Looks like $A$ is the matrix of the linear transformation $\vec{x}\mapsto \vec{x}\times (c,b,a)$. Therefore it is the so called infinitesimal generator for the group of rotations around the axis $\vec{n}=(c,b,a)$ (a unit vector!). We get those rotation matrices (in the right handed direction) using the exponential
$$R(\theta)=e^{\theta A},$$
where matrix exponential is defined by the power series
$$
e^X=I_3+\sum_{n=1}^\infty\frac1{n!}X^n.
$$
Of course, $\theta$ is the angle of rotation. If $\vec{n}$ were not a unit vector, the rotations would go at angular speed $\omega=||\vec{n}||$.
Don't know if this makes the matrices special in any way :-(
Basically you are looking at the Lie algebra $\mathfrak{so}(3,\Bbb{R})$. This is in a sense the reason cross products appear frequently when one studies the mechanics of rotations.