Question

(a) Show that the spectral radius of $T=\left(\begin{array}{ll}1 & 1 \\ 0 & 1\end{array}\right)$ is $\rho(T)=1$. (b) Show that most iterates $\mathbf{u}^{(k)}=T^k \mathbf{u}^{(0)}$ become unbounded as $k \rightarrow \infty$. (c) Discuss why the inequality $\left\|\mathbf{u}^{(k)}\right\| \leq C \rho(T)^k$ does not hold when the coefficient matrix is incomplete. $(d)$ Can you prove that $(9.28)$ holds in this example?

   (a) Show that the spectral radius of $T=\left(\begin{array}{ll}1 & 1 \\ 0 & 1\end{array}\right)$ is $\rho(T)=1$.
(b) Show that most iterates $\mathbf{u}^{(k)}=T^k \mathbf{u}^{(0)}$ become unbounded as $k \rightarrow \infty$.
(c) Discuss why the inequality $\left\|\mathbf{u}^{(k)}\right\| \leq C \rho(T)^k$ does not hold when the coefficient matrix is incomplete. $(d)$ Can you prove that $(9.28)$ holds in this example?
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Applied Linear Algebra (Undergraduate Texts in Mathematics)
Applied Linear Algebra (Undergraduate Texts in Mathematics)
Peter J. Olver,… 2nd Edition
Chapter 9, Problem 5 ↓

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To find the spectral radius $\rho(T)$, we first need to find the eigenvalues of the matrix $T$. The eigenvalues $\lambda$ of a matrix $T$ are found by solving the characteristic equation $\det(T - \lambda I) = 0$, where $I$ is the identity matrix. For the matrix  Show more…

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(a) Show that the spectral radius of $T=\left(\begin{array}{ll}1 & 1 \\ 0 & 1\end{array}\right)$ is $\rho(T)=1$. (b) Show that most iterates $\mathbf{u}^{(k)}=T^k \mathbf{u}^{(0)}$ become unbounded as $k \rightarrow \infty$. (c) Discuss why the inequality $\left\|\mathbf{u}^{(k)}\right\| \leq C \rho(T)^k$ does not hold when the coefficient matrix is incomplete. $(d)$ Can you prove that $(9.28)$ holds in this example?
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Key Concepts

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Spectral Radius
The spectral radius of a matrix is defined as the maximum absolute value among its eigenvalues. This concept is crucial because it determines asymptotic behaviors of matrix powers – if the spectral radius is less than one, iterates tend to zero, and if it is greater than one, they tend to become unbounded. Even when the spectral radius is equal to one, additional structural properties of the matrix can affect stability and boundedness of iterates.
Jordan Blocks and Defective Matrices
A matrix that has a repeated eigenvalue and lacks a complete basis of eigenvectors is said to be defective. Such matrices are typically represented in Jordan canonical form where the presence of a Jordan block (with superdiagonal ones) indicates non-diagonalizability. This structure can lead to growth in the powers of the matrix even when the spectral radius is one, as the nilpotent part of the Jordan block can induce polynomial (rather than exponential) growth in the iterates.
Iterative Methods and Matrix Powers
Analyzing the iterates produced by applying a matrix repeatedly to an initial vector is a central topic in iterative methods. The behavior of these iterates is determined by both the eigenvalues and the structure of the matrix. In cases where the matrix is defective, even if all eigenvalues lie on the unit circle (i.e., spectral radius equals one), some non?eigenvector directions can grow unbounded due to contributions from the Jordan blocks.
Matrix Norm Inequalities and Their Limitations
Matrix norm inequalities such as ?u^(k)? ? C ?(T)^k provide a bound on the growth or decay of iterates in terms of the spectral radius. However, these inequalities generally assume that the matrix has a full set of eigenvectors or that it is diagonalizable. In the context of incomplete matrices (or defective matrices), the additional growth induced by the nilpotent Jordan block cannot be captured purely by the spectral radius, which leads to a breakdown of this simple exponential bound.
Proof Techniques for Norm Bounds in Non?Diagonalizable Cases
To analyze and provide rigorous bounds on iterates for non?diagonalizable matrices, one must typically use techniques that account for the Jordan structure of the matrix. This involves showing that the norm of the matrix raised to the k-th power grows at most polynomially in k times the spectral radius raised to the k-th power. Establishing such results often requires careful estimates that combine the effects of the eigenvalue magnitudes with the contributions from the nilpotent parts of the matrix.

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