Abstract
The resonant nuclear reaction $^{1}\mathrm{H}$${(}^{15}$N,\ensuremath{\alpha}\ensuremath{\gamma}${)}^{12}$C was used to measure hydrogen concentrations in thin Nb films as a function of the external ${\mathrm{H}}_{2}$ pressure (H solubility). Experiments were performed in the pressure range up to 1 mbar and temperatures between 166 and 200 \ifmmode^\circ\else\textdegree\fi{}C, i.e., in the region around the critical temperature (177 \ifmmode^\circ\else\textdegree\fi{}C) of the \ensuremath{\alpha}-\ensuremath{\alpha}' phase transition. We find that the hydrogen solubility in thin epitaxial films is considerably reduced compared to bulk data. The analysis of the data within mean-field theory for a lattice gas shows that the H-Nb interaction remains, within the experimental error, unchanged with respect to the bulk value but that the attractive H-H interaction energy is strongly reduced (0.1 eV in the film compared to 0.2 eV in the bulk). The difference is attributed to strain effects due to the clamping of the films to the substrate.
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