We study the propagation of quantum fields on κ-Minkowsi spacetime.
Starting from the non-commutative partition function for a free field written
in momentum space we derive the Feynman propagator and analyze the non-trivial
singularity structure determined by the group manifold geometry of momentum
space. The additional contributions due to such singularity structure result in
a deformed field propagation which can be alternatively described in terms of
an ordinary field propagation determined by a source with a blurred spacetime
profile. We show that the κ-deformed Feynman propagator can be written
in terms of vacuum expectation values of a commutative non-local quantum field.
For sub-Planckian modes the κ-deformed propagator corresponds to the
vacuum expectation value of the time-ordered product of non-local field
operators while for trans-Plankian modes this is replaced by the Hadamard
two-point function, the vacuum expectation value of the anti-commutator of
non-local field operators.Comment: 29 pages, 10 figures; v2: typos corrected, references adde