with eV-0.S}x and a>-1.6/*, one obtains 0.33, as compared with 0.14 for the Dirac electron, while with w=1.85ju the values are 0.16 and 0.03, respectively. Apart from this difference in magnitude, there is also a typical minimum of R with increasing incident energy below co = 3ju, which is impossible with the Dirac electron, where R drops montonically to zero for such high values of o>. Similar marked effects in the region of validity of the ordinary interpretation can be found in other more realistic problems (e.g., Coulomb and Compton scattering, details of which will be given elsewhere), and they may thus lead to tests of the theory regardless of questions of interpretation in other regions.