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Polarized IR spectra of synthetic smoky quartz

โœ Scribed by R. Pankrath


Publisher
Springer-Verlag
Year
1991
Tongue
English
Weight
929 KB
Volume
17
Category
Article
ISSN
0342-1791

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โœฆ Synopsis


Polarized IR spectra of planeparallel (0001) plates of synthetic smoky quartz, with E rotating around [0001], show that the absorption figures of OH-related absorption bands at 3380 (room temperature), 3365 and 3305 cm-1 (liquid nitrogen temperature, -196 ~ C) are strongly anisotropic and violate the trigonal symmetry of low quartz. This effect is correlated with a non-uniform substitution of Si by A1 on the three symmetrically equivalent Si sites, as revealed by EPR measurements. Random distribution of A1 over the three Si sites, obtained by dry annealing of the samples in air, yields isotropic absorption figures in the (0001) plates. It is thus experimentally evident that the absorption bands at 3380, 3365 and 3305cm -1 are caused by the OHstretching vibrations coupled with A1 substituting for Si. For each experimentally determined integral absorption coefficient of the three absorption bands a theoretical absorption coefficient was calculated, based on the symmetry of low quartz and the given A1 distribution. This was done for various orientations of the OH-dipoles with respect to the a axes of low quartz. By comparing the experimentally determined and calculated absorption coefficients, the orientation of the corresponding OH-dipoles with respect to the a axes could be determined.


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## IR and Raman spectra of K,P,O1,Te(OH),2D,O and K,P,0,zTe(OH),2H,0 have been recorded and analysed. The P,O,, modes are assigned on the basis of characteristic vibrations of the POP and POz groups. The P,O:; ion has C,, symmetry and the P,O,, and TeO, groups coexist in this compound. Two crystal