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Alternative Formulations of Scattering in Model Field Theories

Harry Gelman, Kurt L. Haller

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Abstract

A comparison is made between the expression for the boson-fermion scattering amplitude, in a model theory, obtained by renormalizing Feynman diagrams, and the one that originates from the dressed-particle picture. A proof is given of a surmise, previously verified to sixth order, that the two expressions for the transition amplitude are identical, although the former stems from a theory that leads to paradoxes from which the latter is exempt. The proof of the identity of the two representations is extended to transition amplitudes in which a weak interaction, considered to first order, is modified by a strong one considered to all orders. It is shown how the operations in the dressed-particle picture directly lead to iterations in terms of the physical mass and coupling constant, whereas the expressions obtained from the Feynman diagrams require renormalization before they have this form.

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What this paper is about

A comparison is made between the expression for the boson-fermion scattering amplitude, in a model theory, obtained by renormalizing Feynman diagrams, and the one that originates from the dressed-particle picture. A proof is given of a surmise, previously verified to sixth order, that the two expressions for the transition amplitude are identical, although the former stems from a theory that leads to paradoxes from which the latter is exempt. The proof of the identity of the two representations is extended to transition amplitudes in which a weak interaction, considered to first order, is modified by a strong one considered to all orders. It is shown how the operations in the dressed-particle picture directly lead to iterations in terms of the physical mass and coupling constant, whereas the expressions obtained from the Feynman diagrams require renormalization before they have this form.

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Available abstract

A comparison is made between the expression for the boson-fermion scattering amplitude, in a model theory, obtained by renormalizing Feynman diagrams, and the one that originates from the dressed-particle picture. A proof is given of a surmise, previously verified to sixth order, that the two expressions for the transition amplitude are identical, although the former stems from a theory that leads to paradoxes from which the latter is exempt. The proof of the identity of the two representations is extended to transition amplitudes in which a weak interaction, considered to first order, is modified by a strong one considered to all orders. It is shown how the operations in the dressed-particle picture directly lead to iterations in terms of the physical mass and coupling constant, whereas the expressions obtained from the Feynman diagrams require renormalization before they have this form.

Key concepts: Feynman diagram, Renormalization, Scattering amplitude, Coupling constant, Physics, Boson, Field theory (psychology), Quantum field theory

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