Abstract
Exact finite-range distorted-wave Born-approximation calculations have been carried out for ($d,^{3}\mathrm{He}$) and ($d,t$) reactions at incident energies up to 80 MeV. It is found that the local energy approximation does not correctly reproduce the energy variation of exact calculations for $^{51}\mathrm{V}(d,^{3}\mathrm{He})^{50}\mathrm{Ti}(\mathrm{g}.\mathrm{s}.)$ between 30 and 80 MeV and, in addition, overestimates finite-range effects for $^{16}\mathrm{O}(d,^{3}\mathrm{He})^{15}\mathrm{N}(\mathrm{g}.\mathrm{s}.)$ at 80 MeV. The effects of various choices for the range function for ($d,t$) and ($d,^{3}\mathrm{He}$) reactions are discussed. Some new values for the zero range normalization constant are discussed.NUCLEAR REACTIONS Normalization and finite-range effects in DWBA. $^{51}\mathrm{V}(d,^{3}\mathrm{He})$, $^{51}\mathrm{V}(d,t)$, $^{16}\mathrm{O}(d,^{3}\mathrm{He})$, ${T}_{d}=30\ensuremath{-}80$ MeV, calculate $\ensuremath{\sigma}(\ensuremath{\theta})$.
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