Abstract
The first vibrational overtone spectrum of solid parahydrogen with various low orthohydrogen impurity levels has been studied in the range 7900--10 000 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$ using a White-type external multireflection system with a 34.8-cm sample path length. We were able to detect extremely weak features, namely, the ${\mathrm{Y}}_{1}$(0) at 7991.85 (1) ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$, and the double transitions ${\mathrm{U}}_{1}$(0) + ${\mathrm{Q}}_{1}$(1), ${\mathrm{U}}_{1}$(0) + ${\mathrm{S}}_{1}$(0), ${\mathrm{U}}_{1}$(1) + ${\mathrm{Q}}_{1}$(0), and ${\mathrm{Q}}_{1}$(0) + ${\mathrm{Q}}_{1}$(0). The ${\mathrm{Q}}_{1}$(0) + ${\mathrm{Q}}_{1}$(1) and ${\mathrm{Q}}_{1}$(1) + ${\mathrm{Q}}_{1}$(1) double transitions were resolved. We obtained a rich orthohydrogen satellite spectrum associated with the transitions ${\mathrm{Q}}_{2}$(0) and ${\mathrm{Q}}_{2}$(1) near 8060 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$. An analysis and assignment of these satellite transitions are presented. The double transitions of the type ${\mathrm{Q}}_{1}$(J) + ${\mathrm{Q}}_{1}$(${\mathrm{J}}^{|\mathrm{I}\mathrm{H}}$) (J,${\mathrm{J}}^{|\mathrm{I}\mathrm{H}}$ = 0,1) are located in the spectral region around 8300 ${\mathrm{cm}}^{\mathrm{\ensuremath{-}}1}$. The most remarkable features here are the ${\mathrm{Q}}_{1}$(1) + ${\mathrm{Q}}_{1}$(1) transition, which consists entirely of fine structure, and the ${\mathrm{Q}}_{1}$(0) + ${\mathrm{Q}}_{1}$(0) transition, which, to our knowledge, has an intensity that cannot be accounted for by previously proposed mechanisms. Finally the thermal shift of all of the above-mentioned transitions was investigated by lowering the sample temperature from 12.5 K down to 6.5 K while taking spectra. The influence of the change of temperature on the line positions, linewidths, and interaction parameters of solid hydrogen is discussed.
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