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Authors
  • Urazbekov, B. A.1, 2, 3, 4
  • Denikin, A. S.1, 2
  • Itaco, N.3, 4
  • Janseitov, D.2, 5
  • 1 Dubna State University, Dubna, Russia , Dubna (Russia)
  • 2 Joint Institute for Nuclear Research, Dubna, Russia , Dubna (Russia)
  • 3 Dipartimento di Matematica e Fisica, Università degli Studi della Campania ‘‘Luigi Vanvitelli’’, Caserta, Italy , Caserta (Italy)
  • 4 Istituto Nazionale di Fisica Nucleare, Complesso Univeristario di Monte S. Angelo, Napoli, Italy , Napoli (Italy)
  • 5 Institute of Nuclear Physics, National Nuclear Center of Republic of Kazakhstan, Almaty, Republic of Kazakhstan , Almaty (Kazakhstan)
Type
Published Article
Journal
Physics of Atomic Nuclei
Publisher
Pleiades Publishing
Publication Date
May 01, 2021
Volume
84
Issue
3
Pages
250–255
Identifiers
DOI: 10.1134/S1063778821030145
Source
Springer Nature
Disciplines
  • Article
License
Yellow

Abstract

AbstractElastic-scattering processes in the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{3}\textrm{He}+{}^{9}$$\end{document}Be reaction are studied on the basis of the 2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha+n$$\end{document} three-body cluster model of the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{9}$$\end{document}Be nucleus. The \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{9}$$\end{document}Be three-body wave function obtained by the variational method in the Gaussian basis is used to derive an analytic representation of nuclear-matter density distribution. The interaction potential calculated for the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{3}\textrm{He}+{}^{9}$$\end{document}Be system by the double-folding method is employed to analyze experimental data on the differential cross section for the elastic-scattering process \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{9}$$\end{document}Be (\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{3}$$\end{document}He, \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{3}$$\end{document}He)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${}^{9}$$\end{document}Be at collision energies between 30 and 60 MeV.

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