<p>In this work, α-LiFe<sub>5</sub>O<sub>8</sub> with a macro–mesoporous structure was synthesized using a multistep process. X-ray diffraction and Rietveld refinement confirm the formation of a single-phase, highly crystalline α-LiFe<sub>5</sub>O<sub>8</sub> with an ordered cubic spinel structure (P4<sub>3</sub>32), free of secondary phases after calcination. Scanning Electron Microscopy (SEM) reveals, an interconnected sponge-like mesoporous structure (~ 10&#xa0;nm), while electron paramagnetic resonance (EPR) confirms temperature-dependent Fe<sup>3+</sup> super-exchange interactions in α-LiFe<sub>5</sub>O<sub>8</sub>. Over the studied temperature range α-LiFe<sub>5</sub>O<sub>8</sub> exhibits semiconducting behavior. This semiconducting behavior is linked to the thermal activation of the small-polaron hopping transport process. Between 380 and 428&#xa0;K, the dc conductivity of α-LiFe<sub>5</sub>O<sub>8</sub> becomes nearly temperature-independent, confirming the stability of conductivity with temperature. The electrical transport analysis reveals a temperature-dependent transition between distinct conduction mechanisms. At low temperatures, charge carriers follow Mott variable-range hopping (VRH), indicating strong localization within disordered states. In the intermediate region, the data fit the Shklovskii–Efros VRH, confirming the influence of Coulomb gap-controlled hopping. At higher temperatures, the transport is governed by the small-polaron hopping (SPH) mechanism, consistent with thermally activated carrier mobility. These results provide a coherent picture of the conduction behavior across the full investigated temperature range. For all measured temperatures, the conductivity spectra of α-LiFe<sub>5</sub>O<sub>8</sub> are examined via universal power law, revealing a characteristic dispersive behavior. The material exhibits pronounced negative temperature coefficient behavior, characterized by two NTCR values (− 4.31% K<sup>−1</sup> at 343&#xa0;K and − 3.40% K<sup>−−1</sup> at 433&#xa0;K), highlighting the strong potential of α- LiFe<sub>5</sub>O<sub>8</sub> for thermistor and temperature sensing applications.</p>

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Electrical transport mechanisms and structural properties of α-LiFe5O8 macro-mesoporous ferrite prepared by an auto-combustion route

  • Adnene Midouni,
  • Youssef Moualhi,
  • Siwar Guinou,
  • S. Elkossi,
  • H. Rahmouni,
  • Anissa Somrani,
  • Ahmed Hichem Hamzaoui,
  • Mouna Jaouadi

摘要

In this work, α-LiFe5O8 with a macro–mesoporous structure was synthesized using a multistep process. X-ray diffraction and Rietveld refinement confirm the formation of a single-phase, highly crystalline α-LiFe5O8 with an ordered cubic spinel structure (P4332), free of secondary phases after calcination. Scanning Electron Microscopy (SEM) reveals, an interconnected sponge-like mesoporous structure (~ 10 nm), while electron paramagnetic resonance (EPR) confirms temperature-dependent Fe3+ super-exchange interactions in α-LiFe5O8. Over the studied temperature range α-LiFe5O8 exhibits semiconducting behavior. This semiconducting behavior is linked to the thermal activation of the small-polaron hopping transport process. Between 380 and 428 K, the dc conductivity of α-LiFe5O8 becomes nearly temperature-independent, confirming the stability of conductivity with temperature. The electrical transport analysis reveals a temperature-dependent transition between distinct conduction mechanisms. At low temperatures, charge carriers follow Mott variable-range hopping (VRH), indicating strong localization within disordered states. In the intermediate region, the data fit the Shklovskii–Efros VRH, confirming the influence of Coulomb gap-controlled hopping. At higher temperatures, the transport is governed by the small-polaron hopping (SPH) mechanism, consistent with thermally activated carrier mobility. These results provide a coherent picture of the conduction behavior across the full investigated temperature range. For all measured temperatures, the conductivity spectra of α-LiFe5O8 are examined via universal power law, revealing a characteristic dispersive behavior. The material exhibits pronounced negative temperature coefficient behavior, characterized by two NTCR values (− 4.31% K−1 at 343 K and − 3.40% K−−1 at 433 K), highlighting the strong potential of α- LiFe5O8 for thermistor and temperature sensing applications.