It is well know that QFT predicts that an accelerated observer would see Unruh radiation. This is related to the presence of a Rindler horizon and leads to the conclusion that an inertial and an accelerated vacuum are different.
Why can't we naively apply the equivalence principle and say that a static observer under a gravitational field? In this case there could be no horizon and the argument would fail. But I'm not sure why the equivalence principle doesn't work. Maybe the particle concept is a global one?