The dual basis is the collection of linear functionals characterized by
Explicitly, . Every linear functional satisfies , proving that the displayed functionals span the dual space. Evaluating a zero linear combination at each makes all its coefficients zero, so they are also linearly independent. Thus they form a basis of .
Define the bidual evaluation map by evaluation:
For fixed , this is a linear functional of , so it belongs to the double dual. It is also linear as a function of . If , some coordinate of in a basis is nonzero, and the corresponding dual basis functional detects it. Hence , proving injectivity.
The spaces all have the same finite dimension. Therefore an injective linear map is surjective, proving the required linear isomorphism.
This linear isomorphism is natural because evaluation requires no basis. More explicitly, for any linear map , its dual map satisfies
so .
Writing and , evaluation against the dual basis gives
This has codomain , not the printed . For a nonzero vector space, take and to obtain . Only the diagonal values must be real. The displayed formula defines the intended complex inner product.
It is linear in the first argument and conjugate-linear in the second:
It has conjugate symmetry, since . Finally,
with equality exactly when every coordinate vanishes, equivalently . This proves positive definiteness. Since , the original basis is orthonormal. This is the inner product determined by a basis.
Use the convention of part (a): the inner product is linear in its first argument. If with , the adjoint operator identity and give
Positive definiteness makes , so
Thus every eigenvalue of a skew-adjoint operator is purely imaginary, including zero.
Take and . Because is an invariant subspace, . The adjoint operator relation yields
This holds for every , so . Therefore the orthogonal complement is also an invariant subspace.
Proceed by induction on the dimension. For positive dimension, the fundamental theorem of algebra gives a root of the characteristic polynomial, hence a nonzero eigenvector . Normalize it to have norm one. Its span is an invariant subspace, and part (ii) makes its orthogonal complement invariant too:
The restriction of to the complement remains skew-adjoint, since the same inner product identity holds there. The induction hypothesis supplies an orthonormal eigenbasis for that smaller space. Adjoining gives an orthonormal eigenbasis for .
The zero-dimensional base case is immediate. Thus is diagonalizable, indeed unitarily diagonalizable. This proves the finite-dimensional case of the spectral theorem for a skew-adjoint operator without assuming that distinct eigenvalues have multiplicity one.
Regard the real skew-symmetric matrix as acting on . Its Hermitian adjoint is . Parts (i) and (iii) show that its eigenvalues are purely imaginary and its complex minimal polynomial has no repeated roots.
Since has real entries, nonreal eigenvalues occur in conjugate pairs. A nonzero pair has the form , with , and contributes the real quadratic polynomial
Zero, if present, contributes one factor . Hence the real minimal polynomial is
The product annihilates after complexification of a real vector space, so it also annihilates the original real linear map; no factor can be removed because each displayed complex root is an eigenvalue. This proves both the asserted form and its minimality. The case has and an empty product.

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