Abstract

We present a method for calculating scattering phase shifts which utilizes continuum-discretized states obtained in a bound-state type calculation. The wrong asymptotic behavior of the discretized state is remedied by means of the Green's function formalism. Test examples confirm the accuracy of the method. The α+n\alpha+n scattering is described using realistic nucleon-nucleon potentials. The 3/23/2^- and 1/21/2^- phase shifts obtained in a single-channel calculation are too small in comparison with experiment. The 1/2+1/2^+ phase shifts are in reasonable agreement with experiment, and gain contributions both from the tensor and central components of the nucleon-nucleon potential.Comment: 16 pages, 5 figure

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