Similar Matrices
25.1 Similar Matrices
One of the major generator of a positive definite matrix is when we square one. In a nutsheel, the matrix \(A^TA\) is always positive definite. To prove this, let \(A\) be a \(m \times n\) rectangular matrix. Then \(A^TA\) is a square symmetric matrix. If we evaluate the expression \(x^T(A^TA)x\), we get \(x^T(A^TA)x = (x^TA^T)(Ax) = (Ax)^T(Ax) = |Ax|^2 > 0\) if \(Ax\) is non-zero. Another important thing to note is if matrix \(A, B\) are positive definite, \(A+B\) is positive definite.
Matrices \(A\) and \(B\) are similar if for some invertible matrix \(M\), \(B=M^{-1}AM\). One of the examples is the eigen value matrix \(\Lambda\). As we know that for any matrix \(A\), \(S^{-1}AS = \Lambda\). This means \(A\) is similar to \(\Lambda\) where \(M=S\). Let’s take an example, where
\[\begin{align} A = \begin{bmatrix} 2 & 1 \\ 1 & 2 \end{bmatrix};\Lambda = \begin{bmatrix} 3 & 0 \\ 0 & 1 \end{bmatrix} \end{align}\]We can find a lot of values of \(M\) and hence \(B\) and one of it is as follows:
\[\begin{align} \begin{bmatrix} 1 & -4 \\ 0 & 1 \end{bmatrix}\begin{bmatrix} 2 & 1 \\ 1 & 2 \end{bmatrix}\begin{bmatrix} 1 & 4 \\ 0 & 1 \end{bmatrix}=\begin{bmatrix} -2 & -15 \\ 1 & 6 \end{bmatrix} = B \end{align}\]The most important fact about similar matrices is that they have the same eigenvalues.
25.2 Why Similar Matrices have same Eigenvalues?
Let \(A\) and \(B\) are similar matrices and \(\lambda\) is one of the eigen values of \(A\). Then, \(Ax = \lambda x\) and \(B = M^{-1}AM\). We can write \(Ax\) as \(Ax = AIx = AMM^{-1}x = \lambda x\). Multiplying by \(M^{-1}\) on the both side, we get \(M^{-1}AMM^{-1}x = \lambda M^{-1}x \implies (M^{-1}AM)M^{-1}x = \lambda M^{-1}x \implies BM^{-1}x = \lambda M^{-1}x \implies B(M^{-1}x) = \lambda (M^{-1}x)\). Hence \(\lambda\) is alse an eigenvalue of \(B\) with \(M^{-1}x\) being it’s eigenvector. Hence, Similar Matrices have the same eigenvalues with the eigenvectors moved around.
25.3 Non-diagonalizable Matrix and Jordan Form
Let the eigenvalues of \(A\) are same. For example, let us say \(\lambda_1 = \lambda_2 = 4\). In this case, one family of similar matrices is just the matrix \(\begin{bmatrix} 4 & 0 \\ 0 & 4 \end{bmatrix}\) as for all \(M\), \(M^{-1}\begin{bmatrix} 4 & 0 \\ 0 & 4 \end{bmatrix}M = \begin{bmatrix} 4 & 0 \\ 0 & 4 \end{bmatrix}\).
Another family of similar matrices will have matrices in the form of \(\begin{bmatrix} 4 & 1 \\ 0 & 4 \end{bmatrix}, \begin{bmatrix} 4 & 0 \\ 17 & 4 \end{bmatrix}, \begin{bmatrix} 5 & 1 \\ -1 & 3 \end{bmatrix}\), where the first matrix representing the simplest (the best we can get to a diagonal matrix) matrix in the family. This matrix is called in the Jordan Form. A matrix in the Jordan Form can be divided into Jordan Blocks and each Jordan Block has one eigenvalue in it. In a nutshell, every square matrix \(A\) is similar to a Jordan Matrix \(J\) with \(n\) Jordan Blocks where \(n\) is the number of eigenvalues of \(A\), as we have one eigenvalue per Jordan Block. When the matrix \(A\) is diagonalizable, i.e. it has distinct eigenvalues, then \(J = \Lambda\).