30.3: The Power of a Matrix
- Page ID
- 69507
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\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)- For a diagonalizable matrix \(A\), we have \(C^{-1}AC = D\). Then we have \(A = CDC^{-1}\)
- We have \(A^2 = CDC^{-1}CDC^{-1} = CD^{2}C^{-1}A^{n} = CDC^{-1} \ldots CDC^{-1} = CD^{n}C^{-1}\).
- Because the columns of \(C\) are eigenvectors, so we can say that the eigenvectors for \(A\) and \(A^n\) are the same if \(A\) is diagonalizable.
- If \(x\) is an eigenvector of \(A\) with the corresponding eigenvalue \(\lambda\), then \(x\) is also an eigenvector of \(A^n\) with the corresponding eigenvalue \(\lambda^n\).
Graph Random Walk
- Define the following matrices:
- \(I\) is the identity matrix
- \(A\) is the adjacency matrix
- \(D\) is diagonal matrix of degrees (number of edges connected to each node)
\[W=\frac{1}{2}(I + AD^{-1}) \nonumber \]
- The lazy random walk matrix, \(W\), takes a distribution vector of stuff, \(p_t\), and diffuses it to its neighbors:
\[p_{t+1}=Wp_{t} \nonumber \]
- For some initial distribution of stuff, \(p_0\), we can compute how much of it would be at each node at time, \(t\), by powering \(W\) as follows:
\[p_{t}=W^{t}p_{0} \nonumber \]
- Plugging in the above expression yields:
\[p_{t}=\left( \frac{1}{2}(I+AD^{-1}) \right)^t p_{0} \nonumber \]
Using matrix algebra, show that \(\frac{1}{2}(I + AD^{-1})\) is similar to \(I-\frac{1}{2}N\), where \(N=D^{-\frac{1}{2}}(D-A)D^{-\frac{1}{2}}\) is the normalized graph Laplacian.
Random Walk on Barbell Graph
To generate the barbell graph, run the following cell.
Generate the lazy random walk matrix, \(W\), for the above graph.
Compute the eigenvalues and eigenvectors of \(W\). Make a diagonal matrix \(J\) with the eigenvalues on the diagonal. Name the matrix of eigenvectors \(V\) (each column is an eigenvector).
Now we make sure we constructed \(V\) and \(A\) correctly by double checking that \(W = VJV^{-1}\)
Let your \(p_0 = [1,0,0, \ldots, 0]\). Compute \(p_t\) for \(t = 1,2,\ldots,100\), and plot \(||v_1 - p_t||_1\) versus \(t\), where \(v_1\) is the eigenvector associated with the largest eigenvalue \(\lambda_1 = 1\) and whose sum equals 1. (Note: \(||\cdot||_1\) may be computed using np.linalg.norm(v_1-p_t, 1)
.)
Compare to Complete Graph
If you complete the above, do the same for a complete graph on the same number of nodes.
What do you notice about the graph that is different from that above?