Abstract
The reactions K−d → NΛπ and NΣπ are calculated using a three‐body multichannel formalism and two‐body interactions between all pairs of particles. Quantitative agreement with the data on relative rates and spectra is found using acceptable two‐body potentials. The results imply that there is no unstable bound state (2nd sheet pole above Λ N threshold) in the (ΣN, ΛN) system but do require a virtual state (4th sheet pole) near the ΣN threshold.
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