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Astrophysical<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>S</mml:mi></mml:math>factor of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mrow/><mml:mn>3</mml:mn></mml:msup></mml:math>He<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mrow><mml:mo>(</mml:mo><mml:mi>α</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mn>7</mml:mn></mml:msup></mml:math>Be

A. KontosDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAE. UbersederDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAR. J. deBoerDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAJ. GörresDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAC. AkersDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAA. BestDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAM. CouderDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USAM. WiescherDepartment of Physics, University of Notre Dame, Notre Dame, Indiana 46556, USA
2013lv
ABI

Annotatsiya

Background: The ${}^{3}$He${(\ensuremath{\alpha},\ensuremath{\gamma})}^{7}$Be reaction is important for the neutrino production in the sun's core and the production of ${}^{7}$Li during big bang nucleosynthesis. The reaction mechanism is characterized by a strong direct capture component and nearby broad unbound resonance levels.Purpose: Recent experiments have opened up a new energy window into the reaction mechanism and it becomes more and more evident that, in order to understand the shape of the $S$ factor, theoretical calculations need to take into account possible resonance contributions from higher energies as well.Method: In the present work, a relatively wide energy window was investigated, ${E}_{c.m.}=300$--1460 keV, by detecting the prompt $\ensuremath{\gamma}$ rays from the reaction. An extensive $R$-matrix analysis was performed, utilizing all modern literature capture data, as well as elastic scattering data, which are important in constraining some $R$-matrix parameters.Results: The new experimental data agree very well with the modern literature data. The final result from the $R$-matrix fit gives a zero-energy $S$ factor of $S(0)=0.554(20)$ keV b. A table with the newly calculated reaction rate is given.Conclusions: The simultaneous $R$-matrix analysis of the ${}^{3}$He${(\ensuremath{\alpha},\ensuremath{\gamma})}^{7}$Be and ${}^{3}$He${(\ensuremath{\alpha},\ensuremath{\alpha})}^{3}$He channels yielded a reliable fit, consistent with all the included experimental data sets. In order to further constrain the reaction rate within the $R$-matrix framework, additional high-energy capture data, $\ensuremath{\gamma}$-ray angular distributions, and the inclusion of other relevant reaction channels are necessary.

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