Abstract
The high-energy forward scattering of a pseudoscalar meson (μ) and a baryon (B) is discussed on the basis of the Amati-Bertocchi-Fubini-Stanghellini-Tonin multiperipheral model. Assuming that the low-energy μB amplitude is dominated by the baryon pole plus the first elastic resonance, and using the approximate solution to the μμ integral equation proposed by Abarbanel, Chew, Goldberger, and Saunders, we derive an expression for the high-energy limit of σμBtot. A numerical estimate based on SU(3) symmetry is given.