SU(2)

Introduction

From here.
The simplest compact Lie group is the circle S1SO(2). Part of the reason it is so simple to understand is that Euler’s formula gives an extremely nice parameterization eix=cosx+isinx of its elements, showing that it can be understood either in terms of the group of elements of norm 1 in C (that is, the unitary group U(1)) or the imaginary subspace of C.
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In the case of SU(2) we have a total analogy, with C replaced by the quaternions H. First, S3SU(2). And SU(2) is isomorphic to the group of elements of norm 1 in H, and there is an exponential map from the imaginary subspace of H to this group.
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Composing with the double cover SU(2)SO(3) lets us handle elements of SO(3) almost as easily as we handle elements of SO(2).

Definition

See also this.

It consists of 2x2 complex matrices of the form

U=[a+idc+ibc+ibaid]

with a2+b2+c2+d2=1. They are unitary (UU=I).
These matrices can be decomposed as

U=aId+biσx+ciσy+diσz,

where σx,σy,σz are the Pauli matrices. Since iσx,iσy,iσz satisfy the same relation that the basis quaternions i,j,j, the group SU(2) is in correspondence with unitary quaternions. The whole set of quaternions is not U(2), but the set of matrices satisfying MMR, i.e., a multiple of identity, and det(M)0. From here.

Topologically, SU(2) is the 3-sphere.

Related: relation SO(3) and SU(2).

Representations of SU(2)

There is exactly 1 irreducible representation of SU(2) in GL(n,C) for every nN. See this video. SU(2)
According to @baez1994gauge page 174, physicists call to the representation of SU(2) of dimension n the spin-j representation, with j=(n1)/2.
To reconcile this with the mathematician language: SU(2) is the spin group corresponding to SO(3). The representations of SU(2) of odd dimension (j=0,1,2,) descend to a representation of SO(3) (said in @baez1994gauge page 180) so they are not spin representations. But in the case of even dimension (j=12,32,52,), it doesn't descend, so it is indeed a proper spin representation.

The Lie algebra

What is the Lie algebra of SU(2)?

Observe that if A(0)=Id, then ddetA(t)dt|t=0=trA(0) (it can be shown expanding by minors).
Then, if det(A(t))=1,
trA(0)=0
So the Lie algebra su(2) consists of anti-Hermitian traceless matrices.

Any anti-Hermitian matrix can be written as
[i(a+d)c+ibc+ibi(ad)]=
=a[i00i]+b[0ii0]+c[0110]+d[i00i]=
=ai1+bi+cj+dk
and it is traceless if and only if a=0, so su(2) corresponds to R3, and so with so(3), the Lie algebra of SO(3).
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These generators
[0ii0],[0110],[i00i]
are the Pauli matrices multiplied by i.