The adjoint operator is defined bySince is a nonzero finite-dimensional complex vector space, has an eigenvector with eigenvalue . Normality givesfor every , by expanding both sides and using . Taking yields
For the common eigenvector , its orthogonal complement is invariant under both and . Indeed, if , thenand the analogous calculation applies to . The restriction of to is therefore again normal. Induction on , beginning with the normalized vector , produces an orthonormal eigenbasis. This proves the finite-dimensional spectral theorem for normal operators.
If for a nonzero real vector , then skew-symmetry givesThusso a real skew-symmetric matrix has no nonzero real eigenvalue.
Over , the real skew-symmetric matrix is normal because . Part (a) gives an orthonormal complex eigenbasis, and the nonzero eigenvalues are purely imaginary pairs .
For each , choose a unit real vector in the kernel of and putThen , , andThus has matrixon the orthonormal basis . Distinct such invariant planes are orthogonal; complete them by an orthonormal basis of . Taking these basis vectors as the columns of an orthogonal matrix gives
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