Parafermionic zero modes are a novel set of excitations displaying non-Abelian statistics somewhat richer than that of Majorana modes. These modes are predicted to occur when nearby fractional quantum Hall edge states are gapped by an interposed superconductor. Despite substantial experimental progress, we argue that the necessary crossed Andreev reflection in this arrangement is a challenging milestone to reach. We propose a superconducting quantum dot array structure on a fractional quantum Hall edge that can lead to parafermionic zero modes from coherent superconducting forward scattering on a quantum Hall edge. Such coherent forward scattering has already been demonstrated in recent experiments. We show that for a spin-singlet superconductor interacting with loops of spin unpolarized 2/3 fractional quantum edge, even an array size of order ten should allow one to systematically tune into a parafermionic degeneracy.Introduction.-Theoretical understanding and experimental realization of non-Abelian anyons has attracted considerable attention in the past few years. This surge of interest can be largely attributed to potential application of such systems as building blocks for topological quantum computers [1]. Majorana zero modes (MZMs) [2][3][4][5][6][7] provide the simplest and experimentally the most promising example of non-Abelian anyons. So far, most of the effort in searching for non-Abelian anyons has been focused on MZMs. Following a series of theoretical proposals [8][9][10][11], suggestive experimental evidence of MZMs has been observed in semiconductor/superconductor heterostructures [12][13][14][15][16][17][18]. Despite their fascinating properties MZMs are non-Abelian anyons of the Ising (Z 2 ) type. Universal quantum computation cannot be implemented using braiding of the Z 2 anyons alone. Therefore, searching for a computationally richer set of anyons seems necessary.