Noheda, B., Gonzalo, I.A., Guo, R., Park, S.-E., Cross, L.E., Cox, D.E. and Shirane, G. (2000) Tetragonal-to-Monoclinic Phase Transition in a Ferroelectric Perovskite: The Structure of PbZr_0.52Ti_0.48O₃. Physical Review B, 61, 8687.
http://dx.doi.org/10.1103/PhysRevB.61.8687

has been cited by the following article:

• TITLE: Structure and Dielectric Relaxation Behaviour of [Pb0.94Sr0.06][(Mn1/3Sb2/3)0.05 (Zr0.49Ti0.51)0.95]O3 Ceramics

  AUTHORS: Kumar Brajesh, Kiran Kumari

  KEYWORDS: Perovskite Oxide, Dielectric Relaxation, Rietveld Analysis

  JOURNAL NAME: World Journal of Condensed Matter Physics, Vol.5 No.3, August 21, 2015

  ABSTRACT: The field dependences of the dielectric response and conductivity are measured in a frequency range from 100 Hz to 1 MHz and in a temperature range from 300 K to about 775 K. The dielectric measurements (real and imaginary parts) of this composition with temperature (300 K - 775 K) at different frequencies (100 Hz - 1 MHz) unambiguously point towards relaxor behaviour of the material. The real part of the dielectric constant is found to decrease with increasing frequency at different temperatures while the position of dielectric loss peak shifts to higher frequencies with increasing temperature indicating a strong dispersion beyond the transition temperature, a feature known for relaxational systems such as dipole glasses. The frequency dependence of the loss peak obeys an Arrhenius law with activation energy of 0.15 eV. The distribution of relaxation times is confirmed by Cole-Cole plots as well as the scaling behavior of the imaginary part of the electric modulus. The frequency-dependent electrical data are also analyzed in the framework of the conductivity and modulus formalisms. Both these formalisms yield qualitative similarities in the relaxation times. The Rietveld analysis conforms that the materials exhibits tetragonal structure. The SEM photographs of the sintered specimens present the homogenous structures and well-grown grains with a sharp grain boundary.