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Multicluster study of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">C</mml:mi><mml:mo>+</mml:mo><mml:mi>n</mml:mi></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">C</mml:mi><mml:mo>+</mml:mo><mml:mi>p</mml:mi></mml:math>systems

M. DufourLaboratoire de Physique Théorique, Université Louis Pasteur, 23 rue du Loess, F67037 Strasbourg, FranceP. DescouvemontPhysique Nucléaire Théorique et Physique Mathématique, C.P. 229, Université Libre de Bruxelles, B1050 Bruxelles, Belgium
1997lv
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We use the generator coordinate method to study the ${}^{12}$C($n,\ensuremath{\gamma}{)}^{13}$C and ${}^{12}$C($p,\ensuremath{\gamma}{)}^{13}$N reactions, as well as the ${}^{13}$C and ${}^{13}$N spectroscopy. The ${}^{12}$C wave functions are defined by three $\ensuremath{\alpha}$ particles in a regular triangle of size ${R}_{C}.$ Different configurations are considered, in order to analyze clustering effects. It is shown that spectroscopic properties of ${}^{13}$C and ${}^{13}$N are sensitive to the ${}^{12}$C wave function; reasonable agreement with experiment is found with ${R}_{C}$ values minimizing the ${}^{12}$C binding energy. The present study supports the suggestion of a halo structure for the 1/2${}^{+}$ excited state in ${}^{13}$C. The neutron and proton capture cross sections are in good agreement with experiment. Finally, we analyze distortion effects in the ${}^{12}\mathrm{C}+n$ wave functions.

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