Elastic α transfer in the 16O+12C scattering and its impact on the nuclear rainbow

Elastic 16 O + 12 C scattering is known to exhibit the nuclear rainbow pattern at incident energies E lab ≳ 200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (...

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Published inThe European physical journal. A, Hadrons and nuclei Vol. 57; no. 1
Main Authors Phuc, Nguyen Hoang, Khoa, Dao T., Phuc, Nguyen Tri Toan
Format Journal Article
LanguageEnglish
Published Berlin/Heidelberg Springer Berlin Heidelberg 01.01.2021
Springer Nature B.V
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ISSN1434-6001
1434-601X
DOI10.1140/epja/s10050-020-00325-3

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Abstract Elastic 16 O + 12 C scattering is known to exhibit the nuclear rainbow pattern at incident energies E lab ≳ 200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (OP) given by the double-folding model (DFM). At lower energies, the extensive elastic 16 O + 12 C scattering data show consistently that the nuclear rainbow pattern at backward angles is deteriorated by an oscillating enhancement of elastic cross section that is difficult to describe in the conventional optical model (OM). Given a significant α spectroscopic factor predicted for the dissociation 16 O → α + 12 C by the shell model and α -cluster models, the contribution of the elastic α transfer (or the core-core exchange) to the elastic 16 O + 12 C scattering should not be negligible and is expected to account for the enhanced elastic cross section at backward angles. To reveal the impact of the elastic α transfer, a systematic coupled reaction channels analysis of the elastic 16 O + 12 C scattering has been performed, with the coupling between the elastic scattering and elastic α transfer channels treated explicitly, using the real OP given by the DFM. We found that the elastic α transfer enhances the near-side scattering significantly at backward angles, giving rise to an oscillating distortion of the smooth Airy structure. The dynamic polarization of the OP by the coupling between the elastic scattering and elastic α transfer channels can be effectively taken into account in the OM calculation by an angular-momentum (or parity) dependent potential added to the imaginary OP, as suggested by Frahn and Hussein 40 years ago.
AbstractList Elastic 16O+12C scattering is known to exhibit the nuclear rainbow pattern at incident energies Elab≳200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (OP) given by the double-folding model (DFM). At lower energies, the extensive elastic 16O+12C scattering data show consistently that the nuclear rainbow pattern at backward angles is deteriorated by an oscillating enhancement of elastic cross section that is difficult to describe in the conventional optical model (OM). Given a significant α spectroscopic factor predicted for the dissociation 16O→α+12C by the shell model and α-cluster models, the contribution of the elastic α transfer (or the core-core exchange) to the elastic 16O+12C scattering should not be negligible and is expected to account for the enhanced elastic cross section at backward angles. To reveal the impact of the elastic α transfer, a systematic coupled reaction channels analysis of the elastic 16O+12C scattering has been performed, with the coupling between the elastic scattering and elastic α transfer channels treated explicitly, using the real OP given by the DFM. We found that the elastic α transfer enhances the near-side scattering significantly at backward angles, giving rise to an oscillating distortion of the smooth Airy structure. The dynamic polarization of the OP by the coupling between the elastic scattering and elastic α transfer channels can be effectively taken into account in the OM calculation by an angular-momentum (or parity) dependent potential added to the imaginary OP, as suggested by Frahn and Hussein 40 years ago.
Elastic 16 O + 12 C scattering is known to exhibit the nuclear rainbow pattern at incident energies E lab ≳ 200 MeV, with the Airy structure of the far-side scattering cross section clearly seen at medium and large angles. Such a rainbow pattern is well described by the deep real optical potential (OP) given by the double-folding model (DFM). At lower energies, the extensive elastic 16 O + 12 C scattering data show consistently that the nuclear rainbow pattern at backward angles is deteriorated by an oscillating enhancement of elastic cross section that is difficult to describe in the conventional optical model (OM). Given a significant α spectroscopic factor predicted for the dissociation 16 O → α + 12 C by the shell model and α -cluster models, the contribution of the elastic α transfer (or the core-core exchange) to the elastic 16 O + 12 C scattering should not be negligible and is expected to account for the enhanced elastic cross section at backward angles. To reveal the impact of the elastic α transfer, a systematic coupled reaction channels analysis of the elastic 16 O + 12 C scattering has been performed, with the coupling between the elastic scattering and elastic α transfer channels treated explicitly, using the real OP given by the DFM. We found that the elastic α transfer enhances the near-side scattering significantly at backward angles, giving rise to an oscillating distortion of the smooth Airy structure. The dynamic polarization of the OP by the coupling between the elastic scattering and elastic α transfer channels can be effectively taken into account in the OM calculation by an angular-momentum (or parity) dependent potential added to the imaginary OP, as suggested by Frahn and Hussein 40 years ago.
Author Khoa, Dao T.
Phuc, Nguyen Hoang
Phuc, Nguyen Tri Toan
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– reference: FullerRCPhys. Rev. C19751215611975PhRvC..12.1561F
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– reference: BrandanMESatchlerGRPhys. Rep.19972851431997PhR...285..143B
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– reference: FrickeSHBrandanMEMcVoyKWPhys. Rev. C1988386821988PhRvC..38..682F
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Snippet Elastic 16 O + 12 C scattering is known to exhibit the nuclear rainbow pattern at incident energies E lab ≳ 200 MeV, with the Airy structure of the far-side...
Elastic 16O+12C scattering is known to exhibit the nuclear rainbow pattern at incident energies Elab≳200 MeV, with the Airy structure of the far-side...
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springer
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Publisher
SubjectTerms Angular momentum
Channels
Cluster Structure and Dynamics of Nuclei - A Tribute to Mahir Hussein
Coupling
Elastic scattering
Hadrons
Heavy Ions
Nuclear Fusion
Nuclear Physics
Particle and Nuclear Physics
Physics
Physics and Astronomy
Rainbows
Regular Article – Theoretical Physics
Scattering cross sections
Title Elastic α transfer in the 16O+12C scattering and its impact on the nuclear rainbow
URI https://link.springer.com/article/10.1140/epja/s10050-020-00325-3
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