A deformation quantization, in the sense of Rieffel, was recently achieved for de-Sitter spacetime. In this work, we generalize these results to all globally hyperbolic spacetimes and apply the deformation to quantum field theories and their respective states. It turns out that the deformed state (i.e. a state in non-commutative spacetime) has a singularity structure resembling Minkowski, i.e. is Hadamard, if the undeformed state is Hadamard. This proves that the Hadamard condition, and hence the quantum field theoretical implementation of the equivalence principle is a general concept that even holds in spacetimes with quantum features (i.e. a non-commutative spacetime).