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The effects of finite off-normal-incidence angle on the polarized-reflectivity spectra of aluminum phosphate have been investigated in great detail. An unambiguous identification of the extra structure, which manifests itself at 525 cm^-1 in the Γ₂(p) or transverse-magnetic (TM) configuration, has been made. It comes from a strong Γ₃ mode, of which the LO component couples to the light for nonzero values of the angle of incidence. For typical experimental conditions, this results in the appearance of a pronounced extra structure which does not belong to the symmetry of the components under investigation. The corresponding intensity is well accounted for by the appropriate Fresnel equations. Nothing else similar to it appears in the higher-frequency range (where a second Γ₃ mode exists near 1200 cm^-1) or in the lower-frequency part of the spectrum (around 380 cm^-1, where a second additional band was previously identified). In the latter case, no obvious connection with a Γ₃ mode could be discerned. Finally, from the data collected in the pure s (transverse-electric) polarization for both Γ₂ and Γ₃ components, an improved series of transverse and longitudinal phonon frequencies, oscillator strengths, and broadening parameters could be deduced. This gives a better account of the dispersion of the refractive index of aluminum phosphate in the range from 100 to 1500 cm^-1.
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Goullet et al. (1989) studied this question.
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