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Evaluation of modern<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>(<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>α</mml:mi></mml:mrow></mml:math>,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><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">Be</mml:mi><mml:mprescripts/><mml:none/><mml:mrow><mml:mn>7</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>data

R. H. CyburtJoint Institute for Nuclear Astrophysics (JINA) and National Superconducting Cyclotron Laboratory (NSCL), Michigan State University, East Lansing, Michigan 48824, USAB. DavidsJoint Institute for Nuclear Astrophysics (JINA) and National Superconducting Cyclotron Laboratory (NSCL), Michigan State University, East Lansing, Michigan 48824, USA
2008lv
ABI

Аннотация

In both the Sun and the early universe, the $^{3}\mathrm{He}$($\ensuremath{\alpha}$, $\ensuremath{\gamma}$)$^{7}\mathrm{Be}$ reaction plays a key role. The rate of this reaction is the least certain nuclear input needed to calculate both the primordial $^{7}\mathrm{Li}$ abundance in big-bang nucleosynthesis and the solar neutrino flux. Taking advantage of several recent highly precise experiments, we analyze modern $^{3}\mathrm{He}$($\ensuremath{\alpha}$, $\ensuremath{\gamma}$)$^{7}\mathrm{Be}$ data using a robust and minimally model-dependent approach capable of handling discrepant data sets dominated by systematic rather than statistical errors. We find ${S}_{34}(0)=0.580\ifmmode\pm\else\textpm\fi{}0.043(0.054)$ keV b at the 68.3(95.4)% confidence level.

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Цитирований: 4Использованных источников: 0