In this paper, we determine at weak coupling the non-relativistic -body Schrödinger equation that describes the low-lying color singlet bound states of two dimensional adjoint with heavy quarks. In the case of three adjoint quarks, we show that the three-body equation reduces equivalently to the Schrödinger equation that describes a point electric dipole in an electric field in a plane angular sector. We conjecture that the three-body problem is solvable. The eigenstates are given in terms of the triconfluent Heun functions. Our conjecture implies that a bound state of three adjoint quarks is described by a particle confined in a two dimensional Cornell potential. We expect the -parton problem also to be solvable in a similar fashion.

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