Manifestations of the Structure of Wave Functions of the O(g. s.; 3, 6.13 MeV) Nucleus in the Reactions OO and NO

The structure of the wave functions for the O(g. s.; 3 ) nucleus is studied by employing experimental angular distributions of the differential cross sections for the reactions O O(g. s.; 3 ) and N O(g. s.; 3 ) at MeV. The present analysis is carried out by the coupled-channel method with allowance...

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Bibliographic Details
Published in:Physics of atomic nuclei 2022, Vol.85 (6), p.850-857
Main Authors: Galanina, L. I., Zelenskaya, N. S., Lebedev, V. M., Orlova, N. V., Spassky, A. V.
Format: Article
Language:English
Subjects:
Nuclear cross sections
NUCLEI/Theory
Particle and Nuclear Physics
Physics
Physics and Astronomy
Wave functions
Online Access:Get full text
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Summary:The structure of the wave functions for the O(g. s.; 3 ) nucleus is studied by employing experimental angular distributions of the differential cross sections for the reactions O O(g. s.; 3 ) and N O(g. s.; 3 ) at MeV. The present analysis is carried out by the coupled-channel method with allowance for direct mechanisms (proton stripping and transfer of a C heavy cluster) and on the basis of the compound-nucleus model. Each of the mechanisms under consideration is associated with a specific configuration of the wave function for the O nucleus and is found to make a significant contribution to the experimental cross section.
ISSN:1063-7788
1562-692X
DOI:10.1134/S1063778823010209