Abstract

Polarization and differential-cross-section data for backward ${\ensuremath{\pi}}^{+}p$ scattering are explained in terms of a model which includes the ${N}_{\ensuremath{\alpha}}$ Regge pole plus a background term which one may interpret as either a secondary pole or cut. This model, although simplifying the number of exchanges, provides an excellent fit to the data. The dip-bump structure and polarization are related. The rise of the differential cross section after the dip is shown in this model to be due in part to the background term rather than solely the recovery of the ${N}_{\ensuremath{\alpha}}$ Regge-pole term from zero due to the vanishing of $\ensuremath{\alpha}\ensuremath{-}\frac{1}{2}$ near $u=\ensuremath{-}0.14$ ${(\mathrm{G}\mathrm{e}\mathrm{V}/\mathit{c})}^{2}$.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.