Electric-Field-Induced Raman Scattering in SrTiO3 and KTaO3

P. A. Fleury and J. M. Worlock
Phys. Rev. 174, 613 – Published 10 October 1968
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Abstract

In their paraelectric phases, SrTiO3 and KTaO3 crystallize in the cubic perovskite structure (space group Oh1) in which the first-order Raman effect is forbidden. We discuss here experiments in which first order Raman scattering has been induced by the application of an external electric field that serves to remove the center of inversion symmetry of the crystals. An electric field applied along a 001 direction induces a C4v symmetry in the crystal and renders all the phonons first-order Raman-active. We have studied induced scattering from all four TO phonons in SrTiO3 and from three TO phonons in KTaO3 at temperatures between 8 and 300°K and with electric fields between 0.2 to 15 kV/cm. Most attention was given to the lowest-frequency TO phonon—the "soft" or "ferroelectric" mode—whose striking decrease in frequency as the temperature is lowered signals the lattice instability associated with the ferroelectric phase transition. Detailed investigations were also made of the electric field dependence of the soft-mode frequencies in both materials. At 8°K this frequency in SrTiO3 increases from 10 cm1 at zero field to 45 cm1 at 12 kV/cm. Similar behavior is observed in KTaO3. From this behavior we infer values for the nonlinear dielectric response coefficients of the crystals. Some discussion is given of the large discrepancies between the soft-mode linewidths that we observe and those previously obtained from infrared (IR) reflectivity experiments. At 80°K in SrTiO3 the Raman and IR measurements yield values of 3 and 61.7 cm1, respectively. Additional topics considered include relative electric-field-induced scattering cross sections for the various phonon modes, and the temperature dependence of the soft-mode linewidth. Finally, the question of anomalous first-order Raman scattering in the intrinsic spectrum of SrTiO3, recently reported by several authors, is considered in the light of the field-induced first-order Raman scattering.

  • Received 1 May 1968

DOI:https://doi.org/10.1103/PhysRev.174.613

©1968 American Physical Society

Authors & Affiliations

P. A. Fleury and J. M. Worlock

  • Bell Telephone Laboratories, Holmdel, New Jersey 07733

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Issue

Vol. 174, Iss. 2 — October 1968

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