“…First of all, the Lagrangian densities L (b 1 ) and L (b 2 ) have been derived in a completely different manner in our present endeavor if we compare our present derivation against the derivation in our earlier work [12] where we have exploited the method of trial and error. Second, the CF-type restrictions: B + B + m φ = 0 and B + B + m φ = 0 are same as in our earlier work [12,21] but the other two restrictions in (47) are different. Third, if we stick with the CF-type restrictions that have been derived from the superfield approach to BRST formalism in context of 4D Abelian 2-form massless and massive gauge theories [18,21], we find that the other two restrictions of (47) are: B µ + Bµ + ∂ µ φ = 0 and B µ + Bµ + ∂ µ φ = 0.…”