For a Hermitian operator , every eigenvalue is real. Indeed, if with , self-adjointness gives . To prove the finite-dimensional spectral theorem, proceed by induction on the dimension. The fundamental theorem of algebra supplies a root of the characteristic polynomial, hence a unit eigenvector . Its orthogonal complement is invariant: for , . The restriction of to that complement is again Hermitian. Induction supplies an orthonormal basis of eigenvectors there; adjoining gives an orthonormal eigenbasis of the whole space. The zero-dimensional case is immediate. Consequently a Hermitian operator is diagonal in an orthonormal basis, with real diagonal entries.
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