In the single-excitation subspace, part (a) turns each coupling into a hopping coefficient between adjacent sites. With denoting the excitation at site , the two central links give
For the links from these neighbors to the next sites have strength . Applying the Hamiltonian operator a second time yields
The central coefficient is . On the comparison path, direct multiplication gives
Thus the two calculations match under and for . If , the terms involving and distance two are absent on both sides.

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