Abstract

The electric resonance method of molecular beam spectroscopy was used to obtain spectra resulting from induced changes in the space-quantization of the rotational state $J=1$ of CsF in a homogeneous electric field. An analysis of the spectra for several values of the field intensity and for two different vibrational states gave the following molecular constants, ${I}_{e}=(151\ifmmode\pm\else\textpm\fi{}6){10}^{\ensuremath{-}40}$ g ${\mathrm{cm}}^{2}$, ${\ensuremath{\mu}}_{e}=(7.88\ifmmode\pm\else\textpm\fi{}0.17){10}^{\ensuremath{-}18}$ e.s.u., ${B}_{e}=(185\ifmmode\pm\else\textpm\fi{}7){10}^{\ensuremath{-}3}$ ${\mathrm{cm}}^{\ensuremath{-}1}$, ${\ensuremath{\alpha}}_{e}=(1.85\ifmmode\pm\else\textpm\fi{}0.19){10}^{\ensuremath{-}3}$ ${\mathrm{cm}}^{\ensuremath{-}1}$, ${r}_{e}=(2.34\ifmmode\pm\else\textpm\fi{}0.05){10}^{\ensuremath{-}8}$ cm, ${\ensuremath{\omega}}_{e}=(270\ifmmode\pm\else\textpm\fi{}30)$ ${\mathrm{cm}}^{\ensuremath{-}1}$. ${I}_{e}$ is the moment of inertia, ${\ensuremath{\mu}}_{e}$ is the electric dipole moment, ${B}_{e}$ and ${\ensuremath{\alpha}}_{e}$ are rotational constants, ${r}_{e}$ is the internuclear distance and ${\ensuremath{\omega}}_{e}$ is the vibrational constant.

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