4.7 Article

Effects of sintering temperature on microstructure and giant dielectric properties of (V plus Ta) co-doped TiO2 ceramics

Journal

JOURNAL OF ALLOYS AND COMPOUNDS
Volume 725, Issue -, Pages 310-317

Publisher

ELSEVIER SCIENCE SA
DOI: 10.1016/j.jallcom.2017.07.143

Keywords

Rutile-TiO2; Giant dielectric permittivity; Impedance spectroscopy; Ceramic microstructure; X-ray photoelectron spectroscopy; Grain size

Funding

  1. Thailand Research Fund (TRF)
  2. Khon Kaen University, Thailand [RSA5880012]
  3. Nanotechnology Center (NANOTEC)
  4. NSTDA
  5. Ministry of Science and Technology, Thailand through program of Center of Excellence Network
  6. Environment Research Unit [P1551019]
  7. National Metal and Materials Technology Center
  8. Thailand Graduate Institute of Science and Technology (TGIST) [SCA-CO-2558-1033-TH]

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The influences of sintering temperature on the microstructure and giant dielectric properties of a new co-doped TiO2 system, i.e., V and Ta co-doped TiO2, were investigated. The grain size of (V1/2Ta1/2)(0.01)Ti0.99O2 ceramics was enlarged with increasing sintering temperature. Dense microstructure and homogeneous dispersion of dopants were achieved in the ceramics sintered at 1400-1500 degrees C for 5 h. The dielectric permittivity in the frequency range 40-10(6) Hz of the (V1/2Ta1/ 2) 0.01Ti0.99O2 ceramics significantly increased with the mean grain size, while the dielectric loss tangent was reduced to 0.033 at 10(2) Hz. Furthermore, the high-temperature stability of the dielectric permittivity was improved with increasing mean grain size. The electrically heterogeneous microstructure consisting of semiconducting grains and insulating grain boundaries and/or surface layers was confirmed using impedance spectroscopy. The conduction inside the semiconducting grains was attributed to electron hopping between Ti4+ and Ti3+, which was confirmed by X-ray photoelectron spectroscopy. Very high resistivity with a large conduction activation energy of the insulating parts was suggested as the primary cause of the giant dielectric permittivity with low loss tangent. (C) 2017 Elsevier B.V. All rights reserved.

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