The Jordan–Chevalley decomposition is characterized byOver , a semisimple linear operator is a diagonalizable one. These conditions determine the two parts uniquely. Concretely, on the generalized eigenspace for an eigenvalue , the semisimple part is and the nilpotent part is ; both are polynomials in . To see uniqueness, any commuting candidate parts preserve each generalized eigenspace; diagonalize the proposed semisimple part there, and nilpotence then forces its eigenvalue to be the sole eigenvalue of on that space.
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