Abstract

The differential and total cross sections for neutron emission from the d-d reaction have been measured for deuteron energies between 0.5 and 3.7 Mev. A thin deuterium gas target and an energy insensitive neutron detector were used in the measurements. The yield in the center of mass coordinates was of the form $N(\ensuremath{\theta})=K(1+A{cos}^{2}\ensuremath{\theta}+B{cos}^{4}\ensuremath{\theta}+C{cos}^{6}\ensuremath{\theta})$; the total cross section was essentially constant (0.1 barn) for deuteron energies above 1 Mev. The coefficient $A$ was found to be negative above 1.4 Mev and appreciable ${cos}^{4}\ensuremath{\theta}$ was needed at all energies. Above 2.5 Mev, a ${cos}^{6}\ensuremath{\theta}$ term was also appreciable. The angular distribution results can be understood qualitatively in terms of penetration of Coulomb and centrifugal barriers plus spin-orbit coupling.

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