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Field-theoretical description of the deuteron breakup in the clothed particle representation
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Field-theoretical description of the deuteron breakup in the clothed particle representation

O Shebeko, A Arslanaliev, Y Kostylenko, V Chahar, J Golak, H Kamada, W. N Polyzou, D Ramírez, R Skibiński, K Topolnicki, …
ArXiv.org
Cornell University
04/27/2026
DOI: 10.48550/arxiv.2604.24457
url
https://doi.org/10.48550/arxiv.2604.24457View
Preprint (Author's original) This preprint has not been evaluated by subject experts through peer review. Preprints may undergo extensive changes and/or become peer-reviewed journal articles. Open Access

Abstract

We present a field-theoretical description of the deuteron electrodisintegration reaction d(e,e'p)n induced by unpolarized and polarized electrons. The approach combines the Lehmann-Symanzik-Zimmermann in(out) formalism with the clothed particle representation in the instant form of relativistic dynamics, providing a fully relativistic and gauge-independent framework based on the Fock-Weyl criterion. Within the method of unitary clothing transformations, one and the same transformation that generates the relativistic nucleon-nucleon interaction (the Kharkiv potential) also induces a fresh family of electromagnetic current operators. As a result, one-body and two-body (meson-exchange) currents emerge on a common footing. We compute differential cross sections and polarization observables with the inclusion of final-state interaction effects and meson-exchange current contributions, and compare the results with Saclay and Jefferson Lab data as well as with earlier theoretical predictions. The role of relativistic ingredients (one- and two-body currents, Fermi-motion effects, etc.) and the interplay between them are analyzed in several kinematic regimes of the experiments at Saclay and Jefferson Lab.
Physics - Nuclear Theory

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