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Vibrational and electronic spectra of alkali halides doped with CrO42− ions
Authors:S.C. Jain  A.V.R. Warrier  S.K. Agarwal
Affiliation:Solid State Physics Laboratory, Lucknow Road, Delhi-7, India
Abstract:The i.r. spectra of alkali halides doped with FrO42? ions are very sensitive to the concentration of background divalent impurities. Highly pure crystals containing CrO42? ions show a 5 line i.r. spectrum in the v3 stretch frequency region. One of these lines is attributed to CrO42? ions in perfect crystal surroundings having Td symmetry and the other 4 lines are attributed to Cs symmetry produced by a charge compensating anion vacancy in the nearest neighbour position. If the crystal contains a concentration of divalent cation impurity which is equal to or more than that of CrO42? ions, a different spectrum characteristic of C2x symmetry as well as the line corresponding to Td symmetry are obtained. The crystals of ordinary purity contain all the three (Cs, C2x and Td symmetry) species and show eight line spectra. The changes in force constants calculated from the observed splitting of the energy levels agree with those evaluated from the known polarizability of the chromate ions.At 600°C, the vibration spectra of the highly pure crystals doped with CrO42? ions show an increase in intensity of the line characteristic of Td symmetry and the other lines practically disappear, because the anion vacancies move away from the neighbourhood of the CrO42? ions at high temperatures. The energy of association of the vacancy with CrO42? ions and the energy of migration of the vacancy are derived from the spectra obtained at different temperatures and with different heat treatments.The electronic spectra of the crystals show 3 bands (at 345, 270 and 240 nm for KCI). The lowest energy band has a fine structure with a spacing of about 800 cm?1 at LAT. Since the transition involved is from a non-bonding to an antibonding state, the Condon parabola is shifted in the excited state and therefore the fine structure is attributed to a vibrational progression involving a totally symmetric frequency 800 cm?1 in the excited state.
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