Abstract
Assuming separable two-body potentials, a general derivation is given of the three-nucleon equations. The derivation allows for the full complexity, in separable form, of the two-nucleon interaction including an arbitrary number of (possibly coupled) partial waves and an arbitrary number of separable terms in each partial wave. All three-body partial waves are considered. Using a convenient notation, the three-body equations and their angular momentum decomposition are easily derived.
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