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缺陷型Ti2Nb10O27.1:一种用于锂离子电池的先进负极材料。

Defective Ti2Nb10O27.1: an advanced anode material for lithium-ion batteries.

作者信息

Lin Chunfu, Yu Shu, Zhao Hua, Wu Shunqing, Wang Guizhen, Yu Lei, Li Yanfang, Zhu Zi-Zhong, Li Jianbao, Lin Shiwei

机构信息

Key Laboratory of Ministry of Education for Advanced Materials in Tropical Island Resources, College of Materials and Chemical Engineering, Hainan University, Haikou 570228, PR China.

Department of Physics and Institute of Theoretical Physics and Astrophysics, Xiamen University, Xiamen 361005, PR China.

出版信息

Sci Rep. 2015 Dec 3;5:17836. doi: 10.1038/srep17836.

Abstract

To explore anode materials with large capacities and high rate performances for the lithium-ion batteries of electric vehicles, defective Ti2Nb10O27.1 has been prepared through a facile solid-state reaction in argon. X-ray diffractions combined with Rietveld refinements indicate that Ti2Nb10O27.1 has the same crystal structure with stoichiometric Ti2Nb10O29 (Wadsley-Roth shear structure with A2/m space group) but larger lattice parameters and 6.6% O(2-) vacancies (vs. all O(2-) ions). The electronic conductivity and Li(+)ion diffusion coefficient of Ti2Nb10O27.1 are at least six orders of magnitude and ~2.5 times larger than those of Ti2Nb10O29, respectively. First-principles calculations reveal that the significantly enhanced electronic conductivity is attributed to the formation of impurity bands in Ti2Nb10O29-x and its conductor characteristic. As a result of the improvements in the electronic and ionic conductivities, Ti2Nb10O27.1 exhibits not only a large initial discharge capacity of 329 mAh g(-1) and charge capacity of 286 mAh g(-1) at 0.1 C but also an outstanding rate performance and cyclability. At 5 C, its charge capacity remains 180 mAh g(-1) with large capacity retention of 91.0% after 100 cycles, whereas those of Ti2Nb10O29 are only 90 mAh g(-1) and 74.7%.

摘要

为了探索用于电动汽车锂离子电池的具有高容量和高倍率性能的负极材料,通过在氩气中进行简便的固态反应制备了缺陷型Ti2Nb10O27.1。X射线衍射结合Rietveld精修表明,Ti2Nb10O27.1与化学计量比的Ti2Nb10O29具有相同的晶体结构(具有A2/m空间群的Wadsley-Roth剪切结构),但晶格参数更大且存在6.6%的O(2-)空位(相对于所有O(2-)离子)。Ti2Nb10O27.1的电子电导率和Li(+)离子扩散系数分别比Ti2Nb10O29至少大六个数量级和约2.5倍。第一性原理计算表明,电子电导率的显著提高归因于Ti2Nb10O29-x中杂质带的形成及其导体特性。由于电子和离子电导率的提高,Ti2Nb10O27.1不仅在0.1 C时表现出329 mAh g(-1)的大初始放电容量和286 mAh g(-1)的充电容量,而且具有出色的倍率性能和循环稳定性。在5 C时,其充电容量在100次循环后保持180 mAh g(-1),容量保持率高达91.0%,而Ti2Nb10O29的充电容量仅为90 mAh g(-1),容量保持率为74.7%。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/d9e6/4668578/a3cfb24da48f/srep17836-f1.jpg

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