Theory of interacting Pomerons

A. A. Migdal; A. M. Polyakov; K. A. Ter-Martirosyan

doi:10.1016/0370-2693(74)90021-5

Theory of interacting Pomerons

A. A. Migdal, A. M. Polyakov, K. A. Ter-Martirosyan

Physics

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137 Scopus citations

Abstract

The quantitative theory of Pomeron interaction is developed on the basis of strong coupling methods and ε{lunate}-expansion. The theory is consistent with all unitarity conditions. At asymptotic energy total cross section increases as (ln s)^η, the multiplicity as (lns)^η+1, and diffraction cone shrinks as (lns)^-ν, where η ≈ 1 6, ν ≈ 13 21. At modern energy the theory gives small corrections to the Regge model.

Original language	English (US)
Pages (from-to)	239-242
Number of pages	4
Journal	Physics Letters B
Volume	48
Issue number	3
DOIs	https://doi.org/10.1016/0370-2693(74)90021-5
State	Published - Feb 4 1974

All Science Journal Classification (ASJC) codes

Nuclear and High Energy Physics

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AU - Migdal, A. A.

AU - Polyakov, A. M.

AU - Ter-Martirosyan, K. A.

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N2 - The quantitative theory of Pomeron interaction is developed on the basis of strong coupling methods and ε{lunate}-expansion. The theory is consistent with all unitarity conditions. At asymptotic energy total cross section increases as (ln s)η, the multiplicity as (lns)η+1, and diffraction cone shrinks as (lns)-ν, where η ≈ 1 6, ν ≈ 13 21. At modern energy the theory gives small corrections to the Regge model.

AB - The quantitative theory of Pomeron interaction is developed on the basis of strong coupling methods and ε{lunate}-expansion. The theory is consistent with all unitarity conditions. At asymptotic energy total cross section increases as (ln s)η, the multiplicity as (lns)η+1, and diffraction cone shrinks as (lns)-ν, where η ≈ 1 6, ν ≈ 13 21. At modern energy the theory gives small corrections to the Regge model.

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DO - 10.1016/0370-2693(74)90021-5

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VL - 48

SP - 239

EP - 242

JO - Physics Letters B

JF - Physics Letters B

IS - 3

ER -

Theory of interacting Pomerons

Abstract

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