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Asymptotic normalization coefficients for<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>14</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">N</mml:mi><mml:mo>+</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mn>15</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:math>and the astrophysical<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>S</mml:mi></mml:math>factor for<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>14</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">N</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>15</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:math>

A. M. MukhamedzhanovCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAP. BémNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicB. A. BrownNational Superconducting Cyclotron Laboratory and Michigan State University, East Lansing, Michigan 48824, USAV. BurjanNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicC. A. GagliardiCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAV. KrohaNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicJ. NovakNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicF. M. NunesNational Superconducting Cyclotron Laboratory and Michigan State University, East Lansing, Michigan 48824, USAŠ. PiskořNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicF. PirlepesovCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAE. ŠimečkováNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicR. E. TribbleCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAJ. VincourNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech Republic
2003lv
ABI

Аннотация

The ${}^{14}\mathrm{N}(p,\ensuremath{\gamma}{)}^{15}\mathrm{O}$ reaction, which controls energy production in the CNO cycle, has contributions from both resonance and direct captures to the ground and excited states. The overall normalization of the direct captures is defined by the corresponding asymptotic normalization coefficients (ANCs). Especially important is the ANC for the subthreshold state in ${}^{15}\mathrm{O}$ at $\ensuremath{-}0.504\mathrm{keV}$ since direct capture through this state dominates the reaction rate at stellar energies. In order to determine the ANCs for ${}^{14}\mathrm{N}+{p}^{15}\mathrm{O},$ the ${}^{14}\mathrm{N}{(}^{3}\mathrm{He}{,d)}^{15}\mathrm{O}$ proton transfer reaction has been measured at an incident energy of 26.3 MeV. Angular distributions for proton transfer to the ground and five excited states were obtained. ANCs were then extracted from comparison to both distorted-wave Born approximation and coupled-channels Born approximation calculations. Using these ANCs, we calculated the astrophysical factor and reaction rates for ${}^{14}\mathrm{N}(p,\ensuremath{\gamma}{)}^{15}\mathrm{O}.$ Our analysis favors a low value for the astrophysical factor.

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