Maqola

Asymptotic normalization coefficients and neutron halo of the excited states in<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">B</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>13</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:math>

Z. H. LiuChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaC. J. LinChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaH. Q. ZhangChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaZ. C. LiChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaJ. S. ZhangChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaY. W. WuChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaFang YangChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaM. RuanChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaJ. C. LiuChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaS. Y. LiChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, ChinaZ. H. PengChina Institute of Atomic Energy, P.O. Box 275(10), Beijing 102413, China

2001lv

ABI

Annotatsiya

The transfer reactions of ${}^{11}\mathrm{B}{(d,p)}^{12}\mathrm{B}$ and ${}^{12}\mathrm{C}{(d,p)}^{13}\mathrm{C},$ at incident energy of $11.8 \mathrm{MeV},$ have been used to extract asymptotic normalization coefficients and root-mean-square radii for the last neutron in ${}^{12}\mathrm{B}$ and ${}^{13}\mathrm{C}.$ It is found experimentally that the second ${(J}^{\ensuremath{\pi}}{=2}^{\ensuremath{-}})$ and third ${(J}^{\ensuremath{\pi}}{=1}^{\ensuremath{-}})$ excited states in ${}^{12}\mathrm{B}$ and the first ${(J}^{\ensuremath{\pi}}{=1/2}^{+})$ excited state in ${}^{13}\mathrm{C}$ are the neutron halo states, whereas the third ${(J}^{\ensuremath{\pi}}{=5/2}^{+})$ excited state in ${}^{13}\mathrm{C}$ is a neutron skin state.

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Identifikatorlar

DOI: 10.1103/physrevc.64.034312

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