Abstract
The dual absorptive model of Harari is shown to explain consistently the s and t dependence of the sum of π +p and π −p elastic differential cross sections at high energy. The Pomeran amplitude shrinks at a rate similar to that of K +p elastic scattering while the f amplitude is shown to be dominated by peripheral partial waves at a radius ∼ 1 fm. Finally, the shrinkage and s dependence of the f amplitude follow a canonical Regge behavior.
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