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Fast diffusion mechanism in Li4P2S6 via a concerted process of interstitial Li ions

机译:通过间质锂离子的协调方法在Li4P2S6中快速扩散机制

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The synthesis of Li superionic conductor Li _(7) P _(3) S _(11) may be accompanied by the formation of a detrimental Li _(4) P _(2) S _(6) phase due to a high mixing sensitivity of precursor materials. This phase exhibits a poor ionic conductivity whose origins are not fully understood. Recently Dietrich et al. investigated the energetics of Li ion migration in Li _(4) P _(2) S _(6) with nudged elastic band (NEB) calculations. The observed large migration barrier of 0.51 eV for purely interstitial diffusion leads to an interpretation of the low ionic conductivity by kinetic limitations. Based on ab initio molecular dynamics simulations (AIMD) we propose a new and energetically much more favorable diffusion path available to interstitial Li ion charge carriers that has not been considered so far. It consists of a concerted process in which a second lithium atom is pushed out from its equilibrium lattice position by the diffusing lithium ion. A detailed analysis with NEB calculations shows that the energy barrier for this concerted diffusion is only 0.08 eV, i.e. an order of magnitude lower than the previously reported value for purely interstitial diffusion. Therefore, the observed low ionic conductivity of Li _(4) P _(2) S _(6) is likely not originating from kinetic limitations due to high diffusion barriers but rather from thermodynamic reasons associated with a low concentration of free charge carriers. We therefore expect that increasing the charge carrier concentration by doping is a viable design route to optimize the ionic conductivity of this material.
机译:Li超前导体Li _(7)P _(3)S _(3)的合成可以伴随着由于高位而形成的有害Li _(4)P _(2)S阶段的阶段混合前体材料的敏感性。该阶段表现出较差的离子电导率,其起源不完全理解。最近饮食尤拉德。研究了Li _(4)P _(2)S _(6)中Li离子迁移的能量学,具有闪烁的弹性带(NEB)计算。对于纯粹间隙扩散的观察到的大型迁移屏障为0.51eV,导致动力学限制对低离子电导率的解释。基于AB Initio分子动力学模拟(AIMD),我们向迄今未被视为未被考虑的空间Li离子电荷载体提供了新的和能源勃勃的扩散路径。它包括一个齐心协来的方法,其中通过漫射锂离子从其平衡晶格位置推出第二锂原子。用NEB计算的详细分析表明,该协调扩散的能量屏障仅是0.08eV,即低于先前报告的纯粹间隙扩散的值的数量级。因此,观察到的Li _(4)P _(2)S _(6)的低离子电导率可能由于高扩散屏障而不是引起动力学限制,而是从与低浓度的自由电量载体相关的热力学原因。因此,我们期望通过掺杂增加电荷载流子浓度是优化该材料的离子电导率的可行性设计途径。

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