<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">Be</mml:mi></mml:mrow><mml:mrow><mml:mn>7</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mo>)</mml:mo><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">B</mml:mi></mml:mrow><mml:mrow><mml:mn>8</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Reaction
P. D. ParkerBrookhaven National Laboratory, Upton, New York
1966lv
ABI
Аннотация
Absolute cross sections for the ${\mathrm{Be}}^{7}(p,\ensuremath{\gamma}){\mathrm{B}}^{8}$ reaction have been measured at 8 proton energies between 483 and 1932 keV. These measurements have been used to obtain a zero-energy intercept of the cross-section factor $S(E)$ for this reaction, ${S}_{0}=0.043\ifmmode\pm\else\textpm\fi{}0.004$ keV barn. A resonance was observed in the ${\mathrm{Be}}^{7}(p,\ensuremath{\gamma}){\mathrm{B}}^{8}$ reaction, corresponding to the first excited state of ${\mathrm{B}}^{8}$, and a radiative width of 0.050\ifmmode\pm\else\textpm\fi{}0.025 eV was obtained for this state.
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