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在 Pmmn-Li(1-x)FeO2 电极材料中锂的扩散途径和空位的形成。

Lithium diffusion pathways and vacancy formation in the Pmmn-Li(1-x)FeO2 electrode material.

机构信息

Dipartimento di Scienza dei Materiali, Università di Milano Bicocca, Milano, Italy.

出版信息

Phys Chem Chem Phys. 2011 Jun 21;13(23):11156-64. doi: 10.1039/c1cp20551j. Epub 2011 May 13.

DOI:10.1039/c1cp20551j
PMID:21573290
Abstract

Models for Li(+) ion mobility were developed and investigated in the 'corrugated layer' orthorhombic phase of Li(1-x)FeO(2), an attractive possible electrode material for reversible lithium ion batteries. The ground-state crystal energy was computed by first-principles DFT (Density-Functional-Theory) methods, based on the use of the hybrid B3LYP functional with localized Gaussian-type basis sets. Appropriate supercells were devised as needed, with full least-energy structure optimization. In the defect-free case (x = 0), ion diffusion was found to take place cooperatively inside a fraction of active lithium layers separated by inert ones, so as to reduce lattice strain; intermediate bottleneck states of Li are either in tetrahedral (energy barrier ΔE(a) = 0.410 eV) or linear (ΔE(a) = 0.468 eV) coordination. For the Li(0.75)FeO(2) deintercalated material a number of low energy vacancy configurations were considered, investigating also the vacancy influence on electron density of states and atomic charge distribution. The most favourable ion transport mechanisms (ΔE(a) = 0.292 and 0.304 eV) imply a linear Li bottleneck state, with all lithium layers active and a quite small lattice strain. Accordingly, in the defective material the predicted ionic conductivity at room temperature rises from 10(-5)-10(-6) (LiFeO(2)) to 4 × 10(-4) ohm(-1) cm(-1) (Li(0.75)FeO(2)).

摘要

开发并研究了 Li(+)离子在 Li(1-x)FeO(2)“波纹层”正交相中的迁移模型,Li(1-x)FeO(2)是一种有吸引力的可逆锂离子电池的可能电极材料。通过使用基于局域高斯型基组的杂化 B3LYP 函数的第一性原理 DFT(密度泛函理论)方法,计算了基态晶体能量。根据需要设计了适当的超晶胞,并进行了全最小能量结构优化。在无缺陷的情况下(x=0),发现离子扩散是在由惰性层隔开的一部分活性锂层内部协同进行的,以减少晶格应变;Li 的中间瓶颈状态要么处于四面体形(能量势垒ΔE(a)=0.410 eV),要么处于线性(ΔE(a)=0.468 eV)配位。对于脱插 Li(0.75)FeO(2)材料,考虑了许多低能量空位构型,还研究了空位对电子态密度和原子电荷分布的影响。最有利的离子输运机制(ΔE(a)=0.292 和 0.304 eV)意味着线性 Li 瓶颈状态,所有锂层都活跃,晶格应变很小。因此,在有缺陷的材料中,预测的室温离子电导率从 10(-5)-10(-6)(LiFeO(2))增加到 4×10(-4)ohm(-1)cm(-1)(Li(0.75)FeO(2))。

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