Use the convention
for the characteristic polynomial. Choosing instead multiplies it by and leaves the requested zero identity unchanged. For each eigenvector , induction gives , including . Thus
because has the nonzero kernel vector and therefore has zero determinant. Part (a) supplies a basis consisting of these eigenvectors. A linear map vanishing on every basis vector vanishes everywhere. Consequently
This proves the Cayley-Hamilton theorem identity directly in the distinct-eigenvalue case assumed here.

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