a given integer j with<img src="19-7400795\3bd4db89-8232-4e29-8647-900967992f65.jpg" />, find</p><disp-formula id="scirp.20290-formula46909"><label>(1.3)</label><graphic position="anchor" xlink:href="19-7400795\138d03ad-6384-4361-9bf2-59a136f8de85.jpg"  xlink:type="simple"/></disp-formula><p>We are concerned with the case j = 2 when <img src="19-7400795\62d25504-070d-4862-8288-898b9e97e9cf.jpg" />. We employ analytical approach discussed in [<xref ref-type="bibr" rid="scirp.20290-ref4">4</xref>] and the properties</p><disp-formula id="scirp.20290-formula46910"><label>(1.4)</label><graphic position="anchor" xlink:href="19-7400795\05e5a0cf-46eb-4eb6-87b6-d8503a7b8d14.jpg"  xlink:type="simple"/></disp-formula><p>to determine these bounds. The following result will prove useful later. If <img src="19-7400795\53cc6aa7-933d-4f86-b53c-2452d93b9c78.jpg" /> is any real 3 &#215; 3 matrix such that<img src="19-7400795\a76949a1-aa44-4a12-adf7-4e128490add0.jpg" />, then <img src="19-7400795\9c172585-dd49-4bab-a5da-dd70b31438a6.jpg" /> [5,6]. It immediately follows that if<img src="19-7400795\be9a7b21-d0f6-4597-8d17-7fcfd62b5dc4.jpg" />, then</p><disp-formula id="scirp.20290-formula46911"><label>(1.5)</label><graphic position="anchor" xlink:href="19-7400795\984fef37-f54f-4b5e-a2a0-44d43c7ee48a.jpg"  xlink:type="simple"/></disp-formula><p>This paper is organized as follows. In Section 2, analytical method for eigenvalues of real 3 &#215; 3 symmetric matrices is discussed. In Section 3, we derive bounds for<img src="19-7400795\c3ef5650-d5e0-48da-bae5-b521382d4ad6.jpg" />. Finally, a numerical example is given in Section 4.</p></sec><sec id="s2"><title>2. Analytical Calculation of Eigenvalues</title><p>A detailed description of this technique can be found in [<xref ref-type="bibr" rid="scirp.20290-ref4">4</xref>]. Let</p><disp-formula id="scirp.20290-formula46912"><label>(2.1)</label><graphic position="anchor" xlink:href="19-7400795\143ef4ef-df00-4cbb-81f8-549fe688fcc6.jpg"  xlink:type="simple"/></disp-formula><p>be a real 3 &#215; 3 symmetric matrix. Eigenvalues of A can be directly calculated by solving the corresponding characteristic equation</p><disp-formula id="scirp.20290-formula46913"><label>(2.2)</label><graphic position="anchor" xlink:href="19-7400795\eb89946a-6f7e-4467-bc59-5c962289325e.jpg"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.20290-formula46914"><label>(2.3)</label><graphic position="anchor" xlink:href="19-7400795\026ffa25-6e2f-43c5-bb04-d0375ab6e973.jpg"  xlink:type="simple"/></disp-formula><p>Equation (2.2) is then solved by first depressing it, i.e., transforming it to the form</p><disp-formula id="scirp.20290-formula46915"><label>(2.4)</label><graphic position="anchor" xlink:href="19-7400795\82a20996-d5d5-4360-8a76-cc02975e0f1e.jpg"  xlink:type="simple"/></disp-formula><p>with,</p><disp-formula id="scirp.20290-formula46916"><label>(2.5)</label><graphic position="anchor" xlink:href="19-7400795\42064b97-e916-4361-bb34-1d751bb1b53a.jpg"  xlink:type="simple"/></disp-formula><p>Solutions to Equation (2.4) are given by</p><disp-formula id="scirp.20290-formula46917"><label>(2.6)</label><graphic position="anchor" xlink:href="19-7400795\ebcb321e-546b-4e23-bdfd-6d7c49ef03ac.jpg"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.20290-formula46918"><label>(2.7)</label><graphic position="anchor" xlink:href="19-7400795\a41cf2f5-67c2-41cc-84f3-094f46260d89.jpg"  xlink:type="simple"/></disp-formula><p>Finally, eigenvalues of A becomes</p><p><img src="19-7400795\e55c7a59-e396-42e3-b4b9-03c57c88072a.jpg" />, for <img src="19-7400795\563a05ed-1fbd-463c-a5d6-0e0ea23d2f19.jpg" />(2.8)</p></sec><sec id="s3"><title>3. Bounds for the Second Largest Eigenvalue <img src="19-7400795\63687f28-50b0-4d7a-80f0-d45a3ba7c8b0.jpg" /></title><p>Note that<img src="19-7400795\764b5750-4fed-4fb5-964e-f2a1dd300e65.jpg" />, corresponds to the second largest eigenvalue. We therefore determine the values of x<sub>2</sub>, p and c<sub>2</sub> which minimizes or maximizes<img src="19-7400795\2d304895-78b8-4bef-92e8-569fd9ceb04b.jpg" />. However, this is not straight forward since x<sub>2</sub>, p and c<sub>2</sub> depends on the entries of A which vary in the interval<img src="19-7400795\d4de2b62-dbf7-4c6d-99bb-53bfe48b4e8a.jpg" />. We shall heavily rely on minimizing or maximizing<img src="19-7400795\fa172487-41ad-4844-a8b8-607990d47a55.jpg" />.</p><p>For the lower bound we require the largest possible value of p such that x<sub>2</sub> and <img src="19-7400795\1a5c2a30-f309-4ba2-8fc9-119ff7fbbf78.jpg" /> are minimum. Observe that if we put<img src="19-7400795\fb1e3f92-c067-4dbf-b3df-1d20355a7804.jpg" />, then</p><disp-formula id="scirp.20290-formula46919"><label>(3.1)</label><graphic position="anchor" xlink:href="19-7400795\6cc3b308-38ef-477a-b4c5-7c4934e9cd8a.jpg"  xlink:type="simple"/></disp-formula><p>Setting <img src="19-7400795\9f6f6b5e-9ab9-4bdc-9ff8-daef0532a63c.jpg" /> such that</p><disp-formula id="scirp.20290-formula46920"><label>(3.2)</label><graphic position="anchor" xlink:href="19-7400795\fc3a2237-cb63-460a-baaa-386555da96b2.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="19-7400795\df80697d-8ef5-44d5-87e0-42cb7b71f026.jpg" /> with <img src="19-7400795\1e666f29-11a4-4076-8fd6-253319beda0f.jpg" /> we obtain,</p><p><img src="19-7400795\7b3b949b-319c-4fcc-85f2-c5d98f4eff03.jpg" />and<img src="19-7400795\27b931c7-4fd3-41d0-a5a9-35f6044982ed.jpg" />.(3.3)</p><p>Thus<img src="19-7400795\bffb4a86-883d-472d-8a91-103e99f28219.jpg" />, as required. These correspond to the eigenvalues:</p><disp-formula id="scirp.20290-formula46921"><label>(3.4)</label><graphic position="anchor" xlink:href="19-7400795\bf44797b-5fc7-404f-8513-a891eb81675f.jpg"  xlink:type="simple"/></disp-formula><p>Now, suppose there exist <img src="19-7400795\ee905fbf-061f-4e64-8d66-d5630663b958.jpg" /> and <img src="19-7400795\f4e3c2a7-15d0-4b18-b923-3ab2b080ff08.jpg" /> such that</p><disp-formula id="scirp.20290-formula46922"><label>(3.5)</label><graphic position="anchor" xlink:href="19-7400795\679fe21e-1684-4cee-8f57-5d56141c670b.jpg"  xlink:type="simple"/></disp-formula><p>for some real numbers<img src="19-7400795\626dd51a-6cf2-4aa4-8da5-b95a1915a40c.jpg" />. Note that</p><disp-formula id="scirp.20290-formula46923"><label>(3.6)</label><graphic position="anchor" xlink:href="19-7400795\91cd31e9-3504-4c1a-8e00-708daf1c0b7a.jpg"  xlink:type="simple"/></disp-formula><p>Therefore we must have<img src="19-7400795\8a45fd5f-eedf-4ca6-9138-a13ba83c06a2.jpg" />. However, this is impossible since from (1.5) we have</p><disp-formula id="scirp.20290-formula46924"><label>(3.7)</label><graphic position="anchor" xlink:href="19-7400795\dd6ad664-1c25-4fac-a56d-127746ff8971.jpg"  xlink:type="simple"/></disp-formula><p>We thus deduce that<img src="19-7400795\7e92486b-458b-47db-8cd1-b1e1b5a37663.jpg" />. Equality is attained by the following matrices:</p><disp-formula id="scirp.20290-formula46925"><label>(3.8)</label><graphic position="anchor" xlink:href="19-7400795\09721634-03f2-4e34-ac0e-91d2c990d3b7.jpg"  xlink:type="simple"/></disp-formula><p>Similarly, for the upper bound, we require the largest possible value of p such that x<sub>2</sub> and <img src="19-7400795\7f9de960-213b-42b1-bf8e-27a5b07d6f4c.jpg" /> are maximum. Note that setting <img src="19-7400795\bef0ca6d-1999-4f17-b998-4019847a00c0.jpg" /> yields</p><disp-formula id="scirp.20290-formula46926"><label>(3.9)</label><graphic position="anchor" xlink:href="19-7400795\cf3f0ceb-7d78-42cd-9fd4-6c39220e3646.jpg"  xlink:type="simple"/></disp-formula><p>Now, if we put <img src="19-7400795\f021bc1f-f359-44b6-9ab7-bf10f11036f8.jpg" /> such that</p><disp-formula id="scirp.20290-formula46927"><label>(3.10)</label><graphic position="anchor" xlink:href="19-7400795\4aebe89e-7dd4-4c0d-a755-cca903956e0c.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="19-7400795\2fc5019b-b6cf-43e6-ba35-3948aaf3b78c.jpg" /> with <img src="19-7400795\8ae3eaef-1ac6-447a-abfe-1cb05ab73aaf.jpg" /> we have,</p><p><img src="19-7400795\92202c3a-ba30-480e-9875-9f5957c8fa3d.jpg" />and<img src="19-7400795\03ecf38a-f87e-4bb6-9991-af2adfcad7b4.jpg" />.</p><p>Check that</p><p><img src="19-7400795\6c634865-7ef5-4b5a-9d7b-27bbfc35dc10.jpg" />60˚</p><p>and hence<img src="19-7400795\2fbb2248-1a7b-4fe6-b963-ad9aa8736f04.jpg" />, corresponding to the eigenvalues:</p><disp-formula id="scirp.20290-formula46928"><label>(3.13)</label><graphic position="anchor" xlink:href="19-7400795\6f326932-6f39-4b17-b62b-20337b32215e.jpg"  xlink:type="simple"/></disp-formula><p>Again, assume there exist <img src="19-7400795\640ab5cb-e865-4613-977f-ab45dcdf2cd5.jpg" /> and <img src="19-7400795\dc127872-cc1a-4589-af82-6295a5b04dfa.jpg" /> such that</p><disp-formula id="scirp.20290-formula46929"><label>(3.14)</label><graphic position="anchor" xlink:href="19-7400795\6e17a960-6c0c-4606-bc68-809fbbb92bd0.jpg"  xlink:type="simple"/></disp-formula><p>for some real numbers<img src="19-7400795\1ee2f7bc-2131-4437-9797-2c7bdaf573f5.jpg" />. Considering the fact&#160;</p><disp-formula id="scirp.20290-formula46930"><label>(3.15)</label><graphic position="anchor" xlink:href="19-7400795\f8114942-d8d1-4065-adb8-e2c7b03c7971.jpg"  xlink:type="simple"/></disp-formula><p>we necessarily have<img src="19-7400795\69b02e87-6907-47e8-ada1-93f9d3dc306b.jpg" />. Again from (1.5) we obtain&#160;</p><disp-formula id="scirp.20290-formula46931"><label>(3.16)</label><graphic position="anchor" xlink:href="19-7400795\61d33d0e-16d3-41f5-be2a-6e3aabfa5218.jpg"  xlink:type="simple"/></disp-formula><p>This is a contradiction and hence we conclude that<img src="19-7400795\34c76c78-022b-4e0f-8baa-f7f03bb072ce.jpg" />. Equality is attained by the following matrices:</p><disp-formula id="scirp.20290-formula46932"><label>(3.17)</label><graphic position="anchor" xlink:href="19-7400795\ed22adc2-1a6e-4fb6-abe3-31bbde2f6b03.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Numerical Example</title><p>Let<img src="19-7400795\3800dca2-ddf3-44fa-bd00-f65508c79d13.jpg" />. We first consider the lower bound for<img src="19-7400795\f5b0dc95-2e94-4e22-8a76-2d52429093a7.jpg" />. According to Equation (2.8), we require<img src="19-7400795\609ec45c-f33d-415f-a270-c352490e6671.jpg" />, so that</p><disp-formula id="scirp.20290-formula46933"><label>(4.1)</label><graphic position="anchor" xlink:href="19-7400795\e4332c8d-fd29-4ac5-ac83-e09fe87310c2.jpg"  xlink:type="simple"/></disp-formula><p>Substituting (4.1) into (2.5) yields</p><disp-formula id="scirp.20290-formula46934"><label>(4.2)</label><graphic position="anchor" xlink:href="19-7400795\d043ff85-923d-4b83-a4c3-f820478857ed.jpg"  xlink:type="simple"/></disp-formula><p>Now, p is maximum when<img src="19-7400795\a4b23fc8-4392-41a9-874a-da9b833267ca.jpg" />. However, by noting that<img src="19-7400795\e4fffa90-d6a2-4c59-ba9c-155cd0482709.jpg" />, we require<img src="19-7400795\4130e57d-3103-4da0-a0a5-c038529838bd.jpg" />. Thus we must have<img src="19-7400795\f2d39df9-eaf8-4fea-a13c-ebeca6ad0fbb.jpg" />, with<img src="19-7400795\fe20949c-af98-41e9-b47b-195fdc8edb65.jpg" />. Finally, from (2.6), (2.7) and (4.2), we easily have<img src="19-7400795\5af6edae-5bb1-43a6-8be8-9bbf2b9caac4.jpg" />, corresponding to the eigenvalues<img src="19-7400795\82ef569c-6539-403c-91d9-ddf8111268f4.jpg" />. We now let <img src="19-7400795\9c39fb78-47ef-4d74-a4d3-0c30d1935a8f.jpg" /> and <img src="19-7400795\438d72e0-582e-4467-b5a5-3572cb13b9cd.jpg" /> be eigenvalues such that <img src="19-7400795\44fa4745-157e-42db-ace4-b2da17eeb155.jpg" />for some real numbers<img src="19-7400795\1a85671b-94eb-4fd5-b5e9-39ce3ba1506f.jpg" />. It immediately implies that</p><disp-formula id="scirp.20290-formula46935"><label>(4.3)</label><graphic position="anchor" xlink:href="19-7400795\cf922d05-3c3b-4fa5-b0e9-e2a10a197d75.jpg"  xlink:type="simple"/></disp-formula><p>However, (4.3) is valid only if<img src="19-7400795\8336471b-42af-4e91-83ad-6332763fbb7c.jpg" />. Applying (1.4) results in</p><p><img src="19-7400795\843e0f29-a4e1-44c1-b62a-9033de5c2b61.jpg" /></p><p>Note that</p><p><img src="19-7400795\ce26e017-171a-42cf-8965-8f7d9bc44a51.jpg" /></p><p>where <img src="19-7400795\74e7d6f6-a14d-4ce0-a55b-979ac6f4ffeb.jpg" /> is the maximum determinant of a real 3 &#215; 3 matrix whose entries are in a unit closed disc. Thus<img src="19-7400795\1d58391b-c55e-4612-ac99-477e83984dfe.jpg" />. The minimizing matrices readily follow from (3.8). For the upper bound we set <img src="19-7400795\9f9d12c1-dbf2-4d82-8ef4-1da61ae4278d.jpg" /> 2.3, giving</p><disp-formula id="scirp.20290-formula46936"><label>(4.4)</label><graphic position="anchor" xlink:href="19-7400795\c68cfb38-cf3d-400f-8ccc-962489744c3c.jpg"  xlink:type="simple"/></disp-formula><p>Substituting (4.4) into (2.5) results in</p><disp-formula id="scirp.20290-formula46937"><label>(4.5)</label><graphic position="anchor" xlink:href="19-7400795\ee6481a5-93e7-4dc0-8512-62bcd933f99b.jpg"  xlink:type="simple"/></disp-formula><p>It is easy to check that if<img src="19-7400795\a5837fcb-129e-429d-ae47-32b0ddceb57e.jpg" />, such that<img src="19-7400795\6f356661-0ea3-4148-b91a-7b9d1d152a60.jpg" />, then<img src="19-7400795\8645aef4-6059-4e89-8742-1959cdb2ee4a.jpg" />. This correspond to the eigenvalues<img src="19-7400795\0db9af37-7ddf-4bf9-b1f5-2566308ae146.jpg" />. Similarly if we let <img src="19-7400795\15dceeb9-edf6-4242-b716-f6f3ae88d848.jpg" /> and <img src="19-7400795\0f809787-3066-4f62-8950-84f90a6853f7.jpg" /> such that</p><p><img src="19-7400795\5d851819-3ef3-43c0-92f3-fad3bf844bfe.jpg" />then</p><disp-formula id="scirp.20290-formula46938"><label>(4.6)</label><graphic position="anchor" xlink:href="19-7400795\72d3194d-0645-434d-8ab8-139d529cb52d.jpg"  xlink:type="simple"/></disp-formula><p>Check that (4.6) holds only if<img src="19-7400795\59d6ae21-0746-4292-84eb-0797d63f8470.jpg" />. However,</p><p><img src="19-7400795\7fcc06c1-5567-4d3e-ac2d-bfd73e58b0d0.jpg" /></p><p>Thus <img src="19-7400795\8894b587-e628-4738-aa03-dfd5e7adab7c.jpg" /> and the maximizing matrices follow from (3.17).</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>Thanks are due to the late Professor Cecilia Mwathi for her support during the initial stages of this research.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.20290-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G. Constantine, “Lower Bounds for the Spectra of Symmetric Matrices with Nonnegative Entries,” Linear Algebra and its Applications, Vol. 65, 1985, pp. 171-178. 
doi:10.1016/0024-3795(85)90095-3</mixed-citation></ref><ref id="scirp.20290-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">R. Roth, “On the Eigenvectors Belonging to the Minimum Eigenvalue of an Essentially Nonnegative Symmetric Matrix with Bipartite Graph,” Linear Algebra and Its Applications, Vol. 118, 1989, pp. 1-10.  
doi:10.1016/0024-3795(89)90569-7.</mixed-citation></ref><ref id="scirp.20290-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">X. Zhan, “Extremal Eigenvalues of Real Symmetric Matrices with Entries in an Interval,” Siam Journal of Matrix Analysis and Applications, Vol. 27, No. 3, 2006, pp. 851-860. doi:10.1137/050627812</mixed-citation></ref><ref id="scirp.20290-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">J. Kopp, “Efficient Numerical Diagonalization of 3 × 3 Hermitian Matrices,” International Journal of Modern Physics C, Vol. 19, No. 3, 2008, pp. 523-548.  
doi:10.1142/S0129183108012303</mixed-citation></ref><ref id="scirp.20290-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">J. Brenner, “Hadamard Maximum Determinant Problem,” The American Mathematical Monthly, Vol. 79, No. 6, 1972, pp. 626-630.</mixed-citation></ref><ref id="scirp.20290-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">N. J. A Sloan and P. Simon, “The Encyclopaedia of Integer Sequences,” Academic Press Inc., London, 1995.</mixed-citation></ref></ref-list></back></article>