The functional Schrödinger representation of a scalar field on an n-dimensional static space-time background is argued to be a singular limiting case of the hypercomplex quantum theory of the same system obtained by the precanonical quantization based on the space-time symmetric De Donder-Weyl Hamiltonian theory. The functional Schrödinger representation emerges from the precanonical quantization when the ultraviolet parameter κ introduced by precanonical quantization is replaced by γ 0 δ inv (0), where γ 0 is the time-like tangent space Dirac matrix and δ inv (0) is an invariant spatial (n − 1)-dimensional Dirac's delta function whose regularized value at x = 0 is identified with the cutoff of the volume of the momentum space. In this limiting case, the Schrödinger wave functional is expressed as the trace of the product integral of Clifford-algebra-valued precanonical wave functions restricted to a certain field configuration and the canonical functional derivative Schrödinger equation is derived from the manifestly covariant Dirac-like precanonical Schrödinger equation which is independent of a choice of a codimension-one foliation.