Let be the space of homogeneous degree- polynomials in . For and a column vector , define
Substitution preserves degree, and
so is a continuous representation of a topological group. This is the homogeneous polynomial representation of SU2.
To prove irreducibility, restrict to the diagonal circle
The monomials are its one-dimensional weight spaces, with distinct weights up to our harmless inverse-action convention. If is invariant, Fourier projection along this circle shows that contains a monomial. Differentiating the action of and complexifying gives the operators
Repeated applications of and connect every monomial to every other one. Hence contains the entire monomial basis, so .
Every is conjugate to with . Reading the eigenvalues on the monomial basis gives the character of the homogeneous polynomial representation of SU2
For this is
with the values at obtained by continuity.
For completeness, let be any finite-dimensional irreducible continuous complex representation of . Its restriction to the diagonal circle splits into integral weight spaces. Choose a vector of largest weight . The raising operator kills it, and the commutation relations show that is a nonnegative integer and that successive applications of the lowering operator form a string of weights
Their span is an invariant copy of ; irreducibility forces it to equal . Thus the classification of finite-dimensional representations of SU2 says
If the eigenvalues of are , then the eigenvalues on are for . Therefore the character of an exterior square is
The exterior square of an SU2 irreducible representation or the Clebsch-Gordan decomposition for SU2 with flip parity gives
The dimensions check the result.
The third elementary symmetric polynomial in the , together with Newton identities, gives
For the five-dimensional representation , the canonical duality
finishes the decomposition. The weights sum to zero, so is trivial, and every irreducible is self-dual. Consequently
Schur lemma says that an intertwining linear map between irreducible finite-dimensional complex representations is either zero or an isomorphism. In particular, every endomorphism of an irreducible complex representation is a scalar multiple of the identity.
A continuous representation of a topological group is a continuous homomorphism
for a finite-dimensional complex vector space . It is a unitary representation if has a positive-definite Hermitian inner product for which
for every and .
For , start with any positive-definite Hermitian form and average it using normalized Haar measure:
Translation invariance makes this form -invariant, and positivity is preserved, proving unitarity. Since is abelian, the operators commute; since they are unitary, they are normal. Simultaneous diagonalization therefore decomposes into common one-dimensional eigenspaces. Thus every representation of the circle group is a direct sum of one-dimensional representations.
Write
The group law and inverse are
A calculation gives
Every element of the centre occurs by taking, for example, and . Hence the commutator subgroup is exactly . The image of a one-dimensional representation is abelian, so the one-dimensional representation kills the commutator subgroup and its kernel contains .
Now let be a complex representation of . Its restriction to the central subgroup
is a representation of the circle group. Decompose it into its distinct weight spaces:
Because is central, every commutes with its action and preserves every common eigenspace. Thus the are -subrepresentations, as asserted by the central circle weight-space decomposition.
Let . The map
is a one-dimensional representation of ; after composition with , its kernel contains . On its value is
so . A continuous character of has the form ; the displayed identity forces . Therefore every is trivial. Since the were distinct, and .
It follows that every finite-dimensional complex representation of kills the entire nontrivial central circle . Its kernel is therefore nontrivial, so no such representation is faithful. This is the real Heisenberg quotient has no faithful finite-dimensional representation.