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 polynomialZero, if present, contributes one factor . Hence the real minimal polynomial isThe 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.
The adjoint on an inner product space is characterized byHere is a finite-dimensional construction that supplies every required basis fact. If is any basis, its coordinate linear functionals form a basis of : a linear functional is uniquely specified by its values on these vectors. Hence . The linear mapis injective, because implies , and positive definiteness implies . Equal dimensions make an linear isomorphism. If is the dual map, thenThis establishes existence and linearity. If two possible vectors represent the same linear functional through the inner product, then , so . Applied to every argument, this proves uniqueness of the adjoint on an inner product space.
For linear maps , two applications of the defining inner product identity giveUniqueness therefore gives . Likewise , for real , and . An induction gives , and applying additivity to a polynomial with real coefficients givesSymmetry of the real inner product also gives . If is the minimal polynomial of , the displayed identity gives , so the minimal polynomial of divides . Applying the same argument to gives reverse divisibility. Both polynomials are monic, hence their minimal polynomials are equal.
The distinct eigenvalues are exactly the roots of the minimal polynomial in the chosen field. An eigenvector with eigenvalue satisfies , so . Conversely, if and were a linear isomorphism, then would imply , contradicting minimal degree. Thus is not injective, giving an eigenvector. It follows that and have the same distinct eigenvalues. This includes the complex eigenvalues after complexification of a real vector space; over the real field it states equality of their real eigenvalues.
Past exam of the groups and representations course of the University of Oxford 2024 3 c Solution 2026-10-25
The change of variables in b diagonalizes the complexified action into and . Consequently the conventional complex branching rule isPrecisely, this is a statement about the complexification of a real vector space carrying the real defining representation. Over the real numbers, the six-dimensional space is the realification of a complex representation ; the conjugate summands above are not separate three-dimensional real invariant subspaces.
The block embedding fixes the seventh coordinate. It adds a trivial representation, givingThe dimensions are complex dimensions after complexification of a real vector space, or equivalently as real dimensions before it.
Realification of a complex representation 2026-10-20
A complex group representation defines a real representation on by viewing each complex coordinate as its real and imaginary parts. In grouped coordinates its matrices are the realification of a complex matrix shown in the title. Direct block multiplication gives and , proving the representation property and preservation of invertibility.
Taking the trace gives its character . After complexification of a real vector space, this realification splits as the original representation and its conjugate. Realification need not preserve irreducibility: the answer depends on whether the irreducible complex representation has real, complex or quaternionic representation type. The standard two-dimensional complex representation of the quaternion group gives a four-dimensional real example with character four at the identity, minus four at its central negative identity, and zero at the other six elements.