Since and , the diagonal Hamiltonian is
with the identity on every unlisted qubit. Each computational-basis state is an eigenstate, and its eigenvalue is minus the cost of the corresponding cut. Part i supplies cost four, while the assumed bound rules out a lower energy. Thus the ground-state energy is . For the assignment , one ground state is
Its bitwise complement is another ground state, as are the basis states corresponding to the other maximum cuts.

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