We investigate the structure of resonance widths of a Bose-Hubbard dimer with intersite hopping amplitude k, which is coupled to a continuum at one of the sites with strength γ. Using an effective non-Hermitian Hamiltonian formalism, we show that by varying the on-site interaction term χ the resonances undergo consequent bifurcations. For Λ=k∕γ0.5, the bifurcation points follow a scaling law ̃ \~χₘ≡χₘN∕k=f_Λ(m-0.5∕Λ), where N is the number of bosons. For the function f_Λ two different Λ dependences are found around the minimum and maximum bifurcation points.
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Hiller et al. (2006) studied this question.
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