Differential cross sections for the elastic scattering of negative pi mesons on protons (π^--p→π^--p) were measured at the Berkeley Bevatron at five laboratory kinetic energies of the pion between 500 and 1000 MeV. The results were least-squares fitted with a power series in the cosine of the center-of-mass scattering angle, and total elastic cross sections for π^--p→π^--p were obtained by integrating under the fitted curves. The coefficients of the cosine series are shown plotted versus the incident pion laboratory kinetic energy. These curves display as a striking feature a large value of the coefficient of cos⁵θ* peaking in the vicinity of the 900-MeV resonance. This implies that a superposition of F5/2 and D5/2 partial waves is prominent in the scattering at this energy, since the coefficients for terms above cos⁵θ* are negligible. One possible explanation is that the F5/2 enhancement comes from an elastic resonance in the isotopic spin T=1/2 state, consistent with Regge-pole formalism, and the D5/2 partial-wave state may be enhanced by inelastic processes. At 600 MeV the values of the coefficients do not seem to demand the prominence of any single partial-wave state, although the results are compatible with an enhancement in the J=3/2 amplitude. A table listing quantum numbers plausibly associated with the various peaks and "shoulders" seen in the π^±-p total cross-section curves is presented.
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Helland et al. (1964) studied this question.
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