It is worth noting that the dependence of exciton rotational dynamics on pulse polarization is contingent upon the geometric arrangements of the linear chromophores relative to the axis of light propagation. In the model we present here, this angle is different for the two linear chromophores, i.e., θ a ̸ = θ b . If, on the other hand, θ a = θ b , which would occur if the two linear chromophores were mutually parallel, then no local phase will be introduced into the system and the effect of circularly polarized light on exciton rotation vanishes.