Of all nuclear physics experiments none are more fundamental than elastic'' $p,p$ and, secondarily, $p,d$ or $d,d$ scattering. Recognizing that these particles are themselves composite, elastic’’ scattering may be accompanied by temporary internal rearrangement with undetectably small energy loss. % This paper argues that correct calculation of the spin dependence of elastic scattering must account for a previously-neglected relativistic effect of $G$'', the anomalous magnetic dipole moment (MDM) of the scattering particles and proceeds to describe storage ring $p,p$ scattering configurations capable of confirming this contention. % Especially important experimentally for protons is the existence of near perfect’’ proton-carbon scattering polarimetric analyzing power near ,MeV laboratory kinetic energy. % Possibilities: (i) With counter-circulating MeV energy proton beams the final spin states of coincident scattered protons can be determined with high probability for a significantly large fraction of all scatters. For comparison with current descriptions this corresponds roughly to proton kinetic energy MeV in the laboratory frame, close to the pion production threshold. % (ii) In a DERBENEV-style'' figure-8 storage ring, independently polarized, diametrically opposite bunches on orthogonal orbits can collide at the beam crossover point with symmetric $K''\approx200$ MeV energies in a slow, transversely moving frame. % (iii) $p$ and $d$ beams can counter-circulate at the same time in a small racetrack shaped ring with superimposed electric and magnetic bending. In this case the scattering would be WOLFENSTEIN-style’’ with collinear incident orbits. % To investigate the consistency of quantum mechanics and special relativity it is proposed to implement options (ii) and (iii) in the COSY beam hall.

生成讲解博客的中文版本

生成AI智能校验的中文版本