Abstract
The kinetic-energy distribution of ions produced by a dissociative ionization process is derived, taking into account the effect of thermal motion of the target molecule. In the case of dissociative attachment of monoenergetic electrons to a diatomic molecule, the width at half-maximum of the negative-ion energy distribution is given by ${(11\ensuremath{\beta}\mathrm{kT}{E}_{0})}^{\frac{1}{2}}$, where $\ensuremath{\beta}$ is the ratio of the mass of the ion to that of the parent molecule, $T$ is the target-gas temperature, and ${E}_{0}$ is the most probable ion energy. Using a crossed-field velocity filter, ${\mathrm{O}}^{\ensuremath{-}}$ ion energy distributions arising from the attachment of essentially monoenergetic electrons to ${\mathrm{O}}_{2}$ are studied as a function of electron energy at two gas temperatures. The measured widths of the distributions are consistent with the above relationship. Measurements of ${E}_{0}$ as a function of the electron energy allow a determination of the electron affinity $A$ of atomic oxygen. The result, $A=1.5\ifmmode\pm\else\textpm\fi{}0.1$ eV, is in excellent agreement with photodetachment-threshold determinations.
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