1970Physical Review LettersRequires access

Magnitude of High-Energy Meson-Meson Total Cross Sections

Henry D. I. Abarbanel, Geoffrey F. Chew, M. L. Goldberger, L. M. Saunders

Open publisher page 33 citations

Abstract

The total cross section for meson-meson scattering at high energy is calculated using a simple, but plausible, $\mathrm{SU}(n)$-symmetric multiperipheral model. The resulting ${\ensuremath{\sigma}}_{T}$ is of the order $\frac{16{\ensuremath{\pi}}^{3}}{NM_{V}^{}{}_{}{}^{2}}$, where ${M}_{V}$ is the central mass of the dominant low-energy resonance multiplet in elastic meson-meson scattering and $N$ is the dimensionality of the multiplet of the incident mesons. The nongeometric character of this result is discussed.

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The total cross section for meson-meson scattering at high energy is calculated using a simple, but plausible, $\mathrm{SU}(n)$-symmetric multiperipheral model. The resulting ${\ensuremath{\sigma}}_{T}$ is of the order $\frac{16{\ensuremath{\pi}}^{3}}{NM_{V}^{}{}_{}{}^{2}}$, where ${M}_{V}$ is the central mass of the dominant low-energy resonance multiplet in elastic meson-meson scattering and $N$ is the dimensionality of the multiplet of the incident mesons. The nongeometric character of this result is discussed.

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Available abstract

The total cross section for meson-meson scattering at high energy is calculated using a simple, but plausible, $\mathrm{SU}(n)$-symmetric multiperipheral model. The resulting ${\ensuremath{\sigma}}_{T}$ is of the order $\frac{16{\ensuremath{\pi}}^{3}}{NM_{V}^{}{}_{}{}^{2}}$, where ${M}_{V}$ is the central mass of the dominant low-energy resonance multiplet in elastic meson-meson scattering and $N$ is the dimensionality of the multiplet of the incident mesons. The nongeometric character of this result is discussed.

Key concepts: Physics, Multiplet, Meson, Particle physics, Resonance (particle physics), Scattering, Nuclear physics, Order (exchange)

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