An accelerometer measures deviation from inertial motion. In relativity, it measures an invariant scalar: proper acceleration, which is the norm of acceleration 4-vector, which is derivative of 4-velocity by proper time.
In the frame of an accelerated object, coordinate acceleration is zero, as is coordinate velocity. However, 4-velocity, 4-acceleration, and proper acceleration are not zero.
Relativistic momentum applies to inertial observers and inertial bodies as well as accelerating bodies, so your argument doesn't make sense. How do you apply it to the fact that an inertial proton moving at .99 c has 3 times the momentum as one moving at .9c? Any accelerometer moving with each proton would read zero; each proton is stationary in its frame, and everything in its frame is indistinguishable from the lab frame.