<p>Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>-Li<sub>2</sub>TiO<sub>3</sub> exhibits distinct phases of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> and Li<sub>2</sub>TiO<sub>3</sub> in its heterostructure. Morphological analysis reveals highly crystalline samples with average particle size of 0.3–0.5&#xa0;µm. A wide bandgap of 3.6&#xa0;eV predicts low electronic conductivity of the composite. Both pure and composite samples exhibit oxidation states of +4 for Ti ions. Room-temperature electronic and ionic conductivity of 3.9 × 10<sup>−8</sup> S cm<sup>−1</sup> and 7 × 10<sup>−8</sup>S cm<sup>−1</sup> for Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub> decrease slightly to 2 × 10<sup>−8</sup>S cm<sup>−1</sup> and 4.5 × 10<sup>−8</sup>S cm<sup>−1</sup> for the composite. In a temperature range of 20–300°C the heterostructure demonstrates increased conductivity from 10<sup>−8</sup>S cm<sup>−1</sup> to 10<sup>−5</sup>S cm<sup>−1</sup> in both grains and grain boundaries, attributed to increased interfaces. Arrhenius plots exhibit low activation energy of 0.32&#xa0;eV for the composite. The structural and electrical properties of Li<sub>4</sub>Ti<sub>5</sub>O<sub>12</sub>-Li<sub>2</sub>TiO<sub>3</sub> strongly influence its electrochemical performance as an anode.</p>

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Structural, Optical, and Temperature-Dependent Electrical Transport Properties of Li4Ti5O12-Li2TiO3 Heterostructured Anode for Energy Storage

  • Humaira Safdar Bhatti,
  • Turabb Ali,
  • Asad Muhammad Iqbal,
  • Saif Ullah Awan,
  • Bilal Ahmad

摘要

Li4Ti5O12-Li2TiO3 exhibits distinct phases of Li4Ti5O12 and Li2TiO3 in its heterostructure. Morphological analysis reveals highly crystalline samples with average particle size of 0.3–0.5 µm. A wide bandgap of 3.6 eV predicts low electronic conductivity of the composite. Both pure and composite samples exhibit oxidation states of +4 for Ti ions. Room-temperature electronic and ionic conductivity of 3.9 × 10−8 S cm−1 and 7 × 10−8S cm−1 for Li4Ti5O12 decrease slightly to 2 × 10−8S cm−1 and 4.5 × 10−8S cm−1 for the composite. In a temperature range of 20–300°C the heterostructure demonstrates increased conductivity from 10−8S cm−1 to 10−5S cm−1 in both grains and grain boundaries, attributed to increased interfaces. Arrhenius plots exhibit low activation energy of 0.32 eV for the composite. The structural and electrical properties of Li4Ti5O12-Li2TiO3 strongly influence its electrochemical performance as an anode.