dorsal/arxiv
View SchemaHigher order effects in the $^{16}O(d,p)^{17}O$ and $^{16}O(d,n)^{17}F$ transfer reactions
| Authors | M. Assuncao, R. Lichtenthaler, V. Guimaraes, A. Lepine-Szily, G. F. Lima, A. M. Moro |
|---|---|
| Categories | |
| ArXiv ID | nucl-th/0409004 |
| URL | https://arxiv.org/abs/nucl-th/0409004 |
| DOI | 10.1103/PhysRevC.70.054601 |
| Journal | Phys.Rev. C70 (2004) 054601 |
Abstract
Full Coupled Channels Calculations were performed for the $^{16}O(d,n)^{17}F$ and $^{16}O(d,p)^{17}O$ transfer reactions at several deuteron incident energies from $E_{lab}=2.29$ MeV up to 3.27 MeV. A strong polarization effect between the entrance channel and the transfer channels $^{16}O(d,n)^{17}F(1/2^{+},0.495)$ and $^{16}O(d,p)^{17}O(1/2^{+},0.87)$ was observed. This polarization effect had to be taken into account in order to obtain realistic spectroscopic factors from these reactions.
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"abstract": "Full Coupled Channels Calculations were performed for the $^{16}O(d,n)^{17}F$\nand $^{16}O(d,p)^{17}O$ transfer reactions at several deuteron incident\nenergies from $E_{lab}=2.29$ MeV up to 3.27 MeV. A strong polarization effect\nbetween the entrance channel and the transfer channels\n$^{16}O(d,n)^{17}F(1/2^{+},0.495)$ and $^{16}O(d,p)^{17}O(1/2^{+},0.87)$ was\nobserved. This polarization effect had to be taken into account in order to\nobtain realistic spectroscopic factors from these reactions.",
"arxiv_id": "nucl-th/0409004",
"authors": [
"M. Assuncao",
"R. Lichtenthaler",
"V. Guimaraes",
"A. Lepine-Szily",
"G. F. Lima",
"A. M. Moro"
],
"categories": [
"nucl-th"
],
"doi": "10.1103/PhysRevC.70.054601",
"journal_ref": "Phys.Rev. C70 (2004) 054601",
"title": "Higher order effects in the $^{16}O(d,p)^{17}O$ and $^{16}O(d,n)^{17}F$ transfer reactions",
"url": "https://arxiv.org/abs/nucl-th/0409004"
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