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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Jiang, Yu
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Publications (6/6 displayed)
- 2024Effects of Time-Dependent Rheological Properties of Cementitious Materials on the Print Quality of Extrusion-Based 3D Printing
- 2021Kinetics studies of thin film amorphous titanium niobium oxides for lithium ion battery anodescitations
- 2018Graphene Oxide/Iron Oxide Nanocomposites for Water Remediationcitations
- 2018Graphene oxide-silver nanoparticles in molecularly-imprinted hybrid films enabling SERS selective sensingcitations
- 2016Improving the Selective Efficiency of Graphene-Mediated Enhanced Raman Scattering through Molecular Imprintingcitations
- 2016Effect of blend composition on ternary blend organic solar cells using a low band gap polymercitations
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article
Kinetics studies of thin film amorphous titanium niobium oxides for lithium ion battery anodes
Abstract
<p>Amorphous titanium niobium oxides (TNOs) with varying ratios of Ti and Nb (Ti<sub>4</sub>Nb<sub>2</sub>O<sub>13</sub>, Ti<sub>2</sub>Nb<sub>2</sub>O<sub>9</sub> and TiNb<sub>2</sub>O<sub>7</sub>) are presented as promising anode materials for Li ion batteries. The capacity of the TNO materials is seen to be equivalent to, or larger than, that of the binary oxides, with average volumetric capacities over the first 10 cycles of 717, 1,039 and 925 mAh cm<sup>−3</sup> for amorphous Ti<sub>4</sub>Nb<sub>2</sub>O<sub>13</sub>, Ti<sub>2</sub>Nb<sub>2</sub>O<sub>9</sub> and TiNb<sub>2</sub>O<sub>7</sub><sub>,</sub> respectively at a current density of 0.2 A cm<sup>−3</sup>, compared to 720 mAh cm<sup>−3</sup> and 425 mAh cm<sup>−3</sup> for amorphous TiO<sub>2</sub> and Nb<sub>2</sub>O<sub>5</sub>. Using densities estimated with X-ray reflectometry, these are equivalent to gravimetric capacities of 231, 335, 319 mAh g<sup>−1</sup> for amorphous Ti<sub>4</sub>Nb<sub>2</sub>O<sub>13</sub>, Ti<sub>2</sub>Nb<sub>2</sub>O<sub>9</sub> and TiNb<sub>2</sub>O<sub>7</sub><sub>,</sub> respectively at a current density of ~70 mA g<sup>−1</sup>, compared to 257 mAh g<sup>−1</sup> and 137 mAh g<sup>−1</sup> for amorphous TiO<sub>2</sub> and Nb<sub>2</sub>O<sub>5</sub> at a current density ~80 mA g<sup>−1</sup> and ~50 mA g<sup>−1</sup>, respectively. We discuss how rate capability varies with varying ratios of Ti and Nb and relate this to electrochemical parameters determined by the potentiostatic intermittent titration technique. Our findings reveal that the rate capability of the films is dominated by the diffusion resistance, R<sub>D</sub>, a composite parameter linked to the insertion rate and diffusion coefficient of Li, leading to a conclusion that the rate retention of the thin films is dominated by the density of insertion sites and the insertion reaction more generally.</p>