The proton polarization angular distributions from the following reactions have been measured: ${\mathrm{C}}^{12}\mathrm{}(d,p)\mathrm{}{\mathrm{C}}^{13*}(3.09\mathrm{} \mathrm{MeV},l_n=0)$; ${\mathrm{Mg}}^{24}\mathrm{}(d,p)\mathrm{}{\mathrm{Mg}}^{25}(\mathrm{g}.\mathrm{s}.\mathrm{},l_n=2,\mathrm{and} 0.58 \mathrm{MeV},l_n=0)$; ${\mathrm{Be}}^9\mathrm{}(d,p)\mathrm{}{\mathrm{Be}}^{10}(\mathrm{g}.\mathrm{s}.\mathrm{},l_n=1,\mathrm{and} 3.37 \mathrm{MeV},l_n=1)$; ${\mathrm{Si}}^{28}\mathrm{}(d,p)\mathrm{}{\mathrm{Si}}^{29*}(1.28\mathrm{} \mathrm{MeV},l_n=2)$. The incident deuteron energy was 15 MeV. Carbon and helium were used as polarization analyzers. The results are discussed in terms of distorted-wave theory. In addition to the polarization measurements, the differential cross section of deuterons elastically scattered from aluminum, silicon, and beryllium has been determined.

• Received 19 July 1963

DOI:https://doi.org/10.1103/PhysRev.133.B1155