Structural, Optical, and Magnetic Properties of Brownmillerite KBiFe<sub>2</sub>O<sub>5</sub> and KBiFe<sub>1.95</sub>Ti<sub>0.05</sub>O<sub>5+</sub> via Reactive Templated Method

Brownmillerite KBiFe<sub>2</sub>O<sub>5</sub> (KBFO) and KbiFe<sub>1.95</sub>Ti<sub>0.05</sub>O<sub>5+</sub> (KBFTO) ceramics were synthesized using the prereacted nanopowders of KFeO<sub>2</sub> (KFO) and BiFeO<sub>3</sub> (BFO), and KFO and BiFe<sub>0.95</sub>Ti<sub>0.05</sub>O<sub>3+</sub> (BFTO), respectively, via the reactive templated method. The powder X-ray diffraction patterns confirmed the monoclinic phase of the KBFO and KBFTO samples. The incorporation of Ti<sup>4+</sup> at Fe<sup>3+</sup> site prevented the formation of a secondary phase (Bi<sub>2</sub>Fe<sub>4</sub>O<sub>9</sub>) in the KBFTO sample. Our experimentally determined lattice parameters for the orthorhombic <i>P</i>2/<i>c</i> KBFO and KBFTO are consistent with our density functional theory (DFT) computed lattice parameters (within a 5% error). Scanning electron microscopy images revealed an average grain size of ∼1.38 and 0.85 μm for KBFO and KBFTO, respectively. The calculated optical band gaps of the KBFO and KBFTO using the Kubelka-Munk function from their UV data were found to be 1.69 and 1.71 eV, respectively. The measured surface area of KBFTO (1.339 m<sup>2</sup> g<sup>-1</sup>) obtained from BET analysis was double that of KBFO (0.698 m<sup>2</sup> g<sup>-1</sup>). KBFTO's room-temperature magnetization was 0.986 emu g<sup>-1</sup>, which was twice that of the KBFO, while its room-temperature conductivity measured using impedance spectroscopy was 5.69 × 10<sup>-3</sup> S m<sup>-1</sup> which was 10 times that of KBFO. Notably, our DFT calculations showed that the small Ti dopant concentration enhanced the partial density of states (PDOS) above the Fermi level. It shifted the Fermi level toward higher energy, and the oxygen PDOS for KBFTO was significantly enhanced relative to KBFO, which ultimately helped improve the conductivity.

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Publication Details

Journal
ACS Omega
Published
2024-10-17
DOI
https://doi.org/10.1021/acsomega.4c07882
Citations
8
Primary Topic
Multiferroics and related materials
Type
article
Field-Weighted Citation Impact
0.94

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article

Structural, Optical, and Magnetic Properties of Brownmillerite KBiFe2O5 and KBiFe1.95Ti0.05O5+ via Reactive Templated Method

Rajasekhar Bhimireddi, Lokeswararao Dhavala, Anees A. Ansari, Apparao M. Rao et al.
8 citations
ACS Omega
Multiferroics and related materials
0.94
article

Structural, Optical, and Magnetic Properties of Brownmillerite KBiFe2O5 and KBiFe1.95Ti0.05O5+ via Reactive Templated Method

Rajasekhar Bhimireddi, Lokeswararao Dhavala, Anees A. Ansari, Apparao M. Rao, K. Kanmani Raja, Peshal Karki, A.V. Anupama
article en
8 citations

Abstract

Brownmillerite KBiFe<sub>2</sub>O<sub>5</sub> (KBFO) and KbiFe<sub>1.95</sub>Ti<sub>0.05</sub>O<sub>5+</sub> (KBFTO) ceramics were synthesized using the prereacted nanopowders of KFeO<sub>2</sub> (KFO) and BiFeO<sub>3</sub> (BFO), and KFO and BiFe<sub>0.95</sub>Ti<sub>0.05</sub>O<sub>3+</sub> (BFTO), respectively, via the reactive templated method. The powder X-ray diffraction patterns confirmed the monoclinic phase of the KBFO and KBFTO samples. The incorporation of Ti<sup>4+</sup> at Fe<sup>3+</sup> site prevented the formation of a secondary phase (Bi<sub>2</sub>Fe<sub>4</sub>O<sub>9</sub>) in the KBFTO sample. Our experimentally determined lattice parameters for the orthorhombic <i>P</i>2/<i>c</i> KBFO and KBFTO are consistent with our density functional theory (DFT) computed lattice parameters (within a 5% error). Scanning electron microscopy images revealed an average grain size of ∼1.38 and 0.85 μm for KBFO and KBFTO, respectively. The calculated optical band gaps of the KBFO and KBFTO using the Kubelka-Munk function from their UV data were found to be 1.69 and 1.71 eV, respectively. The measured surface area of KBFTO (1.339 m<sup>2</sup> g<sup>-1</sup>) obtained from BET analysis was double that of KBFO (0.698 m<sup>2</sup> g<sup>-1</sup>). KBFTO's room-temperature magnetization was 0.986 emu g<sup>-1</sup>, which was twice that of the KBFO, while its room-temperature conductivity measured using impedance spectroscopy was 5.69 × 10<sup>-3</sup> S m<sup>-1</sup> which was 10 times that of KBFO. Notably, our DFT calculations showed that the small Ti dopant concentration enhanced the partial density of states (PDOS) above the Fermi level. It shifted the Fermi level toward higher energy, and the oxygen PDOS for KBFTO was significantly enhanced relative to KBFO, which ultimately helped improve the conductivity.

ACS OmegaVol. 9(43)
Mahatma Gandhi Memorial Medical College (IN), King Saud University (SA), Nanomaterials Research (United States) (US), Sri Sathya Sai Institute of Higher Learning (IN), Clemson University (US)
Clemson University
Openalex Percentile: Top 28%
Multiferroics and related materials
0.94
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