Abstract
A narrow stretching absorption band of OH/OD, polarized completely perpendicular to the ferroelectric z-axis, (at RT for OH at 3465.9 cm−1, FWHM = 3.25 cm−1 and for OD at 2561.9 cm−1, FWHM = 2.05 cm−1) is observed in the bulk of nearly stoichiometric LiNbO3 (prepared by the VTE technique [1]). These bands are about an order of magnitude more narrow than the corresponding bands in the bulk of congruent LiNbO3 at RT. The position, halfwidth and integrated absorption of the fundamental as well as the next higher vibrational transition for OH and OD are measured as a function of temperature (RT - LHeT). Electrical and mechanical anharmonicities are discussed on the basis of a Morse-type potential for a diatomic oscillator.
Additional OH and OD absorption bands [2] for OH at 4417 cm−1 and for OD at 3271 cm−1 in the bulk of nearly stoichiometric LiNbO3, are shown to belong to a libration-vibration combination band. The OH libration was also observed directly at 960 cm−1 in Raman scattering and the OD libration at 698 cm−1 in IR-reflection measurements.
The stretching absorption of OH in proton exchanged surface layers was observed in the VTE treated stoichiometric crystal to be as broad as (FWHM ≈30 cm−1, polarized completely perpendicular z) in congruent LiNbO3:PE. In both materials (congruent and stoichiometric) this structural broadered OH absorption band in the PE-layer is nearly independent of temperature.