<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2018.67117</article-id><article-id pub-id-type="publisher-id">JAMP-85885</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>
 
 
  On the Norms of &lt;i&gt;r&lt;/i&gt;-Hankel Matrices Involving Fibonacci and Lucas Numbers
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hasan</surname><given-names>Gökbaş</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>Hasan</surname><given-names>Köse</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Semsi Tebrizi Girl Anatolian Religious Vocational High School, Konya, Turkey</addr-line></aff><aff id="aff2"><addr-line>Science Faculty, Sel&amp;amp;#231;uk Universty, Konya, Turkey</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hgokbas@hotmail.com(HG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>07</month><year>2018</year></pub-date><volume>06</volume><issue>07</issue><fpage>1409</fpage><lpage>1417</lpage><history><date date-type="received"><day>15,</day>	<month>May</month>	<year>2018</year></date><date date-type="rev-recd"><day>7,</day>	<month>July</month>	<year>2018</year>	</date><date date-type="accepted"><day>10,</day>	<month>July</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>
 
 
  Let us define 
  A=H&lt;SUB&gt;r&lt;/SUB&gt;=(a&lt;SUB&gt;ij&lt;/SUB&gt;)
   
  to be n&amp;#215;n
   
  r
  -Hankel matrix. The entries of matrix A are &lt;i&gt;F&lt;sub&gt;n&lt;/sub&gt;&lt;/i&gt;=&lt;i&gt;F&lt;sub&gt;i+j-2&lt;/sub&gt;&lt;/i&gt;
  
   or &lt;i&gt;L&lt;sub&gt;n&lt;/sub&gt;&lt;/i&gt;=&lt;i&gt;F&lt;sub&gt;i+j-2&lt;/sub&gt;&lt;/i&gt;
  
   where &lt;i&gt;F&lt;sub&gt;n&lt;/sub&gt;&lt;/i&gt;
  
   and &lt;i&gt;L&lt;sub&gt;n&lt;/sub&gt;&lt;/i&gt;
  
   denote the usual Fibonacci and Lucas numbers, respectively. 
  Then, 
  we obtained upper and lower bounds for the spectral norm of matrix A. We compared our bounds with exact value of matrix A’s spectral norm. These kinds of matrices have
   connections with signal and image processing, time series analysis and many other problems.
 
</p></abstract><kwd-group><kwd>Euclidean Norm</kwd><kwd> Spectral Norm</kwd><kwd> &lt;i&gt;r&lt;/i&gt;-Hankel Matrix</kwd><kwd> Fibonacci Numbers</kwd><kwd> Lucas Numbers</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>“Special matrices” is a widely studied subject in the research area of matrix analysis. Especially, special matrices whose entries are well known number sequences have become a very interesting research subject in recent years and many authors have obtained some good results in this area. Some researches denoted the norms of the special matrices involving famous number sequences. The authors found lower bounds, upper bounds and exact values for the spectral norms of these matrices.</p><p>Our aim in this study is to obtain some norm bounds more closure than those in literature to the exact value of matrix A’s spectral norm. Lots of articles which concern estimates for spectral norms of special matrices have been written so far.</p><p>Solak has studied the norms of circulant matrices with fibonacci and lucas numbers in [<xref ref-type="bibr" rid="scirp.85885-ref1">1</xref>] , T&#252;rkmen and G&#246;kbaş have made a similar study by using the r-circulant matrix with pell and pell-lucas numbers in [<xref ref-type="bibr" rid="scirp.85885-ref2">2</xref>] , Shen and Cen have made a similar study by using the same special matrix with k-fibonacci and k-lucas numbers in [<xref ref-type="bibr" rid="scirp.85885-ref3">3</xref>] , Akbulak and Bozkurt found lower and upper bounds for the spectral norms of toeplitz matrices with classical fibonacci and lucas numbers entries in [<xref ref-type="bibr" rid="scirp.85885-ref4">4</xref>] , Shen gave upper and lower bounds for the spectral norms of toeplitz matrices with k-fibonacci and k-lucas numbers entries in [<xref ref-type="bibr" rid="scirp.85885-ref5">5</xref>] , Akbulak and Bozkurt have made a similar study by using the hankel matrix with fibonacci and lucas numbers in [<xref ref-type="bibr" rid="scirp.85885-ref6">6</xref>] , G&#246;kbaş and T&#252;rkmen gave upper and lower bounds for the spectral norms of r-toeplitz matrices involving fibonacci and lucas numbers in [<xref ref-type="bibr" rid="scirp.85885-ref7">7</xref>] , Bozkurt and Tam obtained determinants and inverse of circulant matrices with jacobsthal and jacobsthal-lucas numbers in [<xref ref-type="bibr" rid="scirp.85885-ref8">8</xref>] .</p><p>The Fibonacci and Lucas sequences F n and L n are defined by the recurrence relations (<xref ref-type="table" rid="table1">Table 1</xref>)</p><p>F 0 = 0 ,     F 1 = 1 ,     F n = F n − 1 + F n − 2     for   n ≥ 2</p><p>L 0 = 2 ,     L 1 = 1 ,     L n = L n − 1 + L n − 2     for   n ≥ 2</p><p>The following sum formulas the Fibonacci and Lucas numbers are well known [<xref ref-type="bibr" rid="scirp.85885-ref9">9</xref>] :</p><p>∑ k = 1 n − 1 F k 2 = F n F n − 1</p><p>∑ k = 1 n − 1 L k 2 = L n L n − 1 − 2</p><p>∑ k = 1 n k F k 2 = { n F n F n + 1 − F n 2 + 1 ,       if   n   is   odd n F n F n + 1 − F n 2 ,               otherwise</p><p>∑ k = 1 n k L k 2 = { n L n L n + 1 − L n 2 − 1 ,       if   n   is   odd n L n L n + 1 − F n 2 + 4 ,     otherwise</p><p>The Euclidean norm of the matrix A is defined as</p><p>‖ A ‖ E = ( ∑ i , j = 1 n | a i j | 2 ) 1 / 2</p><p>The singular values of the matrix A is</p><p>σ i = λ i ( A * A )</p><p>where λ i is an eigenvalues of matrix A * A and A * is conjugate transpose of the matrix A. The square roots of the maximum eigenvalues of A * A are called the spectral norm of A and are induced by ‖ A ‖ 2 .</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The Fibonacci and Lucas sequence have been given</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >0</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >5</th><th align="center" valign="middle" >6</th><th align="center" valign="middle" >7</th><th align="center" valign="middle" >8</th><th align="center" valign="middle" >9</th><th align="center" valign="middle" >10</th><th align="center" valign="middle" >11</th><th align="center" valign="middle" >…</th></tr></thead><tr><td align="center" valign="middle" >F<sub>n</sub></td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >34</td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >89</td><td align="center" valign="middle" >…</td></tr><tr><td align="center" valign="middle" >Q<sub>n</sub></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >18</td><td align="center" valign="middle" >29</td><td align="center" valign="middle" >47</td><td align="center" valign="middle" >76</td><td align="center" valign="middle" >123</td><td align="center" valign="middle" >199</td><td align="center" valign="middle" >…</td></tr></tbody></table></table-wrap><p>The following imequality holds,</p><p>1 n ‖ A ‖ E ≤ ‖ A ‖ 2 ≤ ‖ A ‖ E</p><p>Define the maximum row length norm r 1 and the maximum column length norm c 1 of any matrix A by</p><p>r 1 ( A ) = max i ∑ j | a i j | 2 and c 1 ( A ) = max j ∑ i | a i j | 2</p><p>respectively. Let A, B and C be m &#215; n matrices. If A = B ∘ C then</p><p>‖ A ‖ 2 ≤ r 1 ( B ) c 1 (C)</p><p>for the matrices A = ( a i j ) m &#215; n and B = ( b i j ) m &#215; n the Hadamard Product of these matrices is defined as A ∘ B = ( a i j b i j ) m &#215; n [<xref ref-type="bibr" rid="scirp.85885-ref10">10</xref>] .</p><p>Let us give some lemmas which we will use in our result.</p><p>Lemma 1.1: Be a Hankel matrix whose entries determined by a i j = F i + j − 2 where F n stands for nth Fibonacci numbers [<xref ref-type="bibr" rid="scirp.85885-ref6">6</xref>] .</p><p>− F 4 n − 3 F 2 n 2 − 2 F 2 n + 6 F n 2 − 2 + 2 [ − 1 ] n 2 n ≤ ‖ A ‖ 2</p><p>‖ A ‖ 2 ≤ ( F 2 n − 2 F 2 n − 3 − F n − 1 F n − 2 + F 2 n − 2 2 ) ( F 2 n − 2 F 2 n − 3 − F n − 1 F n − 2 + 1 )</p><p>Lemma 1.2: Be a Hankel matrix whose entries determined by a i j = F i + j − 2 where F n stands for nth Fibonacci numbers [<xref ref-type="bibr" rid="scirp.85885-ref11">11</xref>] .</p><p>‖ A ‖ 2 = { F 2 n − 1 − 1 + F 2 n − 1 2 − 2 F n − 1 + 4 F n 2 − 3 2 ,     if   n   is   odd F 2 n − 1 − 1 + F 2 n − 1 2 − 2 F n − 1 + 4 F n 2 + 1 2 ,     otherwise</p><p>Lemma 1.3: Be a Hankel matrix whose entries determined by a i j = L i + j − 2 where L n stands for nth Lucas numbers [<xref ref-type="bibr" rid="scirp.85885-ref6">6</xref>] .</p><p>L 2 n − 1 2 − 2 L n − 1 2 + 1 + 5 [ 1 − ( − 1 ) n ] n ≤ ‖ A ‖ 2</p><p>‖ A ‖ 2 ≤ ( L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 − L 2 n − 2 2 + 1 ) ( L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 )</p><p>Lemma 1.4: Be a Hankel matrix whose entries determined by a i j = L i + j − 2 where L n stands for nth Lucas numbers [<xref ref-type="bibr" rid="scirp.85885-ref11">11</xref>] .</p><p>‖ A ‖ 2 = { L 2 n − 1 + 1 + 5 ( L 2 n − 2 + L 2 n − 5 5 ) 2 + 4 2 ,     if   n   is   odd L 2 n − 1 + 1 + 5 ( L 2 n − 2 + L 2 n − 5 5 ) 2 2 ,               otherwise</p></sec><sec id="s2"><title>2. Result</title><p>In this section, we define an n &#215; n r-Hankel matrix A = H r = ( a i j ) whose entries are a i j = F i + j − 2 or a i j = L i + j − 2 where F n and L n denote the usual Fibonacci and Lucas numbers, respectively. We obtain some inequalities related to A = H r = ( a i j ) .</p><p>Definition 2.5: A matrix H r = ( h i j ) ∈ M n , n ( ∁ ) is called a r-Hankel matrix if it is of the form</p><p>H i j = { r h i + j − 2 ,     i + j ≤ n h i + j − 2 ,       i + j &gt; n</p><p>Obviously, the r-Hankel matrix H is determined by parameter r and its first row elements h 0 , h 1 , ⋯ , h n − 1 , thus we denote H = H r ( h 0 , h 1 , ⋯ , h n − 1 ) . For r =1, the matrix H is called a Hankel matrix.</p><p>Theorem 2.6: Let A = H r = ( a i j ) be a Hankel matrix satisfying a i j = F i + j − 2 , where r ∈ ( ∁ ) .</p><p>1) | r | ≥ 1 , F 2 n − 1 F 2 n − 2 + F 2 n − 2 2 − 3 F n − 1 F n − 2 − 2 F n − 2 2 + F n F n − 1 + [ 1 − ( − 1 ) n ] n ≤ A 2</p><p>‖ A ‖ 2 ≤ ( | r | 2 ( n − 1 ) + 1 ) ( F 2 n − 1 F 2 n − 2 − F n − 1 F n − 2 )</p><p>2) | r | &lt; 1 , | r | F 2 n − 1 F 2 n − 2 + F 2 n − 2 2 − 3 F n − 1 F n − 2 − 2 F n − 2 2 + F n F n − 1 + [ 1 − ( − 1 ) n ] n ≤ ‖ A ‖ 2</p><p>‖ A ‖ 2 ≤ n ( F 2 n − 1 F 2 n − 2 − F n − 1 F n − 2 )</p><p>where ‖   .   ‖ 2 is the spectral norm and F n denotes the nth Fibonacci number.</p><p>Proof. The matrix A is of the form</p><p>A = [ r F 0 r F 1 ⋯ F n − 1 r F 1 ⋯ F n ⋮ ⋮ ⋱ ⋮ F n − 1 F n ⋯ F 2 n − 2 ]</p><p>Then,</p><p>‖ A ‖ F 2 = ∑ k = 0 n − 2 | r | 2 ( k + 1 ) F k 2 + ∑ k = n − 1 2 n − 2 ( 2 n − 1 − k ) F k 2 .</p><p>Hence, when | r | ≥ 1 we obtain</p><p>‖ A ‖ F 2 ≥ ∑ k = 0 n − 2 ( k + 1 ) F k 2 + ∑ k = n − 1 2 n − 2 ( 2 n − 1 − k ) F k 2 ≥ ( 2 n − 1 ) ∑ k = 0 n − 2 F k 2 − ∑ k = 1 2 n − 2 k F k 2 − ( 2 n − 1 ) ∑ k = 0 n − 2 F k 2 + 2 ∑ k = 1 n − 2 k F k 2 + ∑ k = 0 n − 2 F k 2 ≥ F 2 n − 1 F 2 n − 2 + F 2 n − 2 2 − 3 F n − 1 F n − 2 − 2 F n − 2 2 + F n F n − 1 + [ 1 − ( − 1 ) n ]</p><p>‖ A ‖ 2 ≥ F 2 n − 1 F 2 n − 2 + F 2 n − 2 2 − 3 F n − 1 F n − 2 − 2 F n − 2 2 + F n F n − 1 + [ 1 − ( − 1 ) n ] n .</p><p>On the other hand, let the matrices B and C be n &#215; n matrices satisfying A = B ∘ C .</p><p>B = [ r r ⋯ 1 r ⋯ 1 ⋮ ⋮ ⋱ ⋮ 1 1 ⋯ 1 ] and C = [ F 0 F 1 ⋯ F n − 1 F 1 ⋯ F n ⋮ ⋮ ⋱ ⋮ F n − 1 F n ⋯ F 2 n − 2 ]</p><p>Since</p><p>r 1 ( B ) = max i ∑ j | b i j | 2 = ∑ j = 0 n − 1 | b n j | 2 = | r | 2 ( n − 1 ) + 1</p><p>and</p><p>c 1 ( C ) = max j ∑ i | c i j | 2 = ∑ i = 0 n − 1 | c i n | 2 = ∑ i = n − 1 2 n − 2 F i 2 = F 2 n − 1 F 2 n − 2 − F n − 1 F n − 2 ,</p><p>we have</p><p>‖ A ‖ 2 ≤ ( | r | 2 ( n − 1 ) + 1 ) ( F 2 n − 1 F 2 n − 2 − F n − 1 F n − 2 ) .</p><p>when | r | &lt; 1 we also obtain</p><p>A F 2 ≥ | r | 2 [ ∑ k = 0 n − 2 ( k + 1 ) F k 2 + ∑ k = n − 1 2 n − 2 ( 2 n − 1 − k ) F k 2 ] ≥ | r | 2 [ ( 2 n − 1 ) ∑ k = 0 n − 2 F k 2 − ∑ k = 1 2 n − 2 k F k 2 − ( 2 n − 1 ) ∑ k = 0 n − 2 F k 2 + 2 ∑ k = 1 n − 2 k F k 2 + ∑ k = 0 n − 2 F k 2 ] ≥ | r | 2 [ F 2 n − 1 F 2 n − 2 + F 2 n − 2 2 − 3 F n − 1 F n − 2 − 2 F n − 2 2 + F n F n − 1 + [ 1 − ( − 1 ) n ] ]</p><p>‖ A ‖ 2 ≥ | r | F 2 n − 1 F 2 n − 2 + F 2 n − 2 2 − 3 F n − 1 F n − 2 − 2 F n − 2 2 + F n F n − 1 + [ 1 − ( − 1 ) n ] n .</p><p>On the other hand, let the matrices B and C be n &#215; n matrices satisfying A = B ∘ C .</p><p>B = [ r r ⋯ 1 r ⋯ 1 ⋮ ⋮ ⋱ ⋮ 1 1 ⋯ 1 ] and C = [ F 0 F 1 ⋯ F n − 1 F 1 ⋯ F n ⋮ ⋮ ⋱ ⋮ F n − 1 F n ⋯ F 2 n − 2 ]</p><p>Since</p><p>r 1 ( B ) = max i ∑ j | b i j | 2 = ∑ j = 0 n − 1 | b n j | 2 = n</p><p>and</p><p>c 1 ( C ) = max j ∑ i | c i j | 2 = ∑ i = 0 n − 1 | c i n | 2 = ∑ i = n − 1 2 n − 2 F i 2 = F 2 n − 1 F 2 n − 2 − F n − 1 F n − 2 ,</p><p>we have</p><p>‖ A ‖ 2 ≤ n ( F 2 n − 1 F 2 n − 2 − F n − 1 F n − 2 ) .</p><p>Thus, the proof is concluded.</p><p>Theorem 2.7: Let A = H r = ( a i j ) be a Hankel matrix satisfying a i j = L i + j − 2 , where r ∈ ( ∁ ) .</p><p>1) | r | ≥ 1 , ‖ A ‖ 2 ≥ { L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 1 n ,       if   n   is   odd L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 6 n ,     otherwise</p><p>‖ A ‖ 2 ≤ ( | r | 2 ( n − 1 ) + 1 ) ( L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 )</p><p>2) | r | &lt; 1 , ‖ A ‖ 2 ≥ { | r | L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 1 n ,     if   n   is   odd | r | L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 6 n ,     otherwise</p><p>‖ A ‖ 2 ≤ n ( L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 )</p><p>where L n is the spectral norm and L n denotes the nth Lucas number.</p><p>Proof. The matrix A is of the form</p><p>A = [ r F 0 r F 1 ⋯ F n − 1 r F 1 ⋯ F n ⋮ ⋮ ⋱ ⋮ F n − 1 F n ⋯ F 2 n − 2 ]</p><p>Then,</p><p>‖ A ‖ F 2 = ∑ k = 0 n − 2 | r | 2 ( k + 1 ) L k 2 + ∑ k = n − 1 2 n − 2 ( 2 n − 1 − k ) L k 2 .</p><p>Hence, when | r | ≥ 1 we obtain</p><p>A F 2 ≥ ∑ k = 0 n − 2 ( k + 1 ) L k 2 + ∑ k = n − 1 2 n − 2 ( 2 n − 1 − k ) L k 2 ≥ ( 2 n − 1 ) ∑ k = 0 n − 2 L k 2 − ∑ k = n − 1 2 n − 2 k L k 2 − ( 2 n − 1 ) ∑ k = 0 n − 2 L k 2 + 2 ∑ k = 1 n − 2 k L k 2 + ∑ k = 0 n − 2 L k 2 ≥ { L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 1 ,     if   n   is   odd L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 6 ,     otherwise</p><p>‖ A ‖ 2 ≥ { L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 1 n ,     if   n   is   odd L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 6 n ,     otherwise</p><p>On the other hand, let the matrices B and C be n &#215; n matrices satisfying A = B ∘ C .</p><p>B = [ r r ⋯ 1 r ⋯ 1 ⋮ ⋮ ⋱ ⋮ 1 1 ⋯ 1 ] and C = [ L 0 L 1 ⋯ L n − 1 L 1 ⋯ L n ⋮ ⋮ ⋱ ⋮ L n − 1 L n ⋯ L 2 n − 2 ]</p><p>Since</p><p>r 1 ( B ) = max i ∑ j | b i j | 2 = ∑ j = 0 n − 1 | b n j | 2 = | r | 2 ( n − 1 ) + 1</p><p>and</p><p>c 1 ( C ) = max j ∑ i | c i j | 2 = ∑ i = 0 n − 1 | c i n | 2 = ∑ i = n − 1 2 n − 2 L i 2 = L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 ,</p><p>we have</p><p>‖ A ‖ 2 ≤ ( | r | 2 ( n − 1 ) + 1 ) ( L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 ) .</p><p>when | r | &lt; 1 we also obtain</p><p>‖ A ‖ F 2 ≥ | r | 2 [ ∑ k = 0 n − 2 ( k + 1 ) L k 2 + ∑ k = n − 1 2 n − 2 ( 2 n − 1 − k ) L k 2 ] ≥ | r | 2 [ ( 2 n − 1 ) ∑ k = 0 n − 2 L k 2 − ∑ k = 1 2 n − 2 k L k 2 − ( 2 n − 1 ) ∑ k = 0 n − 2 L k 2 + 2 ∑ k = 1 n − 2 k L k 2 + ∑ k = 0 n − 2 L k 2 ] ≥ | r | 2 { L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 1 ,     if   n   is   odd L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 6 ,     otherwise</p><p>‖ A ‖ 2 ≥ { | r | L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 1 n ,     if   n   is   odd | r | L 2 n − 1 L 2 n − 2 − 2 L n − 1 L n − 2 + L 2 n − 2 2 − 2 L n − 2 2 + 6 n ,     otherwise</p><p>On the other hand, let the matrices B and C be n &#215; n matrices satisfying A = B ∘ C .</p><p>B = [ r r ⋯ 1 r ⋯ 1 ⋮ ⋮ ⋱ ⋮ 1 1 ⋯ 1 ] and C = [ L 0 L 1 ⋯ L n − 1 L 1 ⋯ L n ⋮ ⋮ ⋱ ⋮ L n − 1 L n ⋯ L 2 n − 2 ]</p><p>Since</p><p>r 1 ( B ) = max i ∑ j | b i j | 2 = ∑ j = 0 n − 1 | b n j | 2 = n</p><p>and</p><p>c 1 ( C ) = max j ∑ i | c i j | 2 = ∑ i = 0 n − 1 | c i n | 2 = ∑ i = n − 1 2 n − 2 L i 2 = L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 ,</p><p>we have ‖ A ‖ 2 ≤ n ( L 2 n − 1 L 2 n − 2 − L n − 1 L n − 2 ) .</p><p>Thus, the proof is concluded.</p></sec><sec id="s3"><title>3. Numerical Examples</title><p>Example 3.8: Let A = H r ( F 0 , F 1 , ⋯ , F n − 1 ) be a r-Hankel matrix where r ∈ ( ∁ ) . It can easily be seen that the values obtained in theorem 2.6. are more closure than those obtained in lemma 1.1. to exact values in from <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>Example 3.9: Let A = H r ( L 0 , L 1 , ⋯ , L n − 1 ) be a r-Hankel matrix where r ∈ ( ∁ ) . It can easily be seen that the values obtained in theorem 2.7. are more closure than those obtained in lemma 1.3. to exact values in from <xref ref-type="table" rid="table3">Table 3</xref>.</p><table-wrap-group id="2"><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Numerical results of a i j = F i + j − 2 , r = 1 </title></caption><table-wrap id="2_1"><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >Lemma 1.1.</th><th align="center" valign="middle" >Theorem 2.6.</th><th align="center" valign="middle" >Lemma 1.2. (exact value)</th></tr></thead></tbody></table></table-wrap><table-wrap id="2_2"><table><tbody><thead><tr><th align="center" valign="middle" >2</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >1 + 5 2</th></tr></thead><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >84</td><td align="center" valign="middle" >42</td><td align="center" valign="middle" >4 + 28 2</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3978</td><td align="center" valign="middle" >408</td><td align="center" valign="middle" >12 + 180 2</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >189744</td><td align="center" valign="middle" >3540</td><td align="center" valign="middle" >33 + 1185 2</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >9057280</td><td align="center" valign="middle" >29280</td><td align="center" valign="middle" >88 + 7674 2</td></tr><tr><td align="center" valign="middle" >⋮</td><td align="center" valign="middle" >⋮</td><td align="center" valign="middle" >⋮</td><td align="center" valign="middle" >⋮</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Numerical results of a i j = L i + j − 2 , r = 1 </title></caption><table><tbody><thead><tr><th align="center" valign="middle" >n</th><th align="center" valign="middle" >Lemma 1.3.</th><th align="center" valign="middle" >Theorem 2.7.</th><th align="center" valign="middle" >Lemma 1.4. (exact value)</th></tr></thead><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >5 + 5 2</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1184</td><td align="center" valign="middle" >222</td><td align="center" valign="middle" >12 + 84 2</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >95370</td><td align="center" valign="middle" >2040</td><td align="center" valign="middle" >30 + 720 2</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >4708068</td><td align="center" valign="middle" >17720</td><td align="center" valign="middle" >77 + 5449 2</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >226236800</td><td align="center" valign="middle" >146400</td><td align="center" valign="middle" >200 + 38720 2</td></tr><tr><td align="center" valign="middle" >⋮</td><td align="center" valign="middle" >⋮</td><td align="center" valign="middle" >⋮</td><td align="center" valign="middle" >⋮</td></tr></tbody></table></table-wrap></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we firstly define the r-Hankel matrix with entries Fibonacci and Lucas numbers. Then we introduce the Euclidean norm equality and the spectral norm inequalities of these matrices. Furthermore, we compared our finding with the exact value of matrix A’s spectral norm. In the future we shall further develop some kinds of r-Hankel matrix such as right r-Hankel, left r-Hankel and geometric r-Hankel. Also we will observe upper and lower bounds for the spectral norm of these matrices involving famous number sequences.</p></sec><sec id="s5"><title>Cite this paper</title><p>G&#246;kbaş, H. and K&#246;se, H. (2018) On the Norms of r-Hankel Matrices Involving Fibonacci and Lucas Numbers. Journal of Applied Mathematics and Physics, 6, 1409-1417. https://doi.org/10.4236/jamp.2018.67117</p></sec></body><back><ref-list><title>References</title><ref id="scirp.85885-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Solak, S. 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