An appropriate definition of the Hodge duality ⋆ operation on any arbitrary dimensional supermanifold has been a long-standing problem. We define a working rule for the Hodge duality ⋆ operation on the (2 + 2)-dimensional supermanifold parametrized by a couple of even (bosonic) spacetime variables x µ (µ = 0, 1) and a couple of odd (fermionic) variables θ andθ of the Grassmann algebra. The Minkowski spacetime manifold, hidden in the supermanifold and parametrized by x µ (µ = 0, 1), is chosen to be a flat manifold on which a two (1 + 1)-dimensional (2D) free Abelian gauge theory, taken as a prototype field theoretical model, is defined. We demonstrate the applications of the above definition (and its further generalization) for the discussion of the (anti-)co-BRST symmetries that exist for the field theoretical models of 2D-and 4D free Abelian gauge theories considered on the four (2 + 2)-and six (4 + 2)-dimensional supermanifolds, respectively.