Abstract
Four-body integral equations are used to calculate dd→dd and dd→H amplitudes using a single-term separable nucleon-nucleon potential in channels and . First-order perturbation theory is used to include in the four-body kernel the contribution of d-wave two- and three-nucleon channel components that result from the tensor force. Cross sections and analyzing powers are calculated using all positive- and negative-parity four-body amplitudes with total angular momentum J≤4. Comparison with data is presented.
- Received 5 June 1989
DOI:https://doi.org/10.1103/PhysRevLett.63.2036
©1989 American Physical Society