Abstract <p>Deuteron photodisintegration is calculated in the photon energy range <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(500{-}600\)</EquationSource> <!--NuclPhys2560193Fiks-m5--> </InlineEquation> MeV, adopting a standard theory in which the nucleonic one-body current, meson exchange currents and isobar excitations are taken into account. The final-state interaction in the isospin-1 states is treated within a three-body <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\pi NN\)</EquationSource> <!--NuclPhys2560193Fiks-m6--> </InlineEquation> model approach. The main attention is paid to the possible contribution of the <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(d^{*}(2380)\)</EquationSource> <!--NuclPhys2560193Fiks-m7--> </InlineEquation> dibaryon. Its influence on this reaction is compared with its role in coherent <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\pi^{0}\pi^{0}\)</EquationSource> <!--NuclPhys2560193Fiks-m8--> </InlineEquation> photoproduction on a deuteron at the same energies.</p>

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Photodisintegration and Coherent \({\pi^{0}\pi^{0}}\) Photoproduction on the Deuteron in the \({d^{*}(2380)}\) Region

  • A. I. Fix

摘要

Abstract

Deuteron photodisintegration is calculated in the photon energy range \(500{-}600\) MeV, adopting a standard theory in which the nucleonic one-body current, meson exchange currents and isobar excitations are taken into account. The final-state interaction in the isospin-1 states is treated within a three-body \(\pi NN\) model approach. The main attention is paid to the possible contribution of the \(d^{*}(2380)\) dibaryon. Its influence on this reaction is compared with its role in coherent \(\pi^{0}\pi^{0}\) photoproduction on a deuteron at the same energies.