One of the interesting features of the Aharonov-Bohm effect is that it shows some form of non-locality: the wave function of a particle is influenced by a magnetic (or electric) field even though the particle is never located where the field is non-zero.
To derive the effect, one considers a semi-classical system: the particle's degrees of freedom are fully quantum, but the magnetic field is just a non-dynamic background.
So it seems to me that the non-locality cannot be considered fundamental in any sense, since a full quantum description would include the quantized electromagnetic field, and then we would see that all interactions are carried by force-carriers (photons).
Am I right?