Excitation of 6Li above the breakup threshold in the 6Li + 208Pb system around the Coulomb barrier View Full Text


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Article Info

DATE

2003-11-18

AUTHORS

M. Mazzocco, P. Scopel, C. Signorini, L. Fortunato, F. Soramel, I. J. Thompson, A. Vitturi, M. Barbui, A. Brondi, M. Cinausero, D. Fabris, E. Fioretto, G. La Rana, M. Lunardon, R. Moro, A. Ordine, G. F. Prete, V. Rizzi, L. Stroe, M. Trotta, E. Vardaci, G. Viesti

ABSTRACT

.The excitation energy above the breakup threshold of the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\alpha + d/^6$\end{document}Li system, after the interaction of 6Li nuclei with a 208Pb target, was deduced from the invariant mass of the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\alpha + d$\end{document} system. Data were collected with a large-solid-angle detector set-up at four beam energies around the Coulomb barrier. The excitation of the 6Li nucleus above the breakup threshold (1.47 MeV) has a quite similar behavior at each measured beam energy and angle; it is peaked at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\sim 1$\end{document} MeV above the threshold and shows an exponential decay on the high energy side, which is a clear signature of a direct breakup process. The experimental excitation energies are reproduced both in shape and absolute value by 1) fully quantum-mechanical Coupled-Channel calculations with coupling to discretized-continuum 6Li excitations, 2) semi-classical Coupled-Channel approach, where the relative motion is treated along a classical trajectory. More... »

PAGES

583-587

References to SciGraph publications

  • 1999-05. Does break-up affect 9Be +209Bi fusion at the barrier? in THE EUROPEAN PHYSICAL JOURNAL A
  • 2001-05. Strong reaction channels at barrier energies in the system 6Li + 208Pb in THE EUROPEAN PHYSICAL JOURNAL A
  • Identifiers

    URI

    http://scigraph.springernature.com/pub.10.1140/epja/i2003-10097-y

    DOI

    http://dx.doi.org/10.1140/epja/i2003-10097-y

    DIMENSIONS

    https://app.dimensions.ai/details/publication/pub.1010261820


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    8 schema:description Abstract.The excitation energy above the breakup threshold of the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\alpha + d/^6$\end{document}Li system, after the interaction of 6Li nuclei with a 208Pb target, was deduced from the invariant mass of the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\alpha + d$\end{document} system. Data were collected with a large-solid-angle detector set-up at four beam energies around the Coulomb barrier. The excitation of the 6Li nucleus above the breakup threshold (1.47 MeV) has a quite similar behavior at each measured beam energy and angle; it is peaked at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\sim 1$\end{document} MeV above the threshold and shows an exponential decay on the high energy side, which is a clear signature of a direct breakup process. The experimental excitation energies are reproduced both in shape and absolute value by 1) fully quantum-mechanical Coupled-Channel calculations with coupling to discretized-continuum 6Li excitations, 2) semi-classical Coupled-Channel approach, where the relative motion is treated along a classical trajectory.
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