<?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.2018.81002</article-id><article-id pub-id-type="publisher-id">ALAMT-81794</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>
 
 
  Moore-Penrose Inverse and Semilinear Equations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hugo</surname><given-names>Leiva</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>Raúl</surname><given-names>Manzanilla</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Yachay Tech, School of Mathematical Sciences and Information Technology, Imbabura, Ecuador</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hleiva@ula.ve(HL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>01</month><year>2018</year></pub-date><volume>08</volume><issue>01</issue><fpage>11</fpage><lpage>17</lpage><history><date date-type="received"><day>24,</day>	<month>November</month>	<year>2017</year></date><date date-type="rev-recd"><day>14,</day>	<month>January</month>	<year>2018</year>	</date><date date-type="accepted"><day>17,</day>	<month>January</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p><html>
 <head></head>
 
  In this paper, we study the existence of solutions for the semilinear equation 
  <img src="Edit_fcfafc28-ce72-4080-ab47-990cb017223a.bmp" alt="" />, where 
  <em>A</em> is a 
  <img src="Edit_5da83526-1cbc-4961-83b8-d87a7acadcfc.bmp" alt="" />, 
  <img src="Edit_f34bf6ec-96a3-4fed-945f-5278bd5ba87a.bmp" alt="" />, 
  <img src="Edit_320b2e23-d602-4a19-97a2-3c647407cee7.bmp" alt="" /> and 
  <img src="Edit_87ff7696-ea2b-4b1c-ad6a-082e191ceb5f.bmp" alt="" /> is a nonlinear continuous function. Assuming that the Moore-Penrose inverse 
  <em>A</em>
  <sup>T</sup>(
  <em>AA</em>
  <sup>T</sup>)
  <sup>-1 </sup>exists (
  <em>A </em>denotes the transposed matrix of 
  <em>A</em>) which is true whenever the determinant of the 
  <img src="Edit_77c9b8e7-5dbc-4650-8fdb-fabfcd0b8f24.bmp" alt="" /> matrix 
  <em>AA</em>
  <sup>T </sup>is different than zero, and the following condition on the nonlinear term 
  <img src="Edit_b41d91f7-cc7a-454b-b959-69c6bd65a492.bmp" alt="" /> satisfied 
  <img src="Edit_b53b8e0e-d717-4305-82cb-5ece1746d037.bmp" alt="" />. We prove that the semilinear equation has solutions for all
  <img src="Edit_87cbc1bc-ac4d-4fce-bd7a-60277a51c7a7.bmp" alt="" />. Moreover, these solutions can be found from the following fixed point relation 
  <img src="Edit_cc5ee4eb-2146-43a2-b996-a2d83109329d.bmp" alt="" />.
 
</html></p></abstract><kwd-group><kwd>Semilinear Equations</kwd><kwd> Moore-Penrose Inverse</kwd><kwd> Rothe’s Fixed Point Theorem</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>This work is devoted to study the existence of solutions for the following semilinear equation</p><p>A x + f ( x ) = b ,     b ∈   I R n ,     x ∈   I R m (1.1)</p><p>where A is a m &#215; n matrix, m ≥ n , b ∈   I R n and f :   I R m →   I R n is a nonlinear continuous function.</p><p>Definition 1.1. The Equation (1.1) is said to be solvable if for all b ∈   I R n there exists x ∈   I R m such that</p><p>A x + f ( x ) = b .</p><p>Proposition 1.1. The Equation (1.1) is solvable if, and only if, the operator A + f ( ⋅ ) :   I R m →   I R n is surjective.</p><p>The corresponding linear equation A x = b has been studied in [<xref ref-type="bibr" rid="scirp.81794-ref1">1</xref>] where a generalization of Cramer’s Rule is given applying the Moore-Penrose inverse A + = A T ( A A T ) − 1 that can be used when ( A A T ) − 1 exists, and a result from [<xref ref-type="bibr" rid="scirp.81794-ref2">2</xref>] . More information about the Moore-Penrose inverse can be found in [<xref ref-type="bibr" rid="scirp.81794-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.81794-ref4">4</xref>] .</p><p>In this paper, using Moore-Penrose inverse A + and the Rothe’s Fixed Theorem [<xref ref-type="bibr" rid="scirp.81794-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.81794-ref6">6</xref>] [<xref ref-type="bibr" rid="scirp.81794-ref7">7</xref>] , we shall prove the following theorem:</p><p>Theorem 1.1. If A T ( A A T ) − 1 exists and f is continuous and satisfies the condition</p><p>lim ‖ x ‖ → ∞ ‖ f ( x ) ‖ ‖ x ‖ = 0 , (1.2)</p><p>then Equation (1.1) is solvable.</p><p>Moreover, for each b ∈   I R n there exists x b ∈   I R m such that</p><p>A x b + f ( x b ) = b ,</p><p>where x b = A T ( A A T ) − 1 ( b − f ( x b ) ) .</p><p>The following theorem will be used to prove our main result.</p><p>Theorem 1.2. (Rothe’s Fixed Theorem [<xref ref-type="bibr" rid="scirp.81794-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.81794-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.81794-ref6">6</xref>] ) Let E be a Banach space. Let B ⊂ E be a closed convex subset such that the zero of E is contained in the interior of B . Let Φ : B → E be a continuous mapping with Φ ( B ) relatively compact in E and Φ ( ∂ B ) ⊂ B . Then there is a point x * ∈ B such that Φ ( x * ) = x * .</p></sec><sec id="s2"><title>2. Proof of the Main Theorems</title><p>In this section we shall prove the main results of this paper, Theorem 1.1, formulated in the introduction of this paper, which concern with the solvability of the semilinear Equation (1.1).</p><p>Proof of Theorem 1.1. Using the Moore-Penrose inverse we define the operator K :   I R m →   I R m by</p><p>K ( x ) = A T ( A A T ) − 1 ( b − f ( x ) ) ,</p><p>and from condition (1.2) we obtain that</p><p>lim ‖ x ‖ → ∞ ‖ K ( x ) ‖ ‖ x ‖ = 0 . (2.3)</p><p>Claim. The operator K has a fixed point. In fact, for a fixed 0 &lt; ρ &lt; 1 , there exists R &gt; 0 big enough such that</p><p>‖ K ( x ) ‖ ≤ ρ ‖ x ‖ ,     ‖ x ‖ = R .</p><p>Hence, if we denote by B ( 0, R ) the ball of center zero and radius R &gt; 0 , we get that K ( ∂ B ( 0, R ) ) ⊂ B ( 0, R ) . Since K is compact and maps the sphere ∂ B ( 0, R ) into the interior of the ball B ( 0, R ) , we can apply Rothe’s fixed point Theorem 1.2 to ensure the existence of a fixed point x b ∈ B ( 0, R ) ⊂   I R m such that</p><p>x b = K ( x b ) . (2.4)</p><p>Then,</p><p>x b = A T ( A A T ) − 1 ( b − f ( x b ) ) .</p><p>Then</p><p>A x b = b − f ( x b ) ⇔ A x b + f ( x b ) = b .</p><p>This complete the proof. □</p><p>From Banach Fixed Point Theorem it is easy to prove the following theorem that we will use to prove the next result of this paper.</p><p>Theorem 2.1. Let W be a Hilbert space and H : W → W is a Lipschitz function with a Lipschitz constant 0 &lt; h &lt; 1 and consider F ( w ) = w + H w . Then F is an homeomorphism whose inverse is a Lipschitz function with a Lipschitz constant ( 1 − h ) − 1 .</p><p>Theorem 2.2. If the Moore-Penrose A T ( A A T ) − 1 exists and the following condition holds</p><p>‖ f ( x 2 ) − f ( x 1 ) ‖ ≤ L ‖ x 2 − x 1 ‖ ,   x 1 , x 2 ∈   I R m , (2.5)</p><p>and</p><p>‖ A T ( A A T ) − 1 ‖ L &lt; ρ &lt; 1 , (2.6)</p><p>then the Equation (1.1) is solvable and a solution of it is given by</p><p>x b = A T ( A A T ) − 1 ( I + f ∘ Γ ) − 1 ( b ) , (2.7)</p><p>where Γ = A T ( A A T ) − 1 .</p><p>Proof. Define the operator F = A + f : I R m →   I R n . Then F ∘ Γ = I + f ∘ Γ and</p><p>‖ ( f ∘ Γ ) ( b 2 ) − ( f ∘ Γ ) ( b 1 ) ‖ ≤ ‖ Γ ‖ L ‖ b 2 − b 1 ‖ ,     ∀ b 1 , b 2 ∈   I R   n ,</p><p>and from condition (2.6)</p><p>‖ Γ ‖ L &lt; ρ &lt; 1 . (2.8)</p><p>Therefore, from Theorem 2.1 and (2.8) we have that F ∘ Γ = I + f ∘ Γ is a homeomorphism Lipschitizian with a Lipschitz constant 1 1 − ρ .</p><p>Then,</p><p>F ∘ ( Γ ∘ ( I + f ∘ Γ ) − 1 ) = I .</p><p>Hence, x b = ( Γ ∘ ( I + f ∘ Γ ) − 1 ) ( b ) is a solution of (1). In fact,</p><p>F ( x b ) = b ⇔ A x b + f ( x b ) = b ,</p><p>and this complete the proof. □</p></sec><sec id="s3"><title>3. Practical Example</title><p>Now, we shall apply Theorem 1.1 to find one solution of the following semilinear system</p><p>{ x 1 + x 2 + sin ( x 1 x 2 ) = 1 − x 1 + x 2 + x 3 + cos ( x 2 x 3 ) = 1 (3.9)</p><p>In this case, the vector of unknown x , the operators A , f ( x ) and the system second member b are:</p><p>x = ( x 1 x 2 x 3 )   ,     A = ( 1 1 0 − 1 1 1 )         and     f ( x ) = ( sin ( x 1 x 2 ) cos ( x 2 x 3 ) )   ,     b = ( 1 1 )</p><p>Therefore, (3.9) can be written in the form of (1.1).</p><p>A x + f ( x ) = b (3.10)</p><p>Applying Theorem 1.1 a solution of (3.10) can be obtained as a solution of the fixed-point problem:</p><p>x = A T ( A A T ) − 1 ( b − f ( x ) ) (3.11)</p><p>In this particular example, one has:</p><p>A T ( A A T ) − 1 = ( 1 2 − 1 2 1 2 1 2 0 1 2 ) (3.12)</p><p>To solve this problem numerically, one uses fixed-point iterations directly, i.e. one uses the following fixed point method:</p><p>{ l x n + 1 = A T ( A A T ) − 1 ( b − f ( x n ) ) x 0 = ( 20 10 − 1 ) (3.13)</p><p>and an error tolerance of 10 − 10 , where the error is defined for each iteration as</p><p>Error ( n ) = ‖ x n − x n − 1 ‖ ,       for     n = 1,2 , ... (3.14)</p><p>In the following figures one shows the convergence process to obtain the approximate solution. Thus, <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the fixed-point iterations (3.13) for different groups of iterations, i.e. in the subfigure “Iteration from 0 to 7” it being showed the seven first fixed-point iteration values and the initial condition x 0 , thus in the figure “Iteration from 8 to 15” it being showed the next eight the fixed-point iteration values and so on for the other subfigures. By changing the scale in the subfigures, one observes the accumulation of the point-fixed iteration values in a specific place of space and that is an indicative of fixed-point iterations convergence.</p><p>As in the previous figure, <xref ref-type="fig" rid="fig2">Figure 2</xref> shows the convergence error (3.14) of the fixed-point iterations for different groups of iterations. Herein, one can appreciate error convergences to zero quickly.</p><p>The approximated value obtained for x solution of (3.13) is:</p><p>( 414.511990290326 e − 003 414.511990290326 e − 003 0.00000000000000 e + 000 )</p><p>Here in, one presents the value <xref ref-type="table" rid="table1">Table 1</xref> of fixed-point iteration.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Fixed-point iteration values</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >i</th><th align="center" valign="middle" >W 1</th><th align="center" valign="middle" >W 2</th><th align="center" valign="middle" >W 3</th></tr></thead><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >20.0000000000000e+000</td><td align="center" valign="middle" >10.0000000000000e+000</td><td align="center" valign="middle" >−1.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >17.1128840687711e−003</td><td align="center" valign="middle" >1.85618441314522e+000</td><td align="center" valign="middle" >919.535764538226e−003</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >−83.6859033311723e−003</td><td align="center" valign="middle" >1.05192657611689e+000</td><td align="center" valign="middle" >567.806239724032e−003</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >457.390133251325e−003</td><td align="center" valign="middle" >630.527636166526e−003</td><td align="center" valign="middle" >86.5687514576005e−003</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >357.047377906710e−003</td><td align="center" valign="middle" >358.536714067085e−003</td><td align="center" valign="middle" >744.668080187583e−006</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >436.167364616208e−003</td><td align="center" valign="middle" >436.167400258264e−003</td><td align="center" valign="middle" >17.8210279311308e−009</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >405.451739883687e−003</td><td align="center" valign="middle" >405.451739883687e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >418.174158181806e−003</td><td align="center" valign="middle" >418.174158181806e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >413.010123030581e−003</td><td align="center" valign="middle" >413.010123030581e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >415.124320120457e−003</td><td align="center" valign="middle" >415.124320120457e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >414.261735970446e−003</td><td align="center" valign="middle" >414.261735970446e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >414.614167222791e−003</td><td align="center" valign="middle" >414.614167222791e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >414.470255524096e−003</td><td align="center" valign="middle" >414.470255524096e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >414.529034297305e−003</td><td align="center" valign="middle" >414.529034297305e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >414.505029226087e−003</td><td align="center" valign="middle" >414.505029226087e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >414.514833210466e−003</td><td align="center" valign="middle" >414.514833210466e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >414.510829199791e−003</td><td align="center" valign="middle" >414.510829199791e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >414.512464474425e−003</td><td align="center" valign="middle" >414.512464474425e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >414.511796615081e−003</td><td align="center" valign="middle" >414.511796615081e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >414.512069374520e−003</td><td align="center" valign="middle" >414.512069374520e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >414.511957977294e−003</td><td align="center" valign="middle" >414.511957977294e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >414.512003472857e−003</td><td align="center" valign="middle" >414.512003472857e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >414.511984892088e−003</td><td align="center" valign="middle" >414.511984892088e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >414.511992480630e−003</td><td align="center" valign="middle" >414.511992480630e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >414.511989381406e−003</td><td align="center" valign="middle" >414.511989381406e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >414.511990647155e−003</td><td align="center" valign="middle" >414.511990647155e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >414.511990130213e−003</td><td align="center" valign="middle" >414.511990130213e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >414.511990341336e−003</td><td align="center" valign="middle" >414.511990341336e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >414.511990255112e−003</td><td align="center" valign="middle" >414.511990255112e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >414.511990290326e−003</td><td align="center" valign="middle" >414.511990290326e−003</td><td align="center" valign="middle" >0.00000000000000e+000</td></tr></tbody></table></table-wrap></sec><sec id="s4"><title>Supported</title><p>This work has been supported by Yachay Tech University.</p></sec><sec id="s5"><title>Cite this paper</title><p>Leiva, H. and Manzanilla, R. (2018) Moore-Penrose Inverse and Semilinear Equations. Advances in Linear Algebra &amp; Matrix Theory, 8, 11-17. https://doi.org/10.4236/alamt.2018.81002</p></sec></body><back><ref-list><title>References</title><ref id="scirp.81794-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Leiva, H. (2015) A Generalization of Cramer’s Rule. Linear Algebra and Matrix Theory, 5, 156-166. https://doi.org/10.4236/alamt.2015.54016</mixed-citation></ref><ref id="scirp.81794-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Burgstahier, S. (1983) A Generalization of Cramer’s Rule. The Two-Year College Mathematics Journal, 14, 203-205. https://doi.org/10.2307/3027088</mixed-citation></ref><ref id="scirp.81794-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Ben-Israel, A. and Greville, T.N.E. (2002) Generalized Inverses: Theory and Applications. 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