Issue |
Eur. Phys. J. Appl. Phys.
Volume 53, Number 2, February 2011
|
|
---|---|---|
Article Number | 20901 | |
Number of page(s) | 10 | |
Section | Imaging, Microscopy and Spectroscopy | |
DOI | https://doi.org/10.1051/epjap/2010100073 | |
Published online | 28 January 2011 |
https://doi.org/10.1051/epjap/2010100073
Dielectric and structural properties of diffuse ferroelectric phase transition in Pb1.85K1.15Li0.15Nb5O15 ceramic
1
LMCN, F.S.T.G. University Cadi Ayyad Marrakech, Marrakech, Morocco
2
LPMC, Université de Picardie, 33 rue Saint-Leu, 80039 Amiens Cedex, France
3
LPMC, Équipe Physique de l'environnement, Université Chouaib DoukKali, F.S. El Jadida, Morocco
4
University of Nîmes, Department of Sciences, Rue du Dr Georges Salan, 30021 Nîmes Cedex 01, France and C2M, Institut C. Gerhardt, UMR-CNRS 5253, 34095 Montpellier Cedex 05, France
5
Dipartimento di Fisica, Universita di Roma II “Tor Vergata”, Via della Ricerca Scientifica, 00133 Roma, Italy
Corresponding author: mezdaoud@yahoo.fr
Received:
12
February
2010
Revised:
28
September
2010
Accepted:
22
November
2010
Published online:
28
January
2011
We studied the structural and dielectric properties of new Tetragonal Tungsten Bronze (TTB) ceramics Pb1.85K1.15Li0.15Nb5O15 that was synthesized by solid-state reaction. We pay a special attention to the diffuse phase transition (DPT) that occurs close to 425 °C. Using dielectric measurements in a frequency range of 10 Hz–1 MHz and in the temperature range 30–560 °C, we have shown that the real permittivity close to DPT is well described by Santos-Eiras phenomenological model. Space-charge polarization, relaxation phenomena and free charges conductivity have been analyzed using dielectric spectroscopy impedance and modulus characterization. Cole-Cole plots show a non-Debye (polydispersive) type relaxation. In paraelectric phase the Arrhenius activation energy was determined as Eτ = 0.72 eV. We demonstrated that frequency dependence of ac conductivity at different temperatures obeys the Jonscher's universal law: σac = σdc + A(ω)n.
© EDP Sciences, 2011
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