4.6 Article

Broadband dielectric spectroscopy of phonons and polar nanoclusters in PbMg1/3Nb2/3O3-35%PbTiO3 ceramics: Grain size effects

Journal

PHYSICAL REVIEW B
Volume 79, Issue 10, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.79.104111

Keywords

dielectric relaxation; disperse systems; ferroelectric ceramics; ferroelectric transitions; grain boundaries; grain size; harmonic generation; lead compounds; nanostructured materials; percolation; permittivity; phonon spectra; terahertz wave spectra

Funding

  1. Czech Science Foundation [202/06/0403, 202/09/0682]
  2. Academy of Sciences of the Czech Republic [AVOZ 10100520, KJB 100100704]
  3. Ministry of Education [COST-OC 101]

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The dielectric response of PbMg1/3Nb2/3O3-35%PbTiO3 ceramics (close to the morphotropic phase boundary) from 100 Hz up to 100 THz was determined in a broad temperature range of 5-900 K. Two ceramics were studied and compared: coarse grain ceramics (CGC) (grain size similar to 4 mu m) and fine grain ceramics (FGC) (grain size similar to 150 nm). Both ceramics showed similar polar-phonon response and the ferroelectric transition near T-C=440 K that was manifested by partial softening of the overdamped lowest-frequency phonon using the time-domain THz spectroscopy. However, the dielectric response was dominated by a complex relaxational dispersion in the microwave range due to relaxorlike dynamics of the polar nanoclusters, which strongly differed in both the ceramics. Whereas the CGC undergoes a well-defined ferroelectric transition such as a single crystal, FGC exhibits a relaxor behavior with substantially smaller permittivity showing partial clamping of the polar nanocluster dynamics by grain boundaries. The pronounced difference was also revealed in a second-harmonic generation showing much larger paraelectric signal in the FGC with a much smeared ferroelectric transition only. Due to contributions of both the soft phonon mode and dielectric relaxations into the dielectric constant near its maximum even in the paraelectric phase, the ferroelectric transition corresponds to a percolation threshold of the polar nanoclusters into macroscopic domains. Such a type of phase transition can be considered as a special case of crossover between the displacive and order-disorder types, where the ordering process concerns a mesoscopic range.

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