I'm not exactly sure what you're asking, but...
General relativity rejects absolute frames of reference.
In Newtonian mechanics, you may have fictitious forces related to gravity and acceleration. In GR, that distinction between real and fictitious forces dissolves rather neatly into a distinction between coordinate-independent (invariant) facts and coordinate-dependent artifacts.
I don’t think that is true. The difference between a real and a fictitious force does not 'dissolve'. Fictitious forces occur when there is a real force of interaction acting on the observer. If the hypothetic observer is in an inertial or free falling frame, then the observer can't observe a fictitious force.
The thrust of a rocket generates a 'proper acceleration' on the spaceman inside. The thrust is a very real force as seen from an inertial frame. This proper acceleration is breaks the symmetry in the so called twin paradox.
Force in relativity impacts reality through proper acceleration. Proper acceleration affects the world line of an observer. In fact, the concept of proper acceleration is necessary to resolve many conundrums in relativity, including the so called twin paradox.
Here is a link on 'proper acceleration'.
https://en.wikipedia.org/wiki/Proper_acceleration
‘In relativity theory, proper acceleration[1] is the physical acceleration (i.e., measurable acceleration as by an accelerometer) experienced by an object. It is thus acceleration relative to a free-fall, or inertial, observer who is momentarily at rest relative to the object being measured. Gravitation therefore does not cause proper acceleration, since gravity acts upon the inertial observer that any proper acceleration must depart from (accelerate from). A corollary is that all inertial observers always have a proper acceleration of zero.
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n situations in which gravitation is absent but the chosen coordinate system is not inertial, but is accelerated with the observer (such as the accelerated reference frame of an accelerating rocket, or a frame fixed upon objects in a centrifuge), then g-forces and corresponding proper accelerations felt by observers in these coordinate systems are caused by the mechanical forces which resist their weight in such systems. This weight, in turn, is produced by fictitious forces or "inertial forces" which appear in all such accelerated coordinate systems, in a manner somewhat like the weight produced by the "force of gravity" in systems where objects are fixed in space with regard to the gravitating body (as on the surface of the Earth).’
The perception that there are no forces in relativity is one of the favorite factoids of the woo woos. Forces are very important in relativity.
Special relativity requires the concept of force just to distinguish inertial frames from accelerating frames. In order to determine whether a reference frame is an inertial frame, one has to demonstrate that the observer associated with that inertial frame has a zero value for proper acceleration. You can’t just assume that a reference frame is inertial.