<?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.2012.39157</article-id><article-id pub-id-type="publisher-id">AM-23015</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>
 
 
  Explicit Inversion for Two Brownian-Type Matrices
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>lorendia</surname><given-names>Valvi</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>Vassilis</surname><given-names>Geroyannis</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, University of Patras, Patras, Greece</addr-line></aff><aff id="aff2"><addr-line>Department of Physics, University of Patras, Patras, Greece</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>fvalvi@upatras.gr(LV)</email>;<email>vgeroyan@upatras.gr(VG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>27</day><month>09</month><year>2012</year></pub-date><volume>03</volume><issue>09</issue><fpage>1068</fpage><lpage>1073</lpage><history><date date-type="received"><day>June</day>	<month>22,</month>	<year>2012</year></date><date date-type="rev-recd"><day>August</day>	<month>13,</month>	<year>2012</year>	</date><date date-type="accepted"><day>August</day>	<month>20,</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>
 
 
  We present explicit inverses of two Brownian-type matrices, which are defined as Hadamard products of certain already known matrices. The matrices under consideration are defined by 3n - 1 parameters and their lower Hessenberg form inverses are expressed analytically in terms of these parameters. Such matrices are useful in the theory of digital signal processing and in testing matrix inversion algorithms.
 
</p></abstract><kwd-group><kwd>Brownian Matrix; Hadamard Product; Hessenberg Matrix; Numerical Complexity; Test Matrix</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Brownian matrices are frequently involved in problems concerning “digital signal processing”. In particular, Brownian motion is one of the most common linear models used for representing nonstationary signals. The covariance matrix of a discrete-time Brownian motion has, in turn, a very characteristic structure, the so-called “Brownian matrix”.</p><p>In [<xref ref-type="bibr" rid="scirp.23015-ref1">1</xref>] (Equation (2)) the explicit inverse of a class of matrices <img src="16-7400911\5a6218a7-9f09-4dae-b38a-bf41184b4c32.jpg" /> with elements</p><disp-formula id="scirp.23015-formula40765"><label>(1)</label><graphic position="anchor" xlink:href="16-7400911\d14dc637-001f-43b9-ab80-11bb8a3d95f2.jpg"  xlink:type="simple"/></disp-formula><p>is given. On the other hand, the analytic expressions of the inverses of two symmetric matrices <img src="16-7400911\5a77413f-58a9-4822-85a1-60bcdd249588.jpg" /> and<img src="16-7400911\2e77f36f-ca2a-449e-ae1b-ed4055f29e04.jpg" />, where</p><disp-formula id="scirp.23015-formula40766"><label>(2)</label><graphic position="anchor" xlink:href="16-7400911\523f3cdc-0b95-447f-8356-0c31979d8335.jpg"  xlink:type="simple"/></disp-formula><p>respectively, are presented in [<xref ref-type="bibr" rid="scirp.23015-ref2">2</xref>] (first equation in p. 113, and Equation (1), respectively). The matrix K is a special case of Brownian matrix and <img src="16-7400911\3b1e3319-2033-46cc-bc96-6074c2c43516.jpg" /> is a lower Brownian matrix, as they have been defined in [<xref ref-type="bibr" rid="scirp.23015-ref3">3</xref>] (Equation (2.1)). Earlier, in [<xref ref-type="bibr" rid="scirp.23015-ref4">4</xref>] (paragraph following Equation (3.3)) the term “pure Brownian matrix” for the type of the matrix K has introduced. Furthermore, in [<xref ref-type="bibr" rid="scirp.23015-ref5">5</xref>] (discussion concerning Equations (28)-(30)) the so-called “diagonal innovation matrices” (DIM) have been treated, special cases of which are the matrices K and N.</p><p>In the present paper, we consider two matrices A<sub>1</sub> and A<sub>2</sub> defined by</p><disp-formula id="scirp.23015-formula40767"><label>(3)</label><graphic position="anchor" xlink:href="16-7400911\fab8c976-1ef2-4d12-8654-1460ee303ab0.jpg"  xlink:type="simple"/></disp-formula><p>where the symbol <img src="16-7400911\ec40df39-5a4b-4098-b7fa-84c8ebc76b40.jpg" /> denotes the Hadamard product. Hence, the matrices have the forms</p><disp-formula id="scirp.23015-formula40768"><label>(4)</label><graphic position="anchor" xlink:href="16-7400911\972a4498-9fef-4d69-bb23-0e6fd2f5aac5.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.23015-formula40769"><label>(5)</label><graphic position="anchor" xlink:href="16-7400911\4154294a-d9aa-408f-a398-63ed451436e7.jpg"  xlink:type="simple"/></disp-formula><p>Let us now define for a matrix <img src="16-7400911\8b84390a-f26b-47ee-aa8a-7cc4b7602b4c.jpg" /> the terms “pure upper Brownian matrix” and “pure lower Brownian matrix”, for the elements of which the following relations are respectively valid</p><disp-formula id="scirp.23015-formula40770"><label>(6)</label><graphic position="anchor" xlink:href="16-7400911\d5596371-8712-42c7-bee7-52af16f98882.jpg"  xlink:type="simple"/></disp-formula><p>The matrix A<sub>1</sub> (Equation (4)) is a lower Brownian matrix. Furthermore, the matrix PNP, where <img src="16-7400911\f52263be-dcc1-4612-a1d4-ebafab6465bb.jpg" /> is the permutation matrix with elements</p><disp-formula id="scirp.23015-formula40771"><label>(7)</label><graphic position="anchor" xlink:href="16-7400911\6193c863-9e90-499f-b976-15cfe4269b68.jpg"  xlink:type="simple"/></disp-formula><p>is a pure Brownian matrix and <img src="16-7400911\f2cbc4be-adee-43c2-a68a-049993defe0c.jpg" /> a pure lower Brownian matrix. Hence, their Hadamard product <img src="16-7400911\d004a82d-06db-49fb-a794-5c63bcc902ea.jpg" /> gives a pure lower Brownian matrix, that is, the matrix<img src="16-7400911\6b4bfc39-dd5e-4ac1-b437-56a2e1ac0925.jpg" />.</p><p>In the following sections, we deduce in analytic form the inverses and determinants of the matrices A<sub>1</sub> and A<sub>2</sub>; and we study the numerical complexity on evaluating <img src="16-7400911\5201b7ac-86c3-4508-9f0a-f74f1f7755a1.jpg" /> and<img src="16-7400911\50da48ac-a45c-41be-9cdc-feb4f697dfb2.jpg" />.</p></sec><sec id="s2"><title>2. The Inverse and Determinant of A<sub>1</sub></title><p>The inverse of A<sub>1</sub> is a lower Hessenberg matrix expressed analytically by the 3n − 1 parameters defining A<sub>1</sub>. In particular, the inverse <img src="16-7400911\4b7afe3b-4193-49d8-8afc-1f520d907cec.jpg" /> has elements given by the relations</p><disp-formula id="scirp.23015-formula40772"><label>(8)</label><graphic position="anchor" xlink:href="16-7400911\5b7e32a3-881c-4dfb-b45c-4d9bc0c18fb3.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.23015-formula40773"><label>(9)</label><graphic position="anchor" xlink:href="16-7400911\88932940-e0b9-4a67-8f0a-bfb7ac763f56.jpg"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.23015-formula40774"><label>(10)</label><graphic position="anchor" xlink:href="16-7400911\dec68098-8d58-4289-b786-6aa74a9da15b.jpg"  xlink:type="simple"/></disp-formula><p>and with the obvious assumptions</p><disp-formula id="scirp.23015-formula40775"><label>(11)</label><graphic position="anchor" xlink:href="16-7400911\466117b1-7878-4df0-b3ca-1b923ccdc1bd.jpg"  xlink:type="simple"/></disp-formula><p>To prove that the relations (8)-(10) give the inverse matrix<img src="16-7400911\fcbb2f84-9931-4b47-a007-0e290fb782de.jpg" />, we reduce A<sub>1</sub> to the identity matrix I by applying a number of elementary row transformations.</p><p>Then the product of the corresponding elementary matrices gives the inverse matrix of A<sub>1</sub>. These transformations are defined by the following sequence of row operations.</p><p>Operation 1 (applied on A<sub>1</sub> and on the identity matrix I):</p><p><img src="16-7400911\62ab13a7-b70f-4ed1-bc1a-644885aeaea1.jpg" /></p><p>which transforms A<sub>1</sub> into the lower triangular matrix C<sub>1</sub> given by</p><p><img src="16-7400911\2e1e612f-a22a-42fb-acb3-39f7546db4e9.jpg" /></p><p>and the identity matrix I into the upper bidiagonal matrix F<sub>1</sub> with main diagonal</p><p><img src="16-7400911\7356e6dd-cc27-4b99-9887-15bf57973377.jpg" /></p><p>and upper first diagonal</p><p><img src="16-7400911\461042bb-6b7a-4094-befc-5ecc498ced1c.jpg" /></p><p>Operation 2 (applied on <img src="16-7400911\73d027eb-ec97-4d4b-81ee-66fcdff5c3eb.jpg" /> and<img src="16-7400911\f19092fe-7969-4132-9b72-9ad7e0b3caf6.jpg" />):</p><p><img src="16-7400911\cd50a412-ede4-4c6b-b2c6-a36013c5917d.jpg" /></p><p>which derives a lower bidiagonal matrix <img src="16-7400911\c022ffd4-274c-4cc9-b933-1dba97c7cf7c.jpg" /> with main diagonal</p><p><img src="16-7400911\3601433f-a294-4497-912d-19b5aa1251ea.jpg" /></p><p>and lower first diagonal</p><p><img src="16-7400911\3c4a1ae4-3e08-4533-bfb4-93ad39958e09.jpg" /></p><p>while the matrix <img src="16-7400911\60a9be49-9d75-4394-8b0d-31d6041a5845.jpg" /> is transformed into the tridiagonal matrix <img src="16-7400911\e0afb429-33ef-4af4-96e2-d4819b5b1276.jpg" /> given by</p><p><img src="16-7400911\091a706d-ada4-4a21-8311-4671f7c4acf2.jpg" /></p><p>Operation 3 (applied on <img src="16-7400911\da8fda3c-fc37-46b1-b8c9-e17b0d45c5a4.jpg" /> and<img src="16-7400911\85cda84d-6fcf-4904-899a-99b950524177.jpg" />):</p><p><img src="16-7400911\6a8f606e-8ab6-4612-b8ce-17c2534869f4.jpg" /></p><p>which derives the diagonal matrix</p><p><img src="16-7400911\9aaf0dbf-c8ae-428e-a94d-536e29e31df0.jpg" /></p><p>and, respectively, the lower Hessenberg matrix F<sub>3</sub> given by</p><p><img src="16-7400911\e4f62458-5246-4e66-ae86-f463c5f07008.jpg" /></p><p>with the symbol s standing for the quantity<img src="16-7400911\d45ddc54-b270-47b4-9ea6-9a89a952f104.jpg" />.</p><p>Operation 4 (applied on <img src="16-7400911\d8b665a8-92d2-4b15-a01a-ac5da89f8551.jpg" /> and<img src="16-7400911\5540b67b-327d-4658-894e-00bf2d01b3e6.jpg" />):</p><p><img src="16-7400911\598cfbc3-90c9-42ed-a44c-c921b5d32610.jpg" /></p><p>which transforms <img src="16-7400911\e8a743cc-f4f7-4fc2-8053-a80922edac8f.jpg" /> into the identity matrix I and the matrix <img src="16-7400911\97238210-62b9-473a-8f7a-7b03715b7786.jpg" /> into the inverse<img src="16-7400911\e982eefb-54ab-47a3-8a79-a680dbeb58c9.jpg" />.</p><p>The determinant of <img src="16-7400911\8e810bf3-5178-4061-aa9e-8fedc6a7db53.jpg" /> takes the form</p><disp-formula id="scirp.23015-formula40776"><label>(12)</label><graphic position="anchor" xlink:href="16-7400911\638acf0b-c7d3-4ba2-b879-c8e3bb02f584.jpg"  xlink:type="simple"/></disp-formula><p>Evidently, <img src="16-7400911\fd953e93-eb98-4c9a-9c68-e69a2b5b8f06.jpg" />is singular if <img src="16-7400911\89b6d41b-b554-4f8e-9a27-bab2eb127388.jpg" /> or, considering the relation (9), if <img src="16-7400911\4d06598d-532e-462a-a92e-6532f3e9ba51.jpg" /> for some<img src="16-7400911\77553a57-5fb0-42d5-acf2-e899d63b4d3a.jpg" />.</p></sec><sec id="s3"><title>3. The Inverse and Determinant of A<sub>2</sub></title><p>In the case of<img src="16-7400911\2fb156b7-b537-45d4-a97d-d5f25a76321b.jpg" />, its inverse <img src="16-7400911\7e580061-573b-4613-9e93-e3a9d57fb489.jpg" /> is a lower Hessenberg matrix with elements given by the relations</p><disp-formula id="scirp.23015-formula40777"><label>(13)</label><graphic position="anchor" xlink:href="16-7400911\6e93a019-36dc-45eb-9363-e87949a43f28.jpg"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.23015-formula40778"><label>(14)</label><graphic position="anchor" xlink:href="16-7400911\285dc019-0655-4065-a9f1-c962af59a64b.jpg"  xlink:type="simple"/></disp-formula><p>with</p><disp-formula id="scirp.23015-formula40779"><label>(15)</label><graphic position="anchor" xlink:href="16-7400911\40edff7c-332c-4c8b-ab0a-5dfb143b4cb6.jpg"  xlink:type="simple"/></disp-formula><p>and with the obvious assumptions</p><disp-formula id="scirp.23015-formula40780"><label>(16)</label><graphic position="anchor" xlink:href="16-7400911\7b1fd009-c79c-4618-a67c-ce96b0f8d298.jpg"  xlink:type="simple"/></disp-formula><p>In order to prove that the relations (13)-(15) give the inverse matrix<img src="16-7400911\94263f29-9e27-47e1-9154-a2754bb1cba1.jpg" />, we follow a similar manner to that of Section 2.</p><p>Operation 1 (applied on A<sub>2</sub> and on the identity matrix I):</p><p><img src="16-7400911\79d004b5-687b-4040-9051-c55252b8607d.jpg" /></p><p>which transforms A<sub>2</sub> into the lower triangular matrix <img src="16-7400911\d4b9a0bf-0c79-49e7-bbbd-a2c927ed6553.jpg" /> equal to</p><p><img src="16-7400911\8219177e-1bcf-44ff-90b0-f6bc7d35053f.jpg" /></p><p>and the identity matrix I into the bidiagonal matrix <img src="16-7400911\304a911d-98dc-4d97-89c0-9ba7781bacd1.jpg" /> with main diagonal</p><p><img src="16-7400911\47a0b236-c06c-4f41-9e10-97936a14f65f.jpg" /></p><p>and upper first diagonal</p><p><img src="16-7400911\bdec5391-997a-42cf-9423-7bd9d518db7f.jpg" /></p><p>Operation 2 (applied on <img src="16-7400911\c8c220ce-bb0d-46e2-adb2-e4f7b3f13672.jpg" /> and<img src="16-7400911\8bb557b7-f23a-428e-acdf-0c2cf7821b24.jpg" />):</p><p><img src="16-7400911\f5a68aa7-b7ac-4d20-8d69-bf23d6933fe1.jpg" /></p><p>which derives the lower bidiagonal matrix D<sub>2</sub> with main diagonal</p><p><img src="16-7400911\6589da8d-e119-4e57-a530-16b103877b4d.jpg" /></p><p>and lower first diagonal</p><p><img src="16-7400911\eaf9f765-5144-4836-a3ee-6bc40080a4a8.jpg" /></p><p>while the matrix <img src="16-7400911\a6d5a87f-6a40-45ad-9430-5d052bcb4580.jpg" /> is transformed into the tridiagonal matrix <img src="16-7400911\51e0c915-5c5a-444a-9fd5-3747266adc9c.jpg" /> with main diagonal</p><p><img src="16-7400911\5d6f6c3c-be15-4c28-a38f-aeb03c82032d.jpg" /></p><p>upper first diagonal</p><p><img src="16-7400911\4ce7e7ee-b923-4ce7-8eed-bc0f331d6ca9.jpg" /></p><p>and lower first diagonal</p><p><img src="16-7400911\4313843a-ffed-4ff0-9829-46e4d737029a.jpg" /></p><p>Operation 3 (applied on <img src="16-7400911\ea366622-5ea5-4ece-9606-4f74623898a2.jpg" /> and<img src="16-7400911\66e92b6c-af0a-4fe2-828a-065fd310b1c9.jpg" />):</p><p><img src="16-7400911\c879d4ff-b588-4721-b9d2-e2893546e44f.jpg" /></p><p>with<img src="16-7400911\249dc036-f225-449a-aea8-9e62666fd0ab.jpg" />, which yields the diagonal matrix<img src="16-7400911\a9958366-b210-456f-940d-514eebd487af.jpg" />,</p><p><img src="16-7400911\02144315-c979-4d60-b4b4-221224fb8bae.jpg" /></p><p>and the lower Hessenberg matrix <img src="16-7400911\86308f7f-4df6-4d2a-8b1e-b555540c172d.jpg" /> equal to</p><p><img src="16-7400911\be57687c-bdcd-4b78-9f91-e2c21afb56a5.jpg" /></p><p>where the symbol <img src="16-7400911\20c9cad2-8390-475c-8fe4-7dfd8f7fbee1.jpg" /> stands for<img src="16-7400911\c1d8c92a-ebf1-46f4-8d35-20238fc92a6e.jpg" />.</p><p>Operation 4 (applied on <img src="16-7400911\e3a0911e-0943-4c9e-b91d-8f65a18910b2.jpg" /> and<img src="16-7400911\251cccd4-5d5e-417f-bedd-58d69c80bf59.jpg" />):</p><p><img src="16-7400911\e28742ec-2a20-4674-9bb4-30fdfb43394d.jpg" /></p><p>which transforms <img src="16-7400911\0b956f1d-fb24-4733-b90f-29517b6910ac.jpg" /> into the identity matrix I and <img src="16-7400911\1ce58a1f-5b1c-4e7f-96ea-f8c825618855.jpg" /> into the inverse<img src="16-7400911\5a12f505-cbf3-4212-831c-4f0b93a4d16c.jpg" />.</p><p>The determinant of <img src="16-7400911\ea7d73b4-f083-411b-ad91-8b04951e3fdf.jpg" /> has the form</p><disp-formula id="scirp.23015-formula40781"><label>(17)</label><graphic position="anchor" xlink:href="16-7400911\5d785332-dc11-46db-bc65-7b549a108215.jpg"  xlink:type="simple"/></disp-formula><p>which shows in turn that the matrix <img src="16-7400911\8d3172ac-8f50-47ab-8f1b-f71c07abb9d0.jpg" /> is singular if<img src="16-7400911\2a7d438d-99ff-4215-9f29-0df7570dfa52.jpg" />, or, adopting the conventions (14), if <img src="16-7400911\882c8f01-0ac4-4509-8f0b-223b2e8d37c1.jpg" /> for some<img src="16-7400911\aed672bc-67c6-45cf-84db-c9b4fca3967f.jpg" />.</p></sec><sec id="s4"><title>4. Numerical Complexity</title><p>The relations (8) and (13) lead to recurrence formulae, by which the inverses <img src="16-7400911\bea89ebd-705c-41ab-9254-5235130502ac.jpg" /> and<img src="16-7400911\6a239c82-e1e2-469e-9eb2-9dae425c746b.jpg" />, respectively, are computed in <img src="16-7400911\2c539542-bfa4-4599-9dfb-edb7d59d85b5.jpg" /> multiplications/divisions and <img src="16-7400911\319d7854-08dc-46b2-a1b8-920125ac1b57.jpg" /> additions/substractions. In fact, the recursive algorithm</p><disp-formula id="scirp.23015-formula40782"><label>(18)</label><graphic position="anchor" xlink:href="16-7400911\c192a6da-e320-4c9a-9e90-4d4db11bbe9c.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.23015-formula40783"><label>(19)</label><graphic position="anchor" xlink:href="16-7400911\bec02d81-9304-44b1-861d-252fdd9de69b.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.23015-formula40784"><label>(20)</label><graphic position="anchor" xlink:href="16-7400911\40aebb0f-d434-41e2-9e1c-1a404e6e81d1.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.23015-formula40785"><label>(21)</label><graphic position="anchor" xlink:href="16-7400911\3b80d668-5e17-4158-89a2-378e213dfeef.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="16-7400911\456b2eea-0405-44a5-8e4f-f9456541d200.jpg" />, <img src="16-7400911\37ad819d-ee73-4446-aff2-f631436d07c8.jpg" />, <img src="16-7400911\8ab2ac4e-0c79-4287-9857-aac18abf8d62.jpg" />, and <img src="16-7400911\3abf919b-bbce-403d-b589-4fafdbc7ae1b.jpg" /> are given by the relation (9), computes <img src="16-7400911\71d5d3a3-6de8-4bd0-a53f-bc69aa4311b6.jpg" /> in <img src="16-7400911\a6eaa10f-7f7a-4b39-a149-afb320d27bc0.jpg" /> mult/div (since the coefficients of <img src="16-7400911\b53dbf3f-ca5e-4337-a7a4-98f2433a4837.jpg" /> depends only on the second subscript) and <img src="16-7400911\fe99fba6-940f-44ee-9237-78d099c4eb5a.jpg" /> add/sub.</p><p>In terms of<img src="16-7400911\82208fa9-65fd-47dc-8764-dc49a5599945.jpg" />, the above algorithm takes the form</p><p><img src="16-7400911\4d70bda6-5d8b-4131-908c-c38ae644524f.jpg" /></p><p><img src="16-7400911\8a768180-0f01-47d3-bc1b-140a98c1fe6e.jpg" /></p><p><img src="16-7400911\163823b8-7a7f-46dd-8235-b0691fc87867.jpg" /></p><p><img src="16-7400911\7ba670f5-ca11-4c86-89c7-23a1da63fb67.jpg" /></p><p>For the computation of <img src="16-7400911\cd7d7457-2846-4905-92bd-631323bd3660.jpg" /> the algorithms (18)-(21) changes only in the estimation of the diagonal elements, for which we have</p><p><img src="16-7400911\2e6f11d4-d879-4ab7-809a-8cfa71d0bf2c.jpg" /></p><p>where<img src="16-7400911\4c047be3-e1ab-4be7-9c5c-1c57abef1b58.jpg" />, <img src="16-7400911\980e24bb-7676-465b-9805-9f4889dc0f28.jpg" />, <img src="16-7400911\40ee060e-6563-42d3-af44-228436bc1586.jpg" />, and <img src="16-7400911\f63aa6f0-ae95-43b1-a2aa-6d9784e8c02f.jpg" /> are given by the relation (14). Therefore, considering the relations (9) and (14), it is clear that the number of mult/div and add/sub in computing <img src="16-7400911\a319f6f0-1c9b-4838-a8ca-ccd98fde589a.jpg" /> is the same with that of<img src="16-7400911\f676763a-daab-4d50-ac35-fd430378e12b.jpg" />.</p></sec><sec id="s5"><title>5. Concluding Remarks</title><p>The matrices A<sub>1</sub> and A<sub>2</sub> represent generalizations of known classes of test matrices. For instance, the test matrices given in [<xref ref-type="bibr" rid="scirp.23015-ref6">6</xref>] (Equations (2.1) and (2.2)) and in [<xref ref-type="bibr" rid="scirp.23015-ref1">1</xref>] (Eq. (2)) belong to the categories presented. Furthermore, by restricting the a’s and b’s to unity, A<sub>1</sub> and A<sub>2</sub> reduce to the matrices given in [<xref ref-type="bibr" rid="scirp.23015-ref2">2</xref>]. Also, the matrices in [<xref ref-type="bibr" rid="scirp.23015-ref7">7</xref>] (pp. 41, 42, 49) are special cases of A<sub>1</sub> and A<sub>2</sub>. On the other hand, concerning the recursive algorithms given in Section 4, we have performed numerical experiments by assigning random values to the parameters of A<sub>1</sub>, and with a variety of the order n from 256 to 1024. We have found that computing <img src="16-7400911\16e5cdcb-c5c8-48dd-9b3a-8c06e0371251.jpg" /> by the recursive algorithms (18)-(21) is ~100 times faster than using the LU decomposition when n = 256 and increases gradually to ~1000 times faster when n = 1024.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.23015-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">R. J. Herbold, “A Generalization of a Class of Test Matrices,” Mathematics of Computation, Vol. 23, 1969, pp. 823-826. doi:10.1090/S0025-5718-1969-0258259-0</mixed-citation></ref><ref id="scirp.23015-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">F. N. Valvi, “Explicit Presentation of the Inverses of Some Types of Matrices,” IMA Journal of Applied Mathematics, Vol. 19, No. 1, 1977, pp. 107-117.  
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doi:10.1080/00207728608926813</mixed-citation></ref><ref id="scirp.23015-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">B. Picinbono, “Fast Algorithms for Brownian Matrices,” IEEE Transactions on Acoustics, Speech and Signal Processing, Vol. 31, No. 2, 1983, pp. 512-514.  
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doi:10.1090/S0025-5718-1968-0239743-1</mixed-citation></ref><ref id="scirp.23015-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">R. T. Gregory and D. L. Karney, “A Collection of Matrices for Testing Computational Algorithms,” Wiley-Interscience, London, 1969.</mixed-citation></ref></ref-list></back></article>