Abstract
The angular distribution of the disintegration protons from the D-D reaction has been investigated as a function of energy from 60 kev to 390 kev. The distribution was found to be well represented by $\mathrm{I}(\ensuremath{\theta})=1+A{cos}^{2}\ensuremath{\theta}$ at any one energy. The value of $A$ increases smoothly with bombarding energy over the range investigated.
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