Quaternions: The skew field $\mathrm{H}$ of quaternions can be identified with the vector space $\mathbb{R}^4$ equipped with a noncommutative multiplication operation. The standard basis vectors $\mathbf{e}_1, \mathbf{e}_2, \mathbf{e}_3, \mathbf{e}_4$ are traditionally denoted by the letters $1, \mathrm{i}, \mathrm{j}, \mathrm{k} ;$ the vector $(a, b, c, d)^T \in \mathbb{R}^4$ corresponds to the quaternion $q=a+b i+c j+d k$. Quaternion addition coincides with vector addition. Quaternion multiplication is defined so that
$$
1 q=q=q 1, \mathrm{i}^2=\mathrm{j}^2=\mathrm{k}^2=-1, \mathrm{i} \mathrm{j}=\mathrm{k}=-\mathrm{j} \mathrm{i}, \mathrm{i} \mathrm{k}=-\mathrm{j}=-\mathrm{ki}, \mathrm{jk}=\mathrm{i}=-\mathrm{k} \mathrm{j},
$$
along with the distributive laws
$$
(q+r) s=q s+r s, \quad q(r+s)=q r+q s, \quad \text { for all } \quad q, r, s \in \mathbb{H} \text {. }
$$