Abstract
The integral intensity of second-harmonic light or hyper-Rayleigh scattering from nominally pure KTaO3 is measured as a function of both scattering geometry and temperature between 10 and 200 K. Evidence is found that hyper-Rayleigh scattering results from an activation of the soft-mode hyper-Raman tensor by quasistatic lattice distortions and macroscopic electric fields.