Any displacement along a line can be written as the sum of two perpendicular displacements, which then form a closed triangle with the total displacement vector.
My question is: Can something similar be done with rotation?
Consider a rotation about a fixed axis. Can this always be decomposed into two rotations about two perpendicular axes, which again form a triangle (or similar) with the total axis of rotation? In other words, if the axis of rotation is inclined such that it has components in $x$ and $y$ with respect to a global coordinate system, will the rotation it permits never involve a rotation about the $z$-axis?
If it is indeed possible to consider rotations in this way, what is the simplest way to decompose the rotation into fractional contributions from these two putative axes?
EDIT (in response to comment):
A "sharpened" version of my "theorem" may read as: Any rotation about a fixed arbitrary axis can be decomposed into a rotation about three orthogonal axes, but not into a rotation about two orthogonal axes."
From the (very helpful) first reply, I surmise this is correct?