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16111, 223 (1985). F. E. Mitchell, and T. yon Egidy, Z. Phys. A 338, 309 (1991). F. G. Bilpuch, CR. F. A. M. R. uation analysis, we are studying the nuclide 30p via the p + 29Si reaction. C. , Phys. Rev. C45, 2746 (1992). The past year has been spent primarily in the final design azd construction of a new spectrometer to study 29Si(p,3,) with high-re_olution _,ray detectors at individual resonances. We have also worked extensively on analysis software. The program GELIFT, used to fit Ge spectra, has been modified to use the PGPLOT graphics package.

Wit88]. To predict d o'(0)/d_ corresponding to different As values, the scattering equations were solved using different 3S 1-3DI force components while keeping all other NN partial waves equal to the one-boson equivalent of the Bonn-B potential (OBEPQ-B) [Mac89]. All calculations were done for a total NN angular momentum of j _<3. We checked that restriction to those states is sufficient at the energies used in the present work. The wellestablished charge-independence breaking in the 1S o NN force was taken into account [Wit91b].

Y. A. WeidenmUller, Phys Lett. 16111, 223 (1985). F. E. Mitchell, and T. yon Egidy, Z. Phys. A 338, 309 (1991). F. G. Bilpuch, CR. F. A. M. R. uation analysis, we are studying the nuclide 30p via the p + 29Si reaction. C. , Phys. Rev. C45, 2746 (1992). The past year has been spent primarily in the final design azd construction of a new spectrometer to study 29Si(p,3,) with high-re_olution _,ray detectors at individual resonances. We have also worked extensively on analysis software. The program GELIFT, used to fit Ge spectra, has been modified to use the PGPLOT graphics package.

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Studies of Nuclear Processes


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