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Asymptotic normalization coefficients from the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Ne</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>20</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>(<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">He</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>3</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>,<i>d</i>)<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Na</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>21</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>reaction and astrophysical factor for<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Ne</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>20</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>(<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi></mml:mrow></mml:math>)<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Na</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>21</mml:mn></mml:mrow></mml:mmultiscripts></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 RepublicV. BurjanNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicC. A. GagliardiCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAB. F. IrgazievPhysics Department, National University, Tashkent, UzbekistanV. KrohaNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicJ. NovakNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicŠ. PiskořNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicE. ŠimečkováNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicR. E. TribbleCyclotron Institute, Texas A&M University, College Station, Texas 77843, USAF. VeselýNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech RepublicJ. VincourNuclear Physics Institute of Czech Academy of Sciences, Prague-Řež, Czech Republic
Physical Review Cjournal2006lv
ABI

Аннотация

The $^{20}\mathrm{Ne}$$(p,\ensuremath{\gamma})$$^{21}\mathrm{Na}$ reaction rate at stellar energies is dominated by capture to the ground state through the tail of a subthreshold resonance state at an excitation energy of 2425 keV in $^{21}\mathrm{Na}$. Both resonant and direct capture contribute to the reaction rate while direct captures to other bound states are negligible. The overall normalization of direct capture to the subthreshold state is determined by the asymptotic normalization coefficient (ANC). Simultaneously this ANC determines the proton partial width of the subthreshold resonance state. To determine the ANC, the $^{20}\mathrm{Ne}$($^{3}\mathrm{He}$$,d)$$^{21}\mathrm{Na}$ proton transfer reaction has been measured, at an incident energy of 25.83 MeV. Angular distributions for proton transfer to the ground and first three excited states were measured, and ANCs were then extracted from comparison with distorted-wave Born approximation calculations. Using these ANCs, we calculated the astrophysical factor for $^{20}\mathrm{Ne}$$(p,\ensuremath{\gamma})$$^{21}\mathrm{Na}$. Our total astrophysical factor is $S(0)=5900\ifmmode\pm\else\textpm\fi{}1200$ keV b. Our analysis confirms that only nonresonant and resonant captures through the subthreshold state are important.

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