Can we define a group operation of pure Lorentz Boosts?
Consider the Lorentz group. By the Wigner rotation, the composition of two pure boosts results in a non-pure boost. However, fortunately a Lorentz group element can always decomposited into a composition of a pure boost and a rotation by polar decomposition theorem, i.e. for any pure boosts $B_1$ and $B_2$ there exists unique pure boost $B_3$ and unique rotation $R$ such that $B_2 \circ B_1 = R \circ B_3$.
I am wondering if we can define a group operation of pure boosts. My thought is that the group operation is defined by $$ B_2 B_1 = B_3 \text{ where } B_2 \circ B_1 = R \circ B_3 \text{ by polar decomposition.} $$ It is a kind of looking like a quotient space of Lorentz group modulo the rotation group, e.g. the oriented hyperbolic space: $SO^+(1, n)/SO(n)$.