Since is upper triangular, its eigenvalues are its diagonal entries. Equivalently, its characteristic polynomial is . Hence
For eigenvalue zero take . For eigenvalue , the first row of gives , so take . These are linearly independent eigenvectors, givingThe identities give , hence the required diagonalization .
The Gauss-Seidel method solves each component using the already updated components from the same iteration. In the splitting , those updated diagonal and lower-triangular terms stay on the left, while upper-triangular terms use the previous iterate. ThusHere is lower triangular with nonzero diagonal, so each new iterate is obtained by forward substitution, starting from the specified zero vector.
As , solve . Its first row gives ; its second gives . ThereforeThe second component uses the new first component , distinguishing Gauss-Seidel iteration from Jacobi iteration.
The exact solution obeys . Subtract this from the iteration to get . Hence the stationary iteration matrix isThis is exactly the matrix from part (a); the sign follows the given convention.
Yes. Part (a) diagonalizes , whose spectral radius is . Thusand every initial error converges to zero. For the specified initial vector, solving gives and . In fact,The special formula is not asserted for , because the zero-eigenvalue component disappears only after the first step.
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