Special Unitary Group - n = 2

n = 2

SU(2) is the following group:

where the overline denotes complex conjugation. Now consider the following map:

where M(2, C) denotes the set of 2 by 2 complex matrices. By considering C2 diffeomorphic to R4 and M(2, C) diffeomorphic to R8 we can see that φ is an injective real linear map and hence an embedding. Now considering the restriction of φ to the 3-sphere, denoted S3, we can see that this is an embedding of the 3-sphere onto a compact submanifold of M(2, C). However it is also clear that φ(S3) = SU(2). Therefore as a manifold S3 is diffeomorphic to SU(2) and so SU(2) is a compact, connected Lie group.

The Lie algebra of SU(2) is:

It is easily verified that matrices of this form have trace zero and are antihermitian. The Lie algebra is then generated by the following matrices

 u_1 = \begin{pmatrix}
0 & i\\
i & 0
\end{pmatrix}
\qquad
u_2 = \begin{pmatrix}
0 & -1\\
1 & 0
\end{pmatrix}
\qquad
u_3 = \begin{pmatrix}
i & 0\\
0 & -i
\end{pmatrix}

which are easily seen to have the form of the general element specified above. These satisfy u3u2 = −u2u3 = −u1 and u2u1 = −u1u2 = −u3. The commutator bracket is therefore specified by

The above generators are related to the Pauli matrices by u1 = i σ1,u2 = −i σ2 and u3 = i σ3. This representation is often used in quantum mechanics (see Pauli matrices and Gell-Mann matrices), to represent the spin of fundamental particles such as electrons. They also serve as unit vectors for the description of our 3 spatial dimensions in loop quantum gravity.

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