The short answer: Inertial forces don't obey Newton's third law. There are no inertial forces in an inertial frame of reference, and that's where Newton's third law applies.
Consider two observers of some events. One of the observers is inertial, the other is rotating at a nonzero rate with respect to the first. Suppose the inertial observer sees an object moving along a straight line trajectory at a constant velocity. The inertial observer will correctly deduce that the object is subject to zero net force.
The rotating observer will see the object moving along a curved trajectory, possibly with a non-constant speed. If that observer insists on explaining that observed motion via F=ma, that perceived acceleration can only be attributed a non-zero external force. The problem: There is no third law counterpart to that force. It's solely a consequence of (mis)using Newton's second law to explain that motion.
Let's add a third non-inertial observer who is rotating differently than the second one. This observer will also see a non-zero acceleration, but different from that of the second. That means the force is different from that inferred by the second observer.
One way to look at fictitious forces is that they are figments of the observer's imagination. They don't exist. Another way to look at them is that they are a mere misapplication of Newton's second law. Newton's second law is properly a concept that applies in inertial frames only.
A third way to look at fictitious forces is that while they might be figments of ones imagination, they are extremely useful figments. Just try to model the weather from the perspective of a non-rotating, non-accelerating frame. Good luck! On the other hand, this task, while difficult, is doable when viewed from the perspective of a frame rotating with the Earth.