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Stabilizing the surface of lithium metal

Published online by Cambridge University Press:  09 May 2014

J.T. Vaughey
Affiliation:
Argonne National Laboratory, IL, USA; vaughey@anl.gov
Gao Liu
Affiliation:
Lawrence Berkeley National Laboratory, CA, USA; gliu@lbl.gov
Ji-Guang Zhang
Affiliation:
Pacific Northwest National Laboratory, WA, USA; jiguang.zhang@pnnl.gov

Abstract

The success of high capacity energy storage systems based on lithium (Li) batteries relies on the realization of the promise of Li-metal anodes. Li metal has many advantageous properties, including an extremely high theoretical specific capacity (3860 mAh g–1), the lowest electrochemical potential (–3.040 V versus standard hydrogen electrode), and low density (0.59 g cm–3), which, all together, make it a very desirable electrode for energy storage devices. However, while primary Li batteries are used for numerous commercial applications, rechargeable Li-metal batteries that utilize Li-metal anodes have not been as successful. This article discusses the properties of Li metal in the absence of surface stabilization, as well as three different approaches currently under investigation for stabilizing the surface of Li metal to control its reactivity within the electrochemical environment of a Li-based battery.

Information

Type
Research Article
Copyright
Copyright © Materials Research Society 2014 
Figure 0

Figure 1. Schematic diagram of a (a) Li-ion battery (blue spheres are lithium cations; red layers represent layers of intercalation host lattice); (b) Li-metal battery and typical morphology of a Li dendrite; and (c) main problems related with dendrite and low Coulombic efficiency (CE). Morphology picture in (c) is reproduced with permission from Reference 11. © 1976 Elsevier.

Figure 1

Figure 2. Scanning electron microscope micrographs showing the time-dependent evolution of morphology of the solid electrolyte interphase layer on metallic lithium electrodes upon contact with the 1.2 M LiPF6/50 wt% ethylene carbonate: 50 wt% ethyl methyl carbonate (EC:EMC) electrolyte solution. (a) Bare lithium, (b) after 20 seconds of contact, (c) after 5 minutes, and (d) after 1 hour.17 The scale bar represents 50 microns.

Figure 2

Figure 3. Scanning electron microscope images of the morphologies of Li films deposited in an electrolyte of 1 M LiPF6/propylene carbonate with CsPF6 concentrations of: (a) 0 M, (b) 0.005 M, and (c) 0.05 M at a current density of 0.1 mA cm–2. Note the surface morphology becomes smoother with increasing Cs+ content. The effect is only seen at these low concentration levels where the effective reduction potential is below the standard lithium cation reduction potential.57

Figure 3

Figure 4. (a) Low magnification scanning electron microscopy (SEM) image of stabilized lithium-metal powder (SLMP) particles.60 (b) Optical microscopic image of SLMP particles. Image courtesy of FMC Lithium Corporation. (c) High magnification SEM image of the SLMP.60 (d) High magnification SEM image of the lithium carbonate coating layer.61

Figure 4

Figure 5. Nanomechanical and electrical measurement of stabilized Li-metal powder (SLMP) under in situ transmission electron microscope observation. (a) Schematic diagram of an in situ compression and electrical test of a single SLMP particle. (b) Displacement-controlled compression of a single particle. (c) Under displacement-controlled compression, the load initially increases versus displacement, then plateaus, but the measured current versus displacement curve remains low throughout the compression. The displacement and current curves are plotted in black and red, respectively. The point of compression where the protective carbonate shell starts to fail is given by the peak load at approximately 1000 μN, just below a displacement of 2000 nm. (d) The schematic diagram of an in situ mechanical and electrical test of a single SLMP using a sharp conductive indenter tip. (e) Displacement-controlled indentation of a single particle. (f) Under displacement-controlled indentation, the load increases versus displacement. The measured current increases when the indentation tip pokes through the LiCO3 layer at ∼200 μN and a displacement of ∼1500 nm, where the metallic lithium has been accessed. The displacement and current curves are plotted in green and red, respectively.60

Figure 5

Figure 6. (a) Cycle performance for graphite/NMC (lithium nickel manganese cobalt oxide Li(Ni1/3Mn1/3Co1/3)O2) full cells with (red symbols) and without stabilized lithium-metal powder (SLMP) (green symbols) at a C/3 rate. The amount of current needed to charge a cell in one hour is referred to as the C-rate. A C/3 rate means 1/3 of that current was used, and the full charge took three hours. (b) The cell with SLMP was rested at open circuit for four days before cycling to allow it to reach equilibrium with the electrolyte. The cell without SLMP was put through a series of low rate formation cycles to allow it to build up a more stable solid electrolyte interphase layer (green symbols) and was cycled at C/25 for five cycles, followed by C/10 for 10 cycles, then cycled at a C/3 rate. The cell without SLMP and not put through formation cycling (blue symbols) was cycled at C/3 directly after assembling.63