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Special Orthogonal Group 📂Representation Theory

Special Orthogonal Group

Definition

Denote by $\operatorname{SO}(n)$ the set of $n \times n$ orthogonal matrices whose determinant is $+1$, and call it the $n$-dimensional special orthogonal group.

$$ \operatorname{SO}(n) := {\left\{ A \in M_{n \times n}(\mathbb{R}) : AA^{T} = I \quad\text{and}\quad \det(A) = +1 \right\}} $$

Explanation

Basically, orthogonal matrices have determinant either $+1$ or $-1$. Among these, those with determinant $+1$ are rotation matrices, so the special orthogonal group is the set of rotation matrices. Hence it is also called the rotation group. In low dimensions the special orthogonal groups are as follows.

  • $\operatorname{SO}(1) \cong \left\{ 1 \right\}$
  • $\operatorname{SO}(2) \cong$ $S^{1}$
  • $\operatorname{SO}(3) \cong \mathbb{P}^{3}$

Note that $\operatorname{SO}(2)$ is $1$-dimensional, whereas $\operatorname{SO}(3)$ is $3$-dimensional. Rotations in the plane can be expressed with $1$ parameters, while $3$-dimensional space is formed from three planes (the $xy–$ plane, the $yz–$ plane, and the $zx–$ plane), so $3$ parameters are required.

Two dimensions

The 2-dimensional rotation group $\operatorname{SO}(2)$ is concretely given by:

$$ \operatorname{SO}(2) = \left\{ \begin{bmatrix} \cos \theta & -\sin \theta \\ \sin \theta & \cos \theta \end{bmatrix} : \theta \in \mathbb{R} \right\} $$

This is isomorphic to the points on the unit circle.

$$ \operatorname{SO}(2) \cong S^{1} $$