In order to calculate the Dirac spectrum on Berger's sphere $(S^3,g_t)$, I came across irreps of SU(2) (see Hitchin p. 30).
Apperently, Hitchin restricts the Dirac operator to the eigenspaces of the Laplacian relative to the standard metric because they commute. That's clear. Now he says, that they are given by irreps of SU(2), ie. homogeneous polynomials in two complex variables. And that's the part I do not understand.
The eigenspaces of the corresponding Laplacian on $S^3$ are given by harmonic homogeneous polynomials all with respect to the Euclidean $\mathbb{R}^4$, aren't they? So why does he talk about just homogeneous polynomials without the harmonic restriction?
I already consulted Bröcker and Hall and cannot find anything helpful.
Obviously, I don't understand the connection between Laplace eigenspaces and irreps and definitely miss something. Maybe it's a silly question. But unfortunately, I don't get the point. So I would appreciate some help.
Thank you! :)
EDIT: I worked up a little and come to the conclusion that the Peter-Weyl theorem is the key point here. It seems that the functions given by the matrix coefficents
\begin{align} g \mapsto f_{v,w}(g) = \left< \pi_k(g)v,w\right> \end{align}
on the irreps $\pi_k$ of SU(2), namely homogeneous polynomials in two complex variables of degree $k$, must give the spherical harmonics I'm seeking for. Can anybody confirm this?
My intuition in the last edit is indeed true. You can find the solution in Folland's book "A Course in Abstract Harmonic Analysis", p. 155. Thank you anyway! :)