<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Be</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>7</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">p</mml:mi><mml:mo>,</mml:mo><mml:mi> </mml:mi><mml:mi>γ</mml:mi><mml:mo>)</mml:mo><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">B</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>8</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>cross section at low energy
F. C. BarkerDepartment of Theoretical Physics, Research School of Physical Sciences, Australian National University, Cannberra, Australian Capital Territory 2601, Australia
1983lv
ABI
Аннотация
The low-energy logarithmic derivative of the $S$ factor for $^{7}\mathrm{Be}(\mathrm{p}, \ensuremath{\gamma})^{8}\mathrm{B}$ calculated by Williams and Koonin using only asymptotic wave functions differs from that obtained with a potential model. It is suggested that this is due at least in part to an inappropriate choice of nuclear phase shift in the former calculation.NUCLEAR REACTIONS $^{7}\mathrm{Be}(\mathrm{p}, \ensuremath{\gamma})^{8}\mathrm{B}$, $E<100$ keV, extrapolated $S$.
Ҳали таржима қилинмаган
Идентификаторлар
Иқтибослар ва манбалар
2 та иқтибос0 та фойдаланилган манба