Abstract

The momentum-space structure of the Faddeev-Yakubovsky (FY)components of weakly-bound tetramers is investigated at the unitary limit using a renormalized zero-range two-body interaction. The results, obtained by considering a given trimer level with binding energy B3B_3, provide further support to a universal scaling function relating the binding energies of two successive tetramer states. The correlated scaling between the tetramer energies comes from the sensitivity of the four-boson system to a short-range four-body scale. Each excited N−N-th tetramer energy B4(N)B_4^{(N)} moves as the short-range four-body scale changes, while the trimer properties are kept fixed, with the next excited tetramer B4(N+1)B_4^{(N+1)} emerging from the atom-trimer threshold for a universal ratio B4(N)/B3=B4(N)/B4(N+1)≃4.6B_4^{(N)}/B_3 = B_4^ {(N)}/B_4^{(N+1)} \simeq 4.6, which does not depend on NN. We show that both channels of the FY decomposition [atom-trimer (K−K-type) and dimer-dimer (H−H-type)] present high momentum tails, which reflect the short-range four-body scale. We also found that the H−H-channel is favored over K−K-channel at low momentum when the four-body momentum scale largely overcomes the three-body one.

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