# STARK MODULATION SPECTROSCOPY OF SOLID HYDROGEN

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 dc.creator Kerr, Karen E. en_US dc.creator Momose, Takamasa en_US dc.creator Gabrys, C. M. en_US dc.creator Weliky, David P. en_US dc.creator Oka, T. en_US dc.date.accessioned 2006-06-15T18:52:06Z dc.date.available 2006-06-15T18:52:06Z dc.date.issued 1993 en_US dc.identifier 1993-RE-8 en_US dc.identifier.uri http://hdl.handle.net/1811/18545 dc.description $^{1}$ R. H. Hughes and E. B. Wilson. Phys. Rev., 71,562(1947). $^{2}$ E. U. Condon. Phys. Rev., 41,759(1932). $^{3}$ M. F. Crawford and I. R. Dagg. Phys. Rev., 91,1569(1953). $^{4.}$R. W. Terhune and C. W. Peters. J. Mol. Spec., 3,138(1959). en_US dc.description Author Institution: Department of Chemistry and Department of Astronomy and Astrophysics, The University of Chicago en_US dc.description.abstract E. B. Wilson and R. H. $Hughes^{1}$ invented the Stark modulation microwave spectrometer in 1947 and demonstrated the power of molecular modulation in increasing the sensitivity of spectroscopy. We report here the construction of a Stark cell for solid state spectroscopy inspired by Wilson's initial work. Unlike in gas phase microwave spectroscopy where the modulation depends on the frequency shift of spectral lines, we plan to use the intensity variation of spectral lines due to the applied electric field. Such an effect was theoretically predicted by $Condon^{2}$ and has been experimentally demonstrated in gaseous $hydrogen^{3.4}$. The field induced transitions are functions of the molecular polarizability and as such obey Raman type selection rules. We should thus observe sharp spectral lines with $\Delta k=0$. Construction of the Stark cell is in progress. We envisage that this will increase the current sensitivity of solid hydrogen spectroscopy by several orders of magnitude. en_US dc.format.extent 96751 bytes dc.format.mimetype image/jpeg dc.language.iso English en_US dc.publisher Ohio State University en_US dc.title STARK MODULATION SPECTROSCOPY OF SOLID HYDROGEN en_US dc.type article en_US