My professor is talking about how Lorentz boosts do not commute and how it relates to Thomas Precession, but I am struggling to wrap my head around the implications of that and how it works. Also confused about how commutation in general is applied to areas other than quantum mechanics.
Asked
Active
Viewed 1,327 times
1 Answers
5
Boosts are proper Lorentz transformations, so are rotations (defined herein as determinant-$1$ metric-preserving linear transformations) in Minkowski spacetime. Just like rotations in Euclidean space, the order matters.
Consider a vector pointing along $x$. If you rotate about $x$, it does nothing. So if you rotate about $x$ and then about $y$ you get a different outcome than if you rotate about $y$ and then $x$.
This is the physical interpretation. A boost is legitimately a rotation in spacetime.