§ Representation theory of SU(2) [TODO ]
-
2x2
unitary matrices, so AA†=I. - Lie algebra is su(2), which are of the form A†=−A, and Tr(A)=0.
- We write Mv≡[ix−y+izy+iz−ix].
- The group elements are matrices, so this is the standard representation, which goes from SU(2) to GL(2,C). Turns out this is irreducible, 2D complex representation.
- We have a transformation which for a g∈SU(2) creates a map which sends a matrix Mv to gMvg−1. so the representation is g↦λMv.gMvg−1, which has type signature SU(2)→GL(su(2)). This is a 3D, real representation: the vectors Mv have 3 degrees of freedom.
- We like complex representations, so we're going to build SU(2)→GL(su(2)⊗C).
- There is the trivial representation λg.(1).
- There is a zero dimensional representation λg.() which maps ⋆∈C0 to ⋆. So it's the identity transformation on C0.
§ Theorem
For any integer n there is an irrep Rn:SU(2)→GL(n,C). Also, any irrep R:SU(2)→GL(v) is isomorphic to one of these.
§ New representations from old
- If we have R:G→GL(V) and S:G→GL(W), what are new representations?
- For one, we can build the direct sum R⊕S. But this is useless, since we don't get irreps.
- We shall choose to take tensor product of representations.
- Symmetric power of R:G→GL(V) is R⊗n:G→GL(V⊗n). This is not irreducible because it contains a subrep of symmetric tensors .
- Example, in C2⊗C2, we can consider e1⊗e1, e2⊗e2, and e1⊗e2+e2⊗e1.
- Define Av (for averaging) of v1⊗v2…vn to be 1/n!∑σ∈Snvσ(1)⊗vσ(2)…vσ(n). In other words, it symmetrizes an input tensor.
- Define Symn(V)=Im(Av:V⊗n→V⊗n). We claim that Symn(V) is a suprep of V. We do this by first showing that Av is a morphism of representations, and then by showing that the image of a morphism is a sub-representation.
§ Weight space decomposition
- SU(2) contains a subgroup isomorphic to U(1). Call this subgroup T, which is of the form [eiθ00e−iθ].