Use the convention that the inner product is conjugate-linear in its first argument and linear in its second, as in part (b). The adjoint operator is characterized by
Existence and uniqueness follow from the finite-dimensional representation of linear functionals by the inner product. More concretely, choose an orthonormal basis and let . Then
which defines uniquely and verifies the required identity by expansion in that basis. Thus its matrix is the conjugate transpose, proved here rather than assumed. A self-adjoint operator satisfies , equivalently for every pair of vectors.

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