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Constraining the 6.05 MeV<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>and 6.13 MeV<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mn>3</mml:mn></mml:mrow><mml:mrow><mml:mo>−</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>Cascade Transitions in the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:mmultiscripts><mml:mo stretchy="false">(</mml:mo><mml:mi>α</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mo stretchy="false">)</mml:mo><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>16</mml:mn></mml:mrow></mml:mmultiscripts></mml:mrow></mml:math>Reaction Using the Asymptotic Normalization Coefficients

M. L. AvilaDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAG. V. RogachevDepartment of Physics & Astronomy and Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USAE. KoshchiyDepartment of Physics & Astronomy and Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USAL. T. BabyDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAJ. BelargeDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAK. W. KemperDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAA. N. KucheraDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAA. M. MukhamedzhanovDepartment of Physics & Astronomy and Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USAD. Santiago-GonzalezDepartment of Physics, Florida State University, Tallahassee, Florida 32306, USAE. UbersederDepartment of Physics & Astronomy and Cyclotron Institute, Texas A&M University, College Station, Texas 77843, USA
2015lv
ABI

Аннотация

The $^{12}\mathrm{C}(\ensuremath{\alpha},\ensuremath{\gamma})^{16}\mathrm{O}$ reaction plays a fundamental role in astrophysics and needs to be known with accuracy better than 10%. Cascade $\ensuremath{\gamma}$ transitions through the excited states of $^{16}\mathrm{O}$ are contributing to the uncertainty. We constrained the contribution of the ${0}^{+}$ (6.05 MeV) and ${3}^{\ensuremath{-}}$ (6.13 MeV) cascade transitions by measuring the asymptotic normalization coefficients for these states using the $\ensuremath{\alpha}$-transfer reaction ${}^{6}\mathrm{L}\mathrm{i}({}^{12}\mathrm{C},d{)}^{16}\mathrm{O}$ at sub-Coulomb energy. The contribution of the $0{}^{+}$ and ${3}^{\ensuremath{-}}$ cascade transitions at 300 keV is found to be $1.96\ifmmode\pm\else\textpm\fi{}0.3$ and $0.12\ifmmode\pm\else\textpm\fi{}0.04\text{ }\text{ }\mathrm{keV}\text{ }\mathrm{b}$ for destructive interference of the direct and resonance capture and $4.36\ifmmode\pm\else\textpm\fi{}0.45$ and $1.44\ifmmode\pm\else\textpm\fi{}0.12\text{ }\text{ }\mathrm{keV}\text{ }\mathrm{b}$ for constructive interference, respectively. The combined contribution of the ${0}^{+}$ and ${3}^{\ensuremath{-}}$ cascade transitions to the ${}^{12}\mathrm{C}(\ensuremath{\alpha},\ensuremath{\gamma}{)}^{16}\mathrm{O}$ reaction cross section at 300 keV does not exceed 4%. Significant uncertainties have been dramatically reduced.

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