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Lithium transport through the Li_(1-δ)CoO_2 film electrode prepared by RF magnetron sputtering

机译:锂通过RF磁控溅射制备的Li_(1-δ)CoO_2薄膜电极的传输

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Lithium transport through the Li_(1-δ)CoO_2 film electrode prepared by RF magnetron sputtering was investigated in a 1 M solution of LiClO_4 in propylene carbonate using the galvanostatic intermittent titration technique (GITT), electrochemical impedance spectroscopy (EIS), and the potentiostatic current transient technique. The experimental cathodic and anodic current transients in the presence of a single phase Li_(1-δ)CoO_2 did not follows Cottrell behaviour, but Ohmic behaviour. This means the relationship between the initial current level and the potential step obeys Ohm's law. In addition, the current transients obtained in the case of coexistence of two phase α and β were characterised by a flatter shape, as compared to those transients in the presence of the respective α and β phases. Also, during phase transformation, the instantaneous current level was proportional to the potential step, in compliance with Ohm's law. From these results, it was suggested that the flux of lithium ion at the electrode | electrolyte interface during lithium transport is limited purely by the 'cell-impedance', not only in the presence of a single phase, but also when the two phases coexist. The value of the 'cell-impedance' calculated from the current transient was almost equal to the values obtained from the impedance spectra and the galvanostatic discharge curve. The current transients were modelled under the assumption of the 'cell-impedance-controlled' lithium intercalation and deintercalation. The current transients calculated theoretically coincided well in value and shape with those measured experimentally.
机译:使用恒电流间歇滴定技术(GITT),电化学阻抗谱(EIS)和恒电位研究了在1M LiClO_4在碳酸亚丙酯中的溶液中研究了通过RF磁控溅射制备的Li_(1-δ)CoO_2薄膜电极中的锂传输情况当前的瞬态技术。在单相Li_(1-δ)CoO_2存在下,实验性阴极和阳极电流瞬变不遵循Cottrell行为,而是遵循欧姆行为。这意味着初始电流水平和电位阶跃之间的关系服从欧姆定律。另外,与存在相应的α相和β相的那些瞬变相比,在两个相α和β共存的情况下获得的电流瞬变的特征在于更平坦的形状。同样,在相变过程中,符合欧姆定律,瞬时电流水平与电位阶跃成正比。根据这些结果,可知电极上的锂离子通量为锂传输过程中的电解质界面不仅受“电池阻抗”的限制,不仅在单相存在时,而且在两相共存时也是如此。从电流瞬态计算出的“电池阻抗”值几乎等于从阻抗谱和恒电流放电曲线获得的值。电流瞬态是在“电池阻抗控制”的锂嵌入和脱嵌的假设下建模的。理论上计算出的电流瞬变在数值和形状上与实验测量的非常吻合。

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