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Enhancement of electrical and magnetic properties in acceptor-doped BaTiO3 ferroelectric ceramics

BaTi 1−x Mn x O 3 (x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO 3 (BTO) ceramics exhibit a tetragonal structure with P 4 mm space group via Rietveld refinement analysis. Also, the phonon mode...

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Bibliographic Details
Published in:Journal of materials science. Materials in electronics 2019-02, Vol.30 (3), p.2953-2965
Main Authors: Madhan, K., Jagadeeshwaran, C., Murugaraj, R.
Format: Article
Language:English
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Summary:BaTi 1−x Mn x O 3 (x = 0.00, 0.25, 0.50, 0.75 mol%) (BTMO) ceramics were synthesized through sol–gel combustion method. The structural studies suggested that Mn-doped BaTiO 3 (BTO) ceramics exhibit a tetragonal structure with P 4 mm space group via Rietveld refinement analysis. Also, the phonon mode at 308 cm −1 through Raman spectral analysis confirms the local structure of tetragonal symmetries. The redshift observed in UV-absorption spectra indicates a decrease of optical band gap from 3.13 to 2.71 eV with increasing Mn 2+ doping. The observed decrease in the intensity of PL emission spectra was due to an increase of Mn 2+ concentration. This indicates that a decrease in oxygen vacancies and a reduction in the number of electrons attributed to the Burstein–Moss shift. The carrier hopping process between Mn 2+ and Mn 3+ is responsible for dielectric as well as magnetization behavior. The ferroelectric double hysteresis loops are related to a ferroelectric and anti-ferroelectric order and it increases with the increase of Mn ion concentration in BTO. Through P–E measurements, the value of remnant electric polarization and coercive field found to be increased with Mn concentration in BTO samples. For BTO sample, two EPR signals with g = 1.969 and g = 2.000 singlets can be assigned with ionized Ba and Ti-vacancy defects. In addition, the EPR signal for BTMO shows a good correlation with Ti vacancies as compensating for lattice defects. Further, the Mn doping induced a weak ferromagnetic to ferromagnetic state due to free carrier concentrations.
ISSN:0957-4522
1573-482X
DOI:10.1007/s10854-018-00573-6