A rigid motion of $\mathbb {R^{n}}$ is a map
$M = T ◦ R : \mathbb {R^{n}} \to \mathbb {R^{n}}$
where $ \mathbb {R^{n}} \to \mathbb {R^{n}} $ is linear and satisfies $|R(v)| = |v| \space \space \space \space \space \space ∀v \in \mathbb {R^{n}}$
And T : $ \mathbb {R^{n}} \to \mathbb {R^{n}} $ is translation, i.e. there exists $ w \in \mathbb {R^{n}}$ such that $T (v) = v + w$ $\space \space \space \space \space∀v \in \mathbb {R^{n}} $
Argue that the function R is represented by a matrix $ R(v) = A(v)$ where A is n x n and satisfies $ A^T A = I $
Im not really familiar with rotational mappings but in Dynamical Systems we used rotational and translation matrices to move solutions around.
How do i argue that a rotational map is the same thing as a rotation matrix?