The slopes $B(k)$ of the exponential forward peak for π^±p and K^±p elastic scattering have been surveyed in the region 0.3Plab20.0 GeV/c. Plots of the momentum dependence of $B(k)$ reveal striking enhancements at momenta corresponding to the location of known high-spin, high-elasticity resonances. There are indications that the background behavior of $B(k)$, when considered over such a wide momentum interval, might be smoothly rising in all cases; thus, the forward peak associated with background diffraction effects would appear to shrink not only in K⁺p→K⁺p interactions, where resonance formation is weak (or absent), but also in π^±p→π^±p and K^-p→K^-p interactions, where many prominent resonant states are formed. An explanation for the behavior of $B(k)$ is presented, based on the properties of the logarithmic derivative of the differential cross section in the forward direction. As a quantitative illustration, B(k)_K^- was derived in terms of a simple phenomenological model, which involves a linear superposition of diffractive-like and resonant amplitudes. In this way a fit to the B(k)_K^- and K^-p total-cross-section data could be obtained throughout the entire momentum region. The information which can be derived from the experimental study of $B(k)$ is discussed; this has bearing on the determination of resonance properties and on the behavior of the spin-flip amplitude.
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Lasinski et al. (1969) studied this question.
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