“…The ∆ρ interaction has been analyzed in the framework of the hidden gauge formalism [25] in terms of the exchange of a ρ meson in the t−channel between the ∆ and the ρ [5,15]. Under the low energy approximation of neglecting q 2 /M 2 V in the propagator of the exchanged vector meson, where q is the momentum transfer, and also the three momentum − → k of the vector meson, one obtains for the ∆ρ → ∆ρ potential the form…”