Abstract
We solve the Faddeev equation in an exactly Poincaré invariant formulation of the three-nucleon problem. The dynamical input is a relativistic nucleon-nucleon () interaction that is exactly on-shell equivalent to the high-precision CD Bonn interaction. -matrix cluster properties dictate how the two-body dynamics is embedded in the three-nucleon mass operator (rest Hamiltonian). We find that for neutron laboratory energies above MeV relativistic effects on are negligible. For energies below MeV dynamical effects lower the nucleon analyzing power maximum slightly by and Wigner rotations lower it further up to , thereby increasing disagreement between data and theory. This indicates that three-nucleon forces (3NF) must provide an even larger increase of the maximum than expected up to now.
- Received 3 January 2008
DOI:https://doi.org/10.1103/PhysRevC.77.034004
©2008 American Physical Society