Study of Alternative Current Conduction Mechanisms on the α‐LiFeO<sub>2</sub>‐Based Cathode Materials

ABSTRACT An improved solid‐state synthesis method was used to create LiFeO 2 layered oxides. The produced material adopts a cubic system (Fm‐3m space group) with a refined cell parameter of a = 4.156(9) Å, as indicated by Rietveld refinement of the crystal structure. A morphological investigation revealed that the sample is composed of small primary particles with sizes ranging from 0.20 to 0.75 μm. IR spectroscopy vibrational analysis revealed the presence of FeO 6 and LiO 6 groups. The compound's semiconductor nature was confirmed when the band gap energy was generated and discovered to be 2 eV. There is a tighter dispersion of localized states within the band gap, as indicated by the obtained Urbach energy (0.39 eV), which presents just 20% from the band gap energy. The material's dielectric characteristics were assessed between 0.1 and 107 Hz in frequency and between 333 K and 523 K in temperature. The presence of both space charge and dipolar polarization is suggested by the real component of the dielectric permittivity, which indicates a high dielectric constant (between 100 and 350) at low frequency. The circuits are made up of constant phase elements (CPE) and bulk resistance R coupled in parallel. Jonscher's law was applied to interpret the frequency‐dependent conductivity. The outcomes of the charge transport investigation on LiFeO 2 imply that the layered oxide material possessed a large polaron tunneling (OLPT) paradigm with activation energy E a of 0.26 eV. Comparing the polaron R ω (2 &lt; R ω &lt; 5 Å) optimal hopping length to the Li–O interatomic gap (2.077(9) Å), it is larger. We identified and examined a correlation between the ionic conductivity and the crystal structure.

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Publication Details

Journal
Applied Organometallic Chemistry
Published
2025-03-17
DOI
https://doi.org/10.1002/aoc.70088
Citations
3
Primary Topic
Advancements in Battery Materials
Type
article
Field-Weighted Citation Impact
2.19
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article

Study of Alternative Current Conduction Mechanisms on the α‐LiFeO2‐Based Cathode Materials

Hala Siddiq, Abdallah Ben Rhaiem, Narimen Chakchouk, Mohamed Houcine Dhaou et al.
3 citations
Applied Organometallic Chemistry
Advancements in Battery Materials
2.19
article

Study of Alternative Current Conduction Mechanisms on the α‐LiFeO2‐Based Cathode Materials

Hala Siddiq, Abdallah Ben Rhaiem, Narimen Chakchouk, Mohamed Houcine Dhaou, Saleh M. Altarifi, Abdulaziz Abdulmohsen Alnafea
article en
3 citations

Abstract

ABSTRACT An improved solid‐state synthesis method was used to create LiFeO 2 layered oxides. The produced material adopts a cubic system (Fm‐3m space group) with a refined cell parameter of a = 4.156(9) Å, as indicated by Rietveld refinement of the crystal structure. A morphological investigation revealed that the sample is composed of small primary particles with sizes ranging from 0.20 to 0.75 μm. IR spectroscopy vibrational analysis revealed the presence of FeO 6 and LiO 6 groups. The compound's semiconductor nature was confirmed when the band gap energy was generated and discovered to be 2 eV. There is a tighter dispersion of localized states within the band gap, as indicated by the obtained Urbach energy (0.39 eV), which presents just 20% from the band gap energy. The material's dielectric characteristics were assessed between 0.1 and 107 Hz in frequency and between 333 K and 523 K in temperature. The presence of both space charge and dipolar polarization is suggested by the real component of the dielectric permittivity, which indicates a high dielectric constant (between 100 and 350) at low frequency. The circuits are made up of constant phase elements (CPE) and bulk resistance R coupled in parallel. Jonscher's law was applied to interpret the frequency‐dependent conductivity. The outcomes of the charge transport investigation on LiFeO 2 imply that the layered oxide material possessed a large polaron tunneling (OLPT) paradigm with activation energy E a of 0.26 eV. Comparing the polaron R ω (2 &lt; R ω &lt; 5 Å) optimal hopping length to the Li–O interatomic gap (2.077(9) Å), it is larger. We identified and examined a correlation between the ionic conductivity and the crystal structure.

Applied Organometallic ChemistryVol. 39(4)
University of Sfax (TN), Qassim University (SA), Jazan University (SA)
Openalex Percentile: Top 13%
Advancements in Battery Materials
2.19
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