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L. T. BabyDepartment of Particle Physics, Weizmann Institute of Science, Rehovot, IsraelC. BordeanuDepartment of Particle Physics, Weizmann Institute of Science, Rehovot, IsraelG. GoldringDepartment of Particle Physics, Weizmann Institute of Science, Rehovot, IsraelM. HassDepartment of Particle Physics, Weizmann Institute of Science, Rehovot, IsraelL. WeissmanNSCL, Michigan State University, East Lansing, Michigan 48824V. N. FedoseyevISOLDE, CERN, Geneva, SwitzerlandU. KösterISOLDE, CERN, Geneva, SwitzerlandY. Nir-ElG. HaquinH. W. GäggelerPaul Scherrer Institute, Villigen, SwitzerlandR. WeinreichPaul Scherrer Institute, Villigen, Switzerland
2003lv
ABI

Аннотация

The ${}^{7}\mathrm{Be}(p,\ensuremath{\gamma}{)}^{8}\mathrm{B}$ reaction plays a central role in the evaluation of solar neutrino fluxes. We report on a new precision measurement of the cross section of this reaction, following our previous experiment with an implanted ${}^{7}\mathrm{Be}$ target, a raster-scanned beam, and the elimination of backscattering losses. The new measurement incorporates a higher activity ${}^{7}\mathrm{Be}$ target and a number of improvements in design and procedure. The cross section at a selected energy ${E}_{\mathrm{c}.\mathrm{m}.}=850\mathrm{keV}$ (where c.m. stands for center of mass) was measured several times under varying experimental conditions, yielding a value of ${S}_{17}{(E}_{\mathrm{c}.\mathrm{m}.}=850\mathrm{keV})=24.0\ifmmode\pm\else\textpm\fi{}0.5\mathrm{eV}\mathrm{}\mathrm{b},$ to serve as a benchmark. Measurements were carried out at lower energies as well. Due to the precise knowledge of the implanted ${}^{7}\mathrm{Be}$ density profile, it was possible to reconstitute both the off- and on-resonance parts of the cross section and to obtain from the entire set of measurements an extrapolated value of ${S}_{17}(0)=21.2\ifmmode\pm\else\textpm\fi{}0.7\mathrm{eV}\mathrm{}\mathrm{b},$ using the cluster model of Descouvemont and Baye.

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