Abstract
The infrared spectra of matrix‐isolated RbOH, RbOD, NaOH, and NaOD have been observed. Both the alkali‐metal–oxygen stretch ν1 and the bending mode ν2 have been assigned for each species. The metal–oxygen stretching mode is found at 354.4, 345, 431, and 422 cm−1 for RbOH, RbOD, NaOH, and NaOD, respectively; the bending mode ν2 is observed at 309.0, 229, 337, and 250 cm−1, respectively. Combination of the results of this study with the microwave measurements for RbOH and RbOD indicates an essentially linear structure for these species. The isotope shift for ν2 observed in NaOH coupled with reasonable bond lengths indicates an equilibrium configuration of NaOH which probably does not deviate significantly from linearity. The assumption of a linear model with a harmonic bending potential yields force constants of 0.046 × 10−18 and 0.053 × 10−18 Nm (0.046 and 0.053 mdyn·Å) for RbOH and NaOH, respectively. These results are consistent with our previously reported results for CsOH.