Computational and Experimental Investigation of the
Electrochemical Stability and Li-Ion Conduction Mechanism of
LiZr
2
(PO
4
)
3
Yusuke Noda,*
,†
Koki Nakano,
‡
Hayami Takeda,
‡,§
Masashi Kotobuki,
∥,⊥
Li Lu,
∥,⊥
and Masanobu Nakayama
†,‡,§,#
†
Center for Materials Research by Information Integration (CMI
2
), Research and Services Division of Materials Data and Integrated
System (MaDIS), National Institute for Materials Science (NIMS), 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan
‡
Frontier Research Institute for Materials Science (FRIMS), Nagoya Institute of Technology, Gokiso, Showa, Nagoya, Aichi
466-8555, Japan
§
Elements Strategy Initiative for Catalysts and Batteries (ESICB), Kyoto University, 1-30 Goryo-Ohara, Nishikyo, Kyoto 615-8245,
Japan
∥
Department of Mechanical Engineering, National University of Singapore, 9 Engineering Drive 1, Singapore 117575, Singapore
⊥
National University of Singapore Suzhou Research Institute, Dushu Lake Science and Education Innovation District, Suzhou
215123, P. R. China
#
Global Research Center for Environment and Energy Based on Nanomaterials Science (GREEN), National Institute for Materials
Science (NIMS), 1-1 Namiki, Tsukuba, Ibaraki 305-0047, Japan
* S Supporting Information
ABSTRACT: Solid electrolytes possessing sufficient ionic
conductivity and electrochemical stability are urgently needed
for the fabrication of all-solid-state Li-ion batteries (LIBs). In
this study, we focus on a solid-state oxide electrolyte
LiZr
2
(PO
4
)
3
(LZP), which has NASICON structure and
electrochemically stable Zr
4+
ions. Using density functional
theory (DFT) to calculate the electrochemical window of LZP,
we find that it is unstable against Li metal, in accordance with
our experimental results. The Li-ion transport is investigated
using first-principles molecular dynamics (FPMD) simulations.
The calculated Li-ion conductivity at room temperature (5.0 ×
10
−6
S/cm) and the activation energy for Li-ion diffusion (0.43
eV) are in fair agreement with experimental results. The
mechanism of Li-ion conduction in LZP is revealed by analyzing the Li-ion trajectories in the FPMD simulations. It is found that
each Li ion migrates between 6b sites as it is pushed out or repelled by other Li ions around these 6b sites. Hence, the high Li-ion
conductivity is attributed to a migration mechanism driven by Frenkel-like defect.
1. INTRODUCTION
The Li-ion battery (LIB) is one of the most popular types of
rechargeable batteries with high energy density, long cycle life,
and good safety. LIBs have been widely used for electric
vehicles, smartphones, laptops, and so on.
1
At present, the
prevailing electrolytes for LIBs are organic liquid solvents, such
as dimethyl carbonate and ethylene carbonate. However, these
electrolytes are at risk of liquid leakage, inflammation, and/or
explosion caused by short circuit.
2
One attractive and important solution to this problem is
replacing the organic liquid electrolytes with inorganic solid
electrolytes. Such solid electrolytes are indispensable for all-
solid-state batteries. Sulfide-based solid electrolytes such as
Li
10
GeP
2
S
12
(LGPS) are well-known as good ionic conductors
with high Li-ion conductivity (10
−2
S/cm) because of their
three-dimensional diffusion channels.
3−5
However, sulfides
present difficulties in the fabrication of all-solid-state batteries,
as they tend to react with water and generate hydrogen sulfide
gas. From this point of view, it is advisable to use oxide-based
solid electrolytes instead. Unfortunately, compared with sulfide-
based solid electrolytes, the oxide-based ones exhibit lower Li-
ion conductivity at room temperature (in the order of 10
−3
S/
cm at the highest). Therefore, it is essential to improve their
ionic conductivity.
Na super ionic conductor (NASICON)-type oxide-based
solid electrolytes, as well as perovskite-type and garnet-type
Received: April 26, 2017
Revised: October 18, 2017
Published: October 18, 2017
Article
pubs.acs.org/cm
© 2017 American Chemical Society 8983 DOI: 10.1021/acs.chemmater.7b01703
Chem. Mater. 2017, 29, 8983−8991
Cite This: Chem. Mater. 2017, 29, 8983-8991
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