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Electromagnetic dissociation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>8</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">B</mml:mi></mml:math>and the rate of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow/><mml:mrow><mml:mn>7</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">Be</mml:mi><mml:mo>(</mml:mo><mml:mi>p</mml:mi><mml:mo>,</mml:mo><mml:mi>γ</mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>8</mml:mn></mml:mrow></mml:msup></mml:mrow><mml:mi mathvariant="normal">B</mml:mi></mml:math>reaction in the Sun

B. DavidsDepartment of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824Sam M. AustinDepartment of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824D. BazinNational Superconducting Cyclotron Laboratory, Michigan State University, East Lansing, Michigan 48824H. EsbensenPhysics Division, Argonne National Laboratory, Argonne, Illinois 60439B. M. SherrillDepartment of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824I. J. ThompsonDepartment of Physics, School of Physics and Chemistry, University of Surrey, Guildford, United KingdomJ. A. TostevinDepartment of Physics, School of Physics and Chemistry, University of Surrey, Guildford, United Kingdom
2001lv
ABI

Аннотация

In an effort to better determine the ${}^{7}\mathrm{Be}(p,\ensuremath{\gamma}{)}^{8}\mathrm{B}$ reaction rate, we have performed inclusive and exclusive measurements of the Coulomb dissociation of ${}^{8}\mathrm{B}.$ The former was a study of longitudinal momentum distributions of ${}^{7}\mathrm{Be}$ fragments emitted in the Coulomb breakup of intermediate energy ${}^{8}\mathrm{B}$ beams on Pb and Ag targets. Analysis of these data yielded the $E2$ contribution to the breakup cross section. In the exclusive measurement, we determined the cross section for the Coulomb breakup of ${}^{8}\mathrm{B}$ on Pb at low relative energies in order to infer the astrophysical S factor for the ${}^{7}\mathrm{Be}(p,\ensuremath{\gamma}{)}^{8}\mathrm{B}$ reaction. Interpreting the measurements with first-order perturbation theory, we obtained ${S}_{E2}{/S}_{E1}{=4.7}_{\ensuremath{-}1.3}^{+2.0}\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}4}$ at ${E}_{\mathrm{rel}}=0.6 \mathrm{MeV},$ and ${S}_{17}{(0)=17.8}_{\ensuremath{-}1.2}^{+1.4} \mathrm{eV}\mathrm{}\mathrm{b}.$ Semiclassical first-order perturbation theory and fully quantum mechanical continuum-discretized coupled channels analyses yield nearly identical results for the $E1$ strength relevant to solar neutrino flux calculations, suggesting that theoretical reaction mechanism uncertainties need not limit the precision of Coulomb breakup determinations of the ${}^{7}\mathrm{Be}(p,\ensuremath{\gamma}{)}^{8}\mathrm{B}$ S factor. A recommended value of ${S}_{17}(0)$ based on a weighted average of this and other measurements is presented.

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