Explicit expressions of the vertex constant for the decay of a nucleus into two charged particles for an arbitrary orbital momentum l are derived for the standard expansion of the effective-range function K l (k 2 ), as well as when the function K0(k 2 ) has a pole. As physical examples, we consider the bound state of the nucleus 3 He and the resonant states of the nuclei 2 He and 3 He in the s-wave, and those of 5 He and 5 Li in the p-wave. For the systems N p and N d the pole trajectories are constructed in the complex planes of the momentum and of the renormalized vertex constant. They correspond to a transition from the resonance state to the virtual state while the Coulomb forces gradually decrease to zero.

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This erratum corrects misprints in Sec. V and in the Conclusion (Sec. VII) of our paper. The end of Eq. (34) should read ANC = 1.032×10 14 fm −1/2 instead of ANC = 1.032×10 4 fm −1/2 . There, the given value of the squared NVCG 2 l is correct. At the end of the Conclusion (p. 7, the right column, the fifth line above the Acknowledgments) the text should read ANC = 2.106×10 4 fm −1/2 instead of ANC = 1.0323×10 4 fm −1/2 .We would like to thank J.-M. Sparenberg who pointed out these misprints in his letter concerning his new preprint. 2469-9985/2016/93(5)/059901(1) 059901-1

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