Battles of El Bruch and Spectral radius: Difference between pages
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In [[mathematics]], the '''spectral radius''' of a [[matrix (mathematics)|matrix]] or a [[bounded linear operator]] is the [[supremum]] among the [[absolute value]]s of the elements in its [[spectrum of a matrix|spectrum]], which is sometimes denoted by ρ(·). |
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{{Infobox Military Conflict |
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|conflict=Battles of El Bruc |
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|partof=the [[Peninsular War]] |
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|image= |
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|caption= |
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|date=[[June 6]] and [[June 14]], [[1808]] |
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|place=the [[Bruc]], near [[Barcelona]], [[Spain]] |
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|result=Spanish victory |
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|combatant1={{flagicon|France}} [[First French Empire|French Empire]] |
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|combatant2={{flagicon|Spain|1785}} [[Spain]] |
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|commander1=[[François Xavier de Schwarz]] |
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|commander2=[[Antonio Franch de Villafranca]] |
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|strength1=3,800 regulars |
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|strength2=2,000 regulars and militia |
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|casualties1=360 dead,<br>600 wounded<br>60 captured |
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|casualties2=20 dead<br>80 wounded |
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}} |
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{{Campaignbox Peninsular War:1808}} |
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==Spectral radius of a matrix== |
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The two '''Battles of the Bruch''' were engagements fought successively between a [[France|French]] column and a body of [[Spain|Spanish]] volunteers and mercenaries on [[June 4]], [[1808]] in the [[Peninsular War]]. |
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Let λ<sub>1</sub>, …, λ<sub>''s''</sub> be the ([[real number|real]] or [[complex number|complex]]) eigenvalues of a matrix ''A'' ∈ '''C'''<sup>''n'' × ''n''</sup>. Then its spectral radius ρ(''A'') is defined as: |
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:<math>\rho(A) := \max_i(|\lambda_i|)</math> |
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The French detachment under General Schwartz emerged from [[Barcelona]] on [[June 4]], advancing in the direction of [[Zaragoza]]–[[Lleida]]. A rainstorm that day slowed their march considerably; the delay gave time for local Spanish forces, composed of militia from the neighboring villages, [[Catalan people|Catalan]] volunteers (''somatén''), and [[Swiss]] and [[Walloons|Walloon]] soldiers from the Barcelona garrison, to mobilize for action. The Spaniards were led by General Franch and deployed along Bruch Pass. |
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The following lemma shows a simple yet useful upper bound for the spectral radius of a matrix: |
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The resulting stand was a success,<ref>Gates, p. 59</ref> and the French under General Schwartz were turned back to Barcelona with the loss of 300 dead and one [[artillery|gun]] captured. The partisans made off with an [[Imperial eagle]], adding to the French humiliation.<ref>Solís, p. 167</ref> |
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'''Lemma''': Let ''A'' ∈ '''C'''<sup>''n'' × ''n''</sup> be a complex-valued matrix, ρ(''A'') its spectral radius and ||·|| a [[matrix norm|consistent matrix norm]]; then, for each ''k'' ∈ '''N''': |
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A second French sortie on [[June 14]] succeeded only in putting to the torch several buildings in El Bruc. |
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:<math>\rho(A)\leq \|A^k\|^{1/k},\ \forall k \in \mathbb{N}.</math> |
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==Notes== |
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<div class="references-2column"><references/></div> |
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''Proof'': Let ('''v''', λ) be an [[eigenvector]]-[[eigenvalue]] pair for a matrix ''A''. By the sub-multiplicative property of the matrix norm, we get: |
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==References== |
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*Gates, David. ''The Spanish Ulcer: A History of the Peninsular War.'' Da Capo Press 2001. ISBN 0-306-81083-2 |
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*Rodríguez-Solís, Enrique. ''Los guerrilleros de 1808: Historia popular de la Guerra de la Independencia.'' Vol. I. Calle de Balmes 1895. |
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::<math>|\lambda|^k\|\mathbf{v}\| = \|\lambda^k \mathbf{v}\| = \|A^k \mathbf{v}\| \leq \|A^k\|\cdot\|\mathbf{v}\|</math> |
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{{DEFAULTSORT:El Bruc}} |
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[[Category:Battles of the Peninsular War]] |
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[[Category:Battles involving Spain]] |
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[[Category:Conflicts in 1808]] |
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[[Category:1808 in France]] |
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:and since '''v''' ≠ 0 for each λ we have |
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{{Spain-battle-stub}} |
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{{France-battle-stub}} |
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:<math>|\lambda|^k\leq \|A^k\|</math> |
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[[ca:Batalla del Bruc]] |
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[[es:Batalla del Bruc]] |
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:and therefore |
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[[gl:Batalla de El Bruc]] |
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[[pl:Bitwa pod El Bruc]] |
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:<math>\rho(A)\leq \|A^k\|^{1/k}\,\,\square</math> |
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The spectral radius is closely related to the behaviour of the convergence of the power sequence of a matrix; namely, the following theorem holds: |
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'''Theorem''': Let ''A'' ∈ '''C'''<sup>''n'' × ''n''</sup> be a complex-valued matrix and ρ(''A'') its spectral radius; then |
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:<math>\lim_{k \to \infty}A^k=0</math> if and only if <math>\rho(A)<1.</math> |
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Moreover, if ρ(''A'')>1, <math>\|A^k\|</math> is not bounded for increasing k values. |
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''Proof'': |
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(<math>\lim_{k \to \infty}A^k = 0 \Rightarrow \rho(A) < 1</math>) |
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:Let ('''v''', λ) be an [[eigenvector]]-[[eigenvalue]] pair for matrix ''A''. Since |
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::<math>A^k\mathbf{v} = \lambda^k\mathbf{v},</math> |
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:we have: |
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::{| |
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|- |
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|<math>0\,</math> |
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|<math>= (\lim_{k \to \infty}A^k)\mathbf{v}</math> |
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|- |
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| |
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|<math>= \lim_{k \to \infty}A^k\mathbf{v}</math> |
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|- |
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| |
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|<math>= \lim_{k \to \infty}\lambda^k\mathbf{v}</math> |
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|- |
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| |
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|<math>= \mathbf{v}\lim_{k \to \infty}\lambda^k</math> |
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|} |
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:and, since by hypothesis '''v''' ≠ 0, we must have |
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::<math>\lim_{k \to \infty}\lambda^k = 0</math> |
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:which implies |λ| < 1. Since this must be true for any eigenvalue λ, we can conclude ρ(''A'') < 1. |
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(<math>\rho(A)<1 \Rightarrow \lim_{k \to \infty}A^k = 0</math>) |
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:From the [[Jordan normal form|Jordan Normal Form]] Theorem, we know that for any complex valued matrix ''A'' ∈ '''C'''<sup>''n'' × ''n''</sup>, a non-singular matrix ''V'' ∈ '''C'''<sup>''n'' × ''n''</sup> and a block-diagonal matrix ''J'' ∈ '''C'''<sup>''n'' × ''n''</sup> exist such that: |
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::<math>A = VJV^{-1}</math> |
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:with |
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::<math>J=\begin{bmatrix} |
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J_{m_1}(\lambda_1) & 0 & 0 & \cdots & 0 \\ |
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0 & J_{m_2}(\lambda_2) & 0 & \cdots & 0 \\ |
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\vdots & \cdots & \ddots & \cdots & \vdots \\ |
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0 & \cdots & 0 & J_{m_{s-1}}(\lambda_{s-1}) & 0 \\ |
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0 & \cdots & \cdots & 0 & J_{m_s}(\lambda_s) |
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\end{bmatrix}</math> |
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:where |
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::<math>J_{m_i}(\lambda_i)=\begin{bmatrix} |
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\lambda_i & 1 & 0 & \cdots & 0 \\ |
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0 & \lambda_i & 1 & \cdots & 0 \\ |
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\vdots & \vdots & \ddots & \ddots & \vdots \\ |
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0 & 0 & \cdots & \lambda_i & 1 \\ |
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0 & 0 & \cdots & 0 & \lambda_i |
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\end{bmatrix}\in \mathbb{C}^{m_i,m_i}, 1\leq i\leq s.</math> |
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:It is easy to see that |
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::<math>A^k=VJ^kV^{-1}</math> |
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:and, since ''J'' is block-diagonal, |
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::<math>J^k=\begin{bmatrix} |
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J_{m_1}^k(\lambda_1) & 0 & 0 & \cdots & 0 \\ |
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0 & J_{m_2}^k(\lambda_2) & 0 & \cdots & 0 \\ |
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\vdots & \cdots & \ddots & \cdots & \vdots \\ |
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0 & \cdots & 0 & J_{m_{s-1}}^k(\lambda_{s-1}) & 0 \\ |
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0 & \cdots & \cdots & 0 & J_{m_s}^k(\lambda_s) |
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\end{bmatrix}</math> |
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:Now, a standard result on the ''k''-power of an ''m''<sub>''i''</sub> × ''m''<sub>''i''</sub> Jordan block states that, for ''k'' ≥ ''m''<sub>''i'' − 1</sub>: |
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::<math>J_{m_i}^k(\lambda_i)=\begin{bmatrix} |
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\lambda_i^k & {k \choose 1}\lambda_i^{k-1} & {k \choose 2}\lambda_i^{k-2} & \cdots & {k \choose m_i-1}\lambda_i^{k-m_i+1} \\ |
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0 & \lambda_i^k & {k \choose 1}\lambda_i^{k-1} & \cdots & {k \choose m_i-2}\lambda_i^{k-m_i+2} \\ |
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\vdots & \vdots & \ddots & \ddots & \vdots \\ |
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0 & 0 & \cdots & \lambda_i^k & {k \choose 1}\lambda_i^{k-1} \\ |
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0 & 0 & \cdots & 0 & \lambda_i^k |
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\end{bmatrix}</math> |
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:Thus, if ρ(''A'') < 1 then |λ<sub>''i''</sub>| < 1 ∀ ''i'', so that |
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::<math>\lim_{k \to \infty}J_{m_i}^k=0\ \forall i</math> |
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:which implies |
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::<math>\lim_{k \to \infty}J^k = 0.</math> |
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:Therefore, |
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::<math>\lim_{k \to \infty}A^k=\lim_{k \to \infty}VJ^kV^{-1}=V(\lim_{k \to \infty}J^k)V^{-1}=0</math> |
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On the other side, if ρ(''A'')>1, there is at least one element in ''J'' which doesn't remain bounded as k increases, so proving the second part of the statement. |
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::<math>\square</math> |
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==Theorem (Gelfand's formula, 1941)== |
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For any [[matrix norm]] ||·||, we have |
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:<math>\rho(A)=\lim_{k \to \infty}||A^k||^{1/k}.</math> |
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In other words, the Gelfand's formula shows how the spectral radius of ''A'' gives the asymptotic growth rate of the norm of ''A''<sup>''k''</sup>: |
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:<math>\|A^k\|\sim\rho(A)^k</math> for <math>k\rightarrow \infty.\,</math> |
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''Proof'': For any ε > 0, consider the matrix |
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::<math>\tilde{A}=(\rho(A)+\epsilon)^{-1}A.</math> |
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:Then, obviously, |
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::<math>\rho(\tilde{A}) = \frac{\rho(A)}{\rho(A)+\epsilon} < 1</math> |
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:and, by the previous theorem, |
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::<math>\lim_{k \to \infty}\tilde{A}^k=0.</math> |
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:That means, by the sequence limit definition, a natural number ''N<sub>1</sub>'' ∈ '''N''' exists such that |
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::<math>\forall k\geq N_1 \Rightarrow \|\tilde{A}^k\| < 1</math> |
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:which in turn means: |
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::<math>\forall k\geq N_1 \Rightarrow \|A^k\| < (\rho(A)+\epsilon)^k</math> |
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:or |
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::<math>\forall k\geq N_1 \Rightarrow \|A^k\|^{1/k} < (\rho(A)+\epsilon).</math> |
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:Let's now consider the matrix |
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::<math>\check{A}=(\rho(A)-\epsilon)^{-1}A.</math> |
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:Then, obviously, |
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::<math>\rho(\check{A}) = \frac{\rho(A)}{\rho(A)-\epsilon} > 1</math> |
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:and so, by the previous theorem,<math>\|\check{A}^k\|</math> is not bounded. |
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:This means a natural number ''N<sub>2</sub>'' ∈ '''N''' exists such that |
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::<math>\forall k\geq N_2 \Rightarrow \|\check{A}^k\| > 1</math> |
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:which in turn means: |
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::<math>\forall k\geq N_2 \Rightarrow \|A^k\| > (\rho(A)-\epsilon)^k</math> |
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:or |
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::<math>\forall k\geq N_2 \Rightarrow \|A^k\|^{1/k} > (\rho(A)-\epsilon).</math> |
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:Taking |
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::<math>N:=max(N_1,N_2)</math> |
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:and putting it all together, we obtain: |
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::<math>\forall \epsilon>0, \exists N\in\mathbb{N}: \forall k\geq N \Rightarrow \rho(A)-\epsilon < \|A^k\|^{1/k} < \rho(A)+\epsilon</math> |
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:which, by definition, is |
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::<math>\lim_{k \to \infty}\|A^k\|^{1/k} = \rho(A).\,\,\square</math> |
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Gelfand's formula leads directly to a bound on the spectral radius of a product of finitely many matrices, namely assuming that they all commute we obtain |
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<math> |
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\rho(A_1 A_2 \ldots A_n) \leq \rho(A_1) \rho(A_2)\ldots \rho(A_n). |
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</math> |
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Actually, in case the norm is [[matrix norm|consistent]], the proof shows more than the thesis; in fact, using the previous lemma, we can replace in the limit definition the left lower bound with the spectral radius itself and write more precisely: |
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::<math>\forall \epsilon>0, \exists N\in\mathbb{N}: \forall k\geq N \Rightarrow \rho(A) \leq \|A^k\|^{1/k} < \rho(A)+\epsilon</math> |
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:which, by definition, is |
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:<math>\lim_{k \to \infty}\|A^k\|^{1/k} = \rho(A)^+.</math> |
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'''Example''': Let's consider the matrix |
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:<math>A=\begin{bmatrix} |
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9 & -1 & 2\\ |
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-2 & 8 & 4\\ |
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1 & 1 & 8 |
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\end{bmatrix}</math> |
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whose eigenvalues are 5, 10, 10; by definition, its spectral radius is ρ(''A'')=10. In the following table, the values of <math>\|A^k\|^{1/k}</math> for the four most used norms are listed versus several increasing values of k (note that, due to the particular form of this matrix,<math>\|.\|_1=\|.\|_\infty</math>): |
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<table border="0" cellspacing="0" cellpadding="0" width="756"> |
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<tr> |
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<td> k </td><td> <math>\|.\|_1=\|.\|_\infty</math> </td><td> <math>\|.\|_F</math> </td><td> <math>\|.\|_2</math> </td> |
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</tr> |
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<tr> |
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<td> </td> |
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</tr> |
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<tr> |
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<td>1</td> |
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<td>14</td> |
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<td>15.362291496</td> |
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<td>10.681145748</td> |
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</tr> |
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<tr> |
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<td>2</td> |
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<td>12.649110641</td> |
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<td>12.328294348</td> |
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<td>10.595665162</td> |
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</tr> |
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<tr> |
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<td>3</td> |
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<td>11.934831919</td> |
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<td>11.532450664</td> |
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<td>10.500980846</td> |
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</tr> |
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<tr> |
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<td>4</td> |
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<td>11.501633169</td> |
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<td>11.151002986</td> |
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<td>10.418165779</td> |
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</tr> |
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<tr> |
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<td>5</td> |
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<td>11.216043151</td> |
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<td>10.921242235</td> |
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<td>10.351918183</td> |
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</tr> |
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<tr> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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</tr> |
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<tr> |
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<td>10</td> |
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<td>10.604944422</td> |
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<td>10.455910430</td> |
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<td>10.183690042</td> |
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</tr> |
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<tr> |
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<td>11</td> |
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<td>10.548677680</td> |
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<td>10.413702213</td> |
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<td>10.166990229</td> |
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</tr> |
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<tr> |
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<td>12</td> |
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<td>10.501921835</td> |
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<td>10.378620930</td> |
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<td>10.153031596</td> |
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</tr> |
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<tr> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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</tr> |
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<tr> |
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<td>20</td> |
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<td>10.298254399</td> |
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<td>10.225504447</td> |
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<td>10.091577411</td> |
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</tr> |
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<tr> |
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<td>30</td> |
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<td>10.197860892</td> |
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<td>10.149776921</td> |
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<td>10.060958900</td> |
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</tr> |
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<tr> |
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<td>40</td> |
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<td>10.148031640</td> |
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<td>10.112123681</td> |
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<td>10.045684426</td> |
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</tr> |
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<tr> |
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<td>50</td> |
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<td>10.118251035</td> |
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<td>10.089598820</td> |
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<td>10.036530875</td> |
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</tr> |
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<tr> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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</tr> |
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<tr> |
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<td>100</td> |
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<td>10.058951752</td> |
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<td>10.044699508</td> |
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<td>10.018248786</td> |
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</tr> |
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<tr> |
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<td>200</td> |
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<td>10.029432562</td> |
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<td>10.022324834</td> |
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<td>10.009120234</td> |
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</tr> |
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<tr> |
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<td>300</td> |
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<td>10.019612095</td> |
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<td>10.014877690</td> |
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<td>10.006079232</td> |
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</tr> |
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<tr> |
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<td>400</td> |
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<td>10.014705469</td> |
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<td>10.011156194</td> |
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<td>10.004559078</td> |
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</tr> |
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<tr> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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</tr> |
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<tr> |
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<td>1000</td> |
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<td>10.005879594</td> |
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<td>10.004460985</td> |
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<td>10.001823382</td> |
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</tr> |
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<tr> |
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<td>2000</td> |
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<td>10.002939365</td> |
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<td>10.002230244</td> |
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<td>10.000911649</td> |
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</tr> |
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<tr> |
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<td>3000</td> |
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<td>10.001959481</td> |
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<td>10.001486774</td> |
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<td>10.000607757</td> |
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</tr> |
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<tr> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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</tr> |
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<tr> |
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<td>10000</td> |
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<td>10.000587804</td> |
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<td>10.000446009</td> |
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<td>10.000182323</td> |
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</tr> |
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<tr> |
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<td>20000</td> |
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<td>10.000293898</td> |
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<td>10.000223002</td> |
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<td>10.000091161</td> |
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</tr> |
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<tr> |
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<td>30000</td> |
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<td>10.000195931</td> |
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<td>10.000148667</td> |
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<td>10.000060774</td> |
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</tr> |
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<tr> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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<td><math>\vdots</math></td> |
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</tr> |
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<tr> |
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<td>100000</td> |
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<td>10.000058779</td> |
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<td>10.000044600</td> |
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<td>10.000018232 </td> |
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</tr> |
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</table> |
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==Spectral radius of a bounded linear operator== |
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For a [[bounded linear operator]] ''A'' and the [[operator norm]] ||·||, again we have |
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:<math>\rho(A) = \lim_{k \to \infty}\|A^k\|^{1/k}.</math> |
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==Spectral radius of a graph== |
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The '''spectral radius''' of a [[graph (mathematics)|graph]] is defined to be the spectral radius of its [[adjacency matrix]]. |
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==See also== |
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* [[Spectral gap]] |
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== External links == |
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* [http://people.csse.uwa.edu.au/gordon/planareig.html Spectral Radius of Planar Graphs] |
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[[Category:Spectral theory]] |
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[[Category:Articles containing proofs]] |
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[[de:Spektralradius]] |
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[[fa:شعاع طیفی]] |
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[[fr:Rayon spectral]] |
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[[it:Raggio spettrale]] |
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[[pl:Promień spektralny]] |
Revision as of 12:44, 11 October 2008
In mathematics, the spectral radius of a matrix or a bounded linear operator is the supremum among the absolute values of the elements in its spectrum, which is sometimes denoted by ρ(·).
Spectral radius of a matrix
Let λ1, …, λs be the (real or complex) eigenvalues of a matrix A ∈ Cn × n. Then its spectral radius ρ(A) is defined as:
The following lemma shows a simple yet useful upper bound for the spectral radius of a matrix:
Lemma: Let A ∈ Cn × n be a complex-valued matrix, ρ(A) its spectral radius and ||·|| a consistent matrix norm; then, for each k ∈ N:
Proof: Let (v, λ) be an eigenvector-eigenvalue pair for a matrix A. By the sub-multiplicative property of the matrix norm, we get:
- and since v ≠ 0 for each λ we have
- and therefore
The spectral radius is closely related to the behaviour of the convergence of the power sequence of a matrix; namely, the following theorem holds:
Theorem: Let A ∈ Cn × n be a complex-valued matrix and ρ(A) its spectral radius; then
- if and only if
Moreover, if ρ(A)>1, is not bounded for increasing k values.
Proof:
()
- Let (v, λ) be an eigenvector-eigenvalue pair for matrix A. Since
- we have:
- and, since by hypothesis v ≠ 0, we must have
- which implies |λ| < 1. Since this must be true for any eigenvalue λ, we can conclude ρ(A) < 1.
()
- From the Jordan Normal Form Theorem, we know that for any complex valued matrix A ∈ Cn × n, a non-singular matrix V ∈ Cn × n and a block-diagonal matrix J ∈ Cn × n exist such that:
- with
- where
- It is easy to see that
- and, since J is block-diagonal,
- Now, a standard result on the k-power of an mi × mi Jordan block states that, for k ≥ mi − 1:
- Thus, if ρ(A) < 1 then |λi| < 1 ∀ i, so that
- which implies
- Therefore,
On the other side, if ρ(A)>1, there is at least one element in J which doesn't remain bounded as k increases, so proving the second part of the statement.
Theorem (Gelfand's formula, 1941)
For any matrix norm ||·||, we have
In other words, the Gelfand's formula shows how the spectral radius of A gives the asymptotic growth rate of the norm of Ak:
- for
Proof: For any ε > 0, consider the matrix
- Then, obviously,
- and, by the previous theorem,
- That means, by the sequence limit definition, a natural number N1 ∈ N exists such that
- which in turn means:
- or
- Let's now consider the matrix
- Then, obviously,
- and so, by the previous theorem, is not bounded.
- This means a natural number N2 ∈ N exists such that
- which in turn means:
- or
- Taking
- and putting it all together, we obtain:
- which, by definition, is
Gelfand's formula leads directly to a bound on the spectral radius of a product of finitely many matrices, namely assuming that they all commute we obtain
Actually, in case the norm is consistent, the proof shows more than the thesis; in fact, using the previous lemma, we can replace in the limit definition the left lower bound with the spectral radius itself and write more precisely:
- which, by definition, is
Example: Let's consider the matrix
whose eigenvalues are 5, 10, 10; by definition, its spectral radius is ρ(A)=10. In the following table, the values of for the four most used norms are listed versus several increasing values of k (note that, due to the particular form of this matrix,):
k | |||
1 | 14 | 15.362291496 | 10.681145748 |
2 | 12.649110641 | 12.328294348 | 10.595665162 |
3 | 11.934831919 | 11.532450664 | 10.500980846 |
4 | 11.501633169 | 11.151002986 | 10.418165779 |
5 | 11.216043151 | 10.921242235 | 10.351918183 |
10 | 10.604944422 | 10.455910430 | 10.183690042 |
11 | 10.548677680 | 10.413702213 | 10.166990229 |
12 | 10.501921835 | 10.378620930 | 10.153031596 |
20 | 10.298254399 | 10.225504447 | 10.091577411 |
30 | 10.197860892 | 10.149776921 | 10.060958900 |
40 | 10.148031640 | 10.112123681 | 10.045684426 |
50 | 10.118251035 | 10.089598820 | 10.036530875 |
100 | 10.058951752 | 10.044699508 | 10.018248786 |
200 | 10.029432562 | 10.022324834 | 10.009120234 |
300 | 10.019612095 | 10.014877690 | 10.006079232 |
400 | 10.014705469 | 10.011156194 | 10.004559078 |
1000 | 10.005879594 | 10.004460985 | 10.001823382 |
2000 | 10.002939365 | 10.002230244 | 10.000911649 |
3000 | 10.001959481 | 10.001486774 | 10.000607757 |
10000 | 10.000587804 | 10.000446009 | 10.000182323 |
20000 | 10.000293898 | 10.000223002 | 10.000091161 |
30000 | 10.000195931 | 10.000148667 | 10.000060774 |
100000 | 10.000058779 | 10.000044600 | 10.000018232 |
Spectral radius of a bounded linear operator
For a bounded linear operator A and the operator norm ||·||, again we have
Spectral radius of a graph
The spectral radius of a graph is defined to be the spectral radius of its adjacency matrix.