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We investigate the structure of resonance widths of a Bose-Hubbard Dimer with intersite hopping amplitude , which is coupled to continuum at one of the sites with strength . Using an effective non-Hermitian Hamiltonian formalism, we show that by varying the on-site interaction term the resonances undergo consequent bifurcations. For , the bifurcation points follow a scaling law ${\tilde \chi}n \equiv \chi_n N/k = f{\Lambda}(n-0.5/\Lambda)N$ is the number of bosons. For the function two different dependences are found around the minimum and the maximum bifurcation point.

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