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Abstract We use a near-threshold parameterization with explicit inclusion of the Castillejo–Dalitz–Dyson poles, which is more general than the effective range expansion, to study the bottomonium-like states $$Z_b(10610)$$ Z b ( 10610 ) and $$Z_b(10650)$$ Z b ( 10650 ) . In terms of the partial-wave amplitude, we fit the event number distribution of $$B^{(*)}{\bar{B}}^*$$ B ( ∗ ) B ¯ ∗ system to the experimental data for these resonances from Belle Collaboration. The data could be described very well in our method, which supports the molecular interpretation. Then the relevant physical quantities are obtained, including the $$B^{(*)}\bar{B}^*$$ B ( ∗ ) B ¯ ∗ scattering length (a), effective range (r), and residue squared ( $$\gamma _s^2$$ γ s 2 ) of the pole in the complex plane. In particular, we find the compositeness can range from about 0.4 up to 1 for the $$B{\bar{B}}^*$$ B B ¯ ∗ ( $$B^*{\bar{B}}^*$$ B ∗ B ¯ ∗ ) component in the resonance $$Z_b(10610)$$ Z b ( 10610 ) ( $$Z_b(10650)$$ Z b ( 10650 ) ).