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通过在石榴石结构的固态电解质和锂金属阳极之间形成一层锗,来降低界面电阻。

Reducing Interfacial Resistance between Garnet-Structured Solid-State Electrolyte and Li-Metal Anode by a Germanium Layer.

机构信息

Department of Materials Science and Engineering, University of Maryland, College Park, MD, 20742, USA.

Department of Mechanical Engineering, University of Maryland, College Park, MD, 20742, USA.

出版信息

Adv Mater. 2017 Jun;29(22). doi: 10.1002/adma.201606042. Epub 2017 Apr 18.

Abstract

Substantial efforts are underway to develop all-solid-state Li batteries (SSLiBs) toward high safety, high power density, and high energy density. Garnet-structured solid-state electrolyte exhibits great promise for SSLiBs owing to its high Li-ion conductivity, wide potential window, and sufficient thermal/chemical stability. A major challenge of garnet is that the contact between the garnet and the Li-metal anodes is poor due to the rigidity of the garnet, which leads to limited active sites and large interfacial resistance. This study proposes a new methodology for reducing the garnet/Li-metal interfacial resistance by depositing a thin germanium (Ge) (20 nm) layer on garnet. By applying this approach, the garnet/Li-metal interfacial resistance decreases from ≈900 to ≈115 Ω cm due to an alloying reaction between the Li metal and the Ge. In agreement with experiments, first-principles calculation confirms the good stability and improved wetting at the interface between the lithiated Ge layer and garnet. In this way, this unique Ge modification technique enables a stable cycling performance of a full cell of lithium metal, garnet electrolyte, and LiFePO cathode at room temperature.

摘要

目前正在进行大量努力来开发全固态锂电池 (SSLiBs),以实现高安全性、高功率密度和高能量密度。石榴石结构的固态电解质由于其高锂离子电导率、宽电位窗口和足够的热/化学稳定性,在 SSLiBs 中具有很大的应用前景。石榴石的一个主要挑战是由于石榴石的刚性,石榴石与锂金属阳极之间的接触不良,这导致有限的活性位点和大的界面电阻。本研究提出了一种通过在石榴石上沉积一层薄薄的锗 (Ge) (20nm) 层来降低石榴石/锂金属界面电阻的新方法。通过采用这种方法,由于锂金属和 Ge 之间的合金反应,石榴石/锂金属界面电阻从约 900Ωcm 降低到约 115Ωcm。与实验一致,第一性原理计算证实了在富锂 Ge 层和石榴石之间的界面上良好的稳定性和改善的润湿性。通过这种方式,这种独特的 Ge 改性技术使全电池在室温下具有稳定的循环性能,包括锂金属、石榴石电解质和 LiFePO4 阴极。

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