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Four-Vectors and Helicity Amplitudes in πN Elastic Scattering

Loren Dell Krase, R. H. Good

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Abstract

There is a natural way to introduce a set of four orthogonal four-vectors in the elastic scattering process. In the $\ensuremath{\pi}N$ elastic problem, they provide a covariant description of the helicity-flip and -nonflip processes. The nonflip interaction operator becomes a rotation through the scattering angle $\ensuremath{\theta}$ about the normal to the scattering plane; the helicity-flip interaction involves a rotation through $\ensuremath{\pi}+\ensuremath{\theta}$.

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What this paper is about

There is a natural way to introduce a set of four orthogonal four-vectors in the elastic scattering process. In the $\ensuremath{\pi}N$ elastic problem, they provide a covariant description of the helicity-flip and -nonflip processes. The nonflip interaction operator becomes a rotation through the scattering angle $\ensuremath{\theta}$ about the normal to the scattering plane; the helicity-flip interaction involves a rotation through $\ensuremath{\pi}+\ensuremath{\theta}$.

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Available abstract

There is a natural way to introduce a set of four orthogonal four-vectors in the elastic scattering process. In the $\ensuremath{\pi}N$ elastic problem, they provide a covariant description of the helicity-flip and -nonflip processes. The nonflip interaction operator becomes a rotation through the scattering angle $\ensuremath{\theta}$ about the normal to the scattering plane; the helicity-flip interaction involves a rotation through $\ensuremath{\pi}+\ensuremath{\theta}$.

Key concepts: Helicity, Physics, Covariant transformation, Scattering amplitude, Scattering, Elastic scattering, Rotation (mathematics), Quantum electrodynamics

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