General relativity is locally just special relativity. Recall general relativity includes gravity, via curved spacetime, but special relativity excludes gravity and assumes flat spacetime. But as Einstein realised, a person freely falling in a uniform gravitational field wouldn't feel their weight (see the equivalence principle); to them, spacetime is locally flat.
Now consider the relativistic Doppler effect in special relativity. This is a "redshift" of light etc caused by relative motion of two observers -- emitter and receiver. But you can apply the exact same formula to two observers in general relativity. We just require they be at the same event (that is, same place and same time), otherwise it is not clear the effect is due to relative motion alone, and not a gravitational redshift for instance. (My Master's thesis showed the interpretation is somewhat flexible.) The reference frame of each observer is described by a set of orthonormal vectors. Then, with caveats I haven't explained, you can apply results from special relativity.
There are various reasons special relativity is still important. Firstly it is simpler, so if you had some difficult research topic you might want to solve it in this arena before attempting curved spacetime. Another is that quantum physics is unified with special relativity but not general relativity, so the physics is not known. In particle accelerators gravity is not important over the short duration of particle collisions.