A Hermitian matrix satisfies , where means conjugate transpose. If with , then is real, since it equals its complex conjugate . Thus every eigenvalue is real. To prove the finite-dimensional spectral theorem, choose a unit eigenvector ; one exists because the complex characteristic polynomial has a root. Its orthogonal complement is invariant, since for ,
The restriction to that complement is again Hermitian. Induction on dimension supplies an orthonormal basis of eigenvectors, so for a unitary matrix .
In this basis, . Therefore . In that case the square root of a matrix
is Hermitian, positive definite and satisfies . For uniqueness, any positive-definite Hermitian satisfying commutes with and hence preserves each eigenspace of . Its restriction to the -eigenspace is Hermitian, and its positive eigenvalues all solve . Thus that restriction is , forcing . This is the principal square root of a positive semidefinite matrix, here strictly positive definite.
Now let and . Expanding without assuming that and commute gives
The Hermitian matrix has because , whereas . Hence . If , , then
Since , every real eigenvalue of is positive. The positive-eigenvalue criterion now gives the strict finite-dimensional operator monotonicity of the square root:
Part c gives the integral representation
The integrand vanishes on the diagonal . Thus the assumed off-diagonal Peskun ordering implies
for every .
On the mean-zero subspace, the variational characterization of the spectral gap of a positive reversible kernel is
It follows immediately that
Equivalently, the energy inequality says in the Löwner order on . Positivity permits the operator monotonicity of the square root and hence ; the spectral representations in the question identify the top spectral values and give the same gap inequality.