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Phys. Rev. B 4, 1360–1366 (1971)

Raman Spectra and Lattice Dynamics of α-Berlinite (AlPO4)

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J. F. Scott*
Department of Natural Philosophy, University of Edinburgh, Edinburgh, Scotland

Received 4 December 1970; published in the issue dated 15 August 1971

Using the Born-von Karman and rigid-ion models of Elcombe for the optical phonons in α-quartz, we have analyzed the Raman spectra of isomorphic AlPO4 (berlinite). The resulting analysis yields several physical parameters which are not accessible to any other experimental measurement; for example, the dispersion of phonon branches in the high-frequency region. Since the AlPO4 Brillouin zone is halved in the [00ζ] direction compared with that of quartz, phonons characteristic of critical point A in quartz are Raman active in AlPO4. The near equivalence of Al + P and 2Si masses and of phonon frequencies experimentally determined in SiO2 and AlPO4 demonstrates that a significant amount of charge compensation exists in AlPO4, such that Al and P each have a nominal valence of ∼ +4, rather than +3 and +5. This is confirmed by the measured LO/TO splitting of modes which would be described as having wave vector (0,0,π/c) in quartz: If Al and P charges and masses were identical, these degeneracies would remain unsplit by the lattice Coulomb field. The small splittings we observe (7-19 cm-1) for each transverse/longitudinal doublet allow us to determine the difference in effective charge for Al and P ions. An estimate of Z(P)-Z(Al)0.2e is obtained from the rigid-ion expression 4π2Σj(ωLO,j2-ωTO,j2)=(4π/V)ΣkZk2/mk, and values Z(P)=2.4e, Z(Al)=2.2e, Z(O)=-1.15e deduced.

© 1971 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.4.1360
DOI:
10.1103/PhysRevB.4.1360
PACS:

*Permanent address: Bell Telephone Laboratories, Holmdel, N. J. 07733.