Based on the fact that any massless free-field with spin higher than 1 2 can be constructed from scalar fields (spin-0) and Dirac-Weyl fields (spin-12 ), we introduce a map between spin-2 massless free-fields (gravity fields) and spin-1 2 massless free-fields (Dirac-Weyl fields) in spinor formalism. The associated Dirac-Weyl spinors can live in certain spacetime are identified. Regarding them as basic units, other higher spin massless free-fields are then constructed. In this way, some hidden fundamental features related to massless-free fields are revealed. In particular, for type N vacuum spacetimes, we show that all higher spin massless free-fields can be constructed by the same type of Dirac-Weyl spinors and an auxiliary scalar field, which satisfies the wave equation not only on curved spacetime but also on Minkowski spacetime. For type D vacuum spacetimes, we show that there exist similar relationships among different spin massless free-fields. Furthermore, we systematically rebuild the Weyl double copy for non-twisting type N vacuum spacetimes and type D vacuum spacetimes. We show that the zeroth copy not only connects the gravity fields with a single copy but also connects those degenerate electromagnetic fields with the Dirac-Weyl fields living in the curved spacetime, both for type N and type D cases. Afterward, we extend the study to type III non-twisting vacuum solutions. Independent of the proposed map, we find that there is a special Dirac-Weyl scalar whose square is just proportional to the Weyl scalar. A degenerate Maxwell field and an auxiliary scalar field are then solved. Both of them play the similar roles as the double copy. The result further confirms that there must exist a deep connection between gravity theory and gauge theory.