Let and . By part (ii), these are complementary projection operators with images and . Thus acts as on and on .
The linear operator preserves both summands because it commutes with its own polynomials. Therefore preserves them too, and its restrictions satisfyPut . Both restrictions of vanish, so the direct sum givesHence is a nilpotent linear map. The operator is diagonalizable, since its two summands are its eigenspaces, and it commutes with . This illustrates the Jordan–Chevalley decomposition in the case of two distinct eigenvalues.
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