The minimal polynomial is the monic polynomial of least polynomial degree such that . Here a polynomial is evaluated at the linear operator by , with the constant term acting as .
An annihilating polynomial exists because lie in the finite-dimensional vector space and are therefore eventually linearly dependent. Uniqueness follows by subtracting two monic annihilators of the same least degree: their difference has smaller degree and still annihilates .
Equivalently,
For the forward implication evaluate the factorization at . For the reverse implication divide by using polynomial division; the remainder annihilates , so minimality makes it zero. This also identifies the annihilating polynomials as the principal ideal generated by .
Suppose . Every vector has the decomposition
If also belongs to , then . Hence
On its image of a linear map, acts as the identity; on its kernel of a linear map, it acts as zero. Concatenate a basis of the image with a basis of the kernel. The resulting matrix is , where .
Conversely, this block matrix squares to itself, so any linear map having that matrix in a basis satisfies . Thus projection operators are precisely the linear maps with this block form. This is an algebraic projection; no inner product or orthogonality is required.
Evaluate Bézout's identity for polynomials at :
All these linear operators commute because they are polynomials in the same operator. Thus every can be written
The first summand belongs to and the second to , since applying the corresponding operator introduces the product .
If lies in both kernels, the same identity gives . Therefore the sum is direct:
This is the kernel decomposition for coprime polynomials. It uses both annihilation by and the coprimality expressed by the Bézout identity.
Write , . The linear operator vanishes on . On , the identity gives .
By the direct sum in part (i), every vector has a unique expression , and
Consequently
The complementary projection operator is , onto along . These are polynomial projections for a coprime decomposition. In particular the projection does not depend on which Bézout coefficients are chosen: its action on the two summands uniquely determines it.
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 satisfy
Put . Both restrictions of vanish, so the direct sum gives
Hence 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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