In the framework of quantum field theory (QFT) on noncommutative (NC)
space-time with the symmetry group O(1,1)×SO(2), we prove that the
Jost-Lehmann-Dyson representation, based on the causality condition taken in
connection with this symmetry, leads to the mere impossibility of drawing any
conclusion on the analyticity of the 2→2-scattering amplitude in
cosΘ, Θ being the scattering angle. Discussions on the possible
ways of obtaining high-energy bounds analogous to the Froissart-Martin bound on
the total cross-section are also presented.Comment: 25 page