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 giveFor the links from these neighbors to the next sites have strength . Applying the Hamiltonian operator a second time yieldsThe central coefficient is . On the comparison path, direct multiplication givesThus the two calculations match under and for . If , the terms involving and distance two are absent on both sides.
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