Using the potentials derived from Ps(jv) meson theory of the second and fourth order, neutron-proton and proton-proton scattering at 40 Mev and 90 Mev in the laboratory system are examined. Calculation is performed by numerical integrations. The characteristic features of high energy nudeon-nudeon scattering are fairly well explained by our pseudoscalar meson potential.Using the potentials derived from Ps(jv) meson theory of the second and fourth order, neutron-proton and proton-proton scattering at 40 Mev and 90 Mev in the laboratory system are examined. Calculation is performed by numerical integrations. The characteristic features of high energy nudeon-nudeon scattering are fairly well explained by our pseudoscalar meson potential. Downloaded from iii) For~:i:he proton-proton scattering, the potential in the singlet even state is, near and outside it"5· range, very small. Therefore, the phase shift of ID-wave ,is also small and consequently the destructive interference does not break the isotropy of angular distribution so severely.The polarization PC 0, cp) appearing after pop scattering by this potential is calculated at 90 Mev, where cp is the azimuthal angle, the z-axis being parallel to the inc;iden~ '" held at
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.