Six representative isotope-labeled samples of titanium dioxide were synthesized: Ti¹⁶O₂, Ti¹⁷O₂ and Ti¹⁸O₂, each in anatase and rutile forms. Their Raman scattering was analyzed at temperatures down to 5 K. Spectral assignment was supported by numerical simulation using DFT calculations. The combination of experimental and theoretical Raman frequencies with the corresponding isotopic shifts allowed us to address various still-open questions about the second-order Raman scattering in rutile, and the analysis of overlapping features in the anatase spectrum.

<mml:math display="inline"><mml:msub><mml:mi mathvariant="normal">Li</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Ti</mml:mi><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mo>O</mml:mo><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub></mml:math>Li4Ti5O12 (spinel) materials were prepared with Brunauer-Emmett-Teller surface areas ranging from 1.3 to 196 m²/g. The corresponding average particle sizes varied from ca. 1 μm to ca. 9 nm. Twenty-five different materials were tested as Li insertion hosts in thin-film electrodes (2-4 μm) made from a pure spinel. Trace amounts of anatase in <mml:math display="inline"><mml:msub><mml:mi mathvariant="normal">Li</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Ti</mml:mi><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mo>O</mml:mo><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub></mml:math>Li4Ti5O12 were conveniently determined by cyclic voltammetry of Li insertion. Electrodes from nanocrystalline <mml:math display="inline"><mml:msub><mml:mi mathvariant="normal">Li</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Ti</mml:mi><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mo>O</mml:mo><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub></mml:math>Li4Ti5O12 exhibited excellent activity towards Li insertion, even at charging rates as high as 250C. The charge capability at 50-250C was proportional to the logarithm of surface area for coarse particles (surface areas smaller than ca. 20 m²/g). With increasing charge/discharge rates, a narrowing plateau in performance was observed for materials with surface areas between ca. 20 to 100 m²/g. These materials can be charged/discharged nearly to the nominal capacity of <mml:math display="inline"><mml:msub><mml:mi mathvariant="normal">Li</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Ti</mml:mi><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mo>O</mml:mo><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub></mml:math>Li4Ti5O12 (175 mAh/g) within a wide range of the rates. Very small particles <mml:math display="inline"><mml:mo stretchy="false">(</mml:mo><mml:mi mathvariant="normal">surface areas</mml:mi><mml:mo>></mml:mo><mml:mn>100</mml:mn><mml:mo> </mml:mo><mml:msup><mml:mi mathvariant="normal">m</mml:mi><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>/</mml:mo><mml:mi mathvariant="normal">g</mml:mi><mml:mo stretchy="false">)</mml:mo></mml:math>(surface areas>100 m2/g) exhibit a growing decrease of charge capability at 50-250C. The Li-diffusion coefficients, calculated from chronoamperometry, decrease by orders of magnitude if the average particle size drops from ca. 1 μm to ca. 9 nm. However, the sluggish <mml:math display="inline"><mml:msup><mml:mi mathvariant="normal">Li</mml:mi><mml:mrow><mml:mo>+</mml:mo></mml:mrow></mml:msup></mml:math>Li+ transport in small particles is compensated by the increase in active electrode area. Materials having surface areas larger than ca. 100 m²/g also tend to show increased charge irreversibility. This could be caused by parasitic cathodic reactions, due to enhanced adsorption of reducible impurities (humidity) or the quality of the spinel crystalline lattice itself. The optimum performance of thin-film <mml:math display="inline"><mml:msub><mml:mi mathvariant="normal">Li</mml:mi><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Ti</mml:mi><mml:mrow><mml:mn>5</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mo>O</mml:mo><mml:mrow><mml:mn>12</mml:mn></mml:mrow></mml:msub></mml:math>Li4Ti5O12 electrodes is achieved, if the parent materials have surface areas between ca. 20 to 110 m²/g, with the maximum peak at 100 m²/g. © 2003 The Electrochemical Society. All rights reserved.