We report on the experimental investigation of a high-frequency ͑1 MHz-1.8 GHz͒ dielectric dispersion in unpoled and poled Pb͑Zr, Ti͒O 3 ceramics. Two overlapping loss peaks could be revealed in the dielectric spectrum. The linear dependence between the lower-frequency peak position and average grain size D , which holds for D Յ 10 m, indicates that the corresponding polarization mechanism originates from piezoelectric resonances of grains. The intensity of the higher-frequency peak is drastically reduced by poling. It is thus proposed that this loss peak is related to domain wall contribution to the dielectric dispersion. © 2009 American Institute of Physics. ͓DOI: 10.1063/1.3147166͔It has been often observed that the lattice permittivity of ferroelectric materials is significantly lower than the permittivity measured at conventionally accessible frequencies, say below 1 MHz. Perhaps the most striking manifestation of this difference is seen in the strong, steplike dispersion of the permittivity accompanied by the loss peak in the frequency range from 10 8 to 10 10 Hz. [1][2][3] Above this frequency range, the permittivity is close to that of the lattice. Several mechanisms have been proposed to explain origins of the dispersion, including resonance of domain walls, 4 translational vibration of domain walls, 5 acoustic shear waves generation by stacks of lamellar 90°domains, 6 and piezoelectric resonance of grains. 7 Some authors have proposed that the dispersion is related to motion of individual ions between off-center position. 8 Being quite far from the state that permits quantitative description, the proposed mechanisms are sometimes arbitrarily invoked to explain any kind of dispersion observed in this frequency range, thus causing controversy and confusion. Most studies usually assign only one mechanism to the high frequency dispersion in a given ferroelectric material. 4,[6][7][8] However, there is no reason why several dispersive processes cannot contribute to the permittivity simultaneously. This is particularly true for piezoelectric resonances of grains and mechanisms related to domain wall displacement. Domain size ͑distance between neighboring domain walls͒ and grain size are coupled 9 and their contribution to the dielectric dispersion may occur in the narrow frequency range. The model of Pertsev and Arlt, 5 for example, suggests that resonance frequency of domain walls may be lower than the frequency of the elastic resonance of grains. The aim of this investigation is thus to specifically address the contribution of grain resonances and domain walls to the dielectric dispersion in 10 8 to 10 10 Hz range in technologically important ferroelectric, Pb͑Zr, Ti͒O 3 or PZT.In order to obtain samples with broad range of average grain size, we take advantage of the fact that in PZT grain size can be significantly affected by dopants. 10 Therefore, the samples of hard and soft PZT ceramics were prepared by a conventional solid state process using standard mixed oxide route. The Zr/Ti ratio ͑in at. %͒ was...