Chemistry Letters 2001
575
and 4, while the calcination in Ar atmosphere gave us a well-crystal-
lized o-LiMnO , of which the average oxidation state of Mn is nearly
2
3
. Crystallographic parameters of the synthesized powder is in a
5,10,11
good agreement with literatures.
As can be seen in the XRD
pattern at 950 °C of Figure 1, there are two secondary phases,
6
LiMn O and Li MnO . In our previous report, we confirmed that
2
4
2
3
Li could be evaporated as an oxide form of Li O at around 940 °C. At
2
higher temperature about 950 °C in Figure 1, lithium can evaporates
from particles. On that way, the formation of Li MnO and LiMn O
2
3
2 4
12
is due to after lithium evaporation. And, the amount of Li MnO
Mn ) is relatively small, comparing to o-LiMnO .
2
3
4+
(
2
LiMnO structure was gradually changed to cycle-induced spinel
2
like phase during cycling. After activation from about the 40th
cycle, the material begins to show a capacity of more than 160 mAh
–
1
g
reversibly. The higher capacity was maintained upon 300
cycles. The excellent cyclability is due probably to the fine single
crystalline particle oxide.
From these results, it was found that o-LiMnO was easily
2
formed from reduction of Li MnO prepared by the emulsion dry-
2
3
ing method. This method is quite effective to synthesize fine single
crystalline oxide electrode material. The product calcined from
emulsion dried powder precursor would show enhanced battery per-
1,2
formance than other powders prepared by other synthetic routes.
We are going to develop the physical and electrochemical proper-
Figure 2 shows TEM bright-field image and selected-area elec-
ties of the o-LiMnO2, and report elsewhere in near future.
tron diffraction (SAD) pattern obtained from o-LiMnO calcined at
2
925 °C for 12 h in an Ar atmosphere. As can be seen in SAD pat-
The authors would like to thank Ms. Nobuko Kumagai for her
helpful assistance in the experimental work. This study was sup-
ported by Industrial Technology Research Grant Program in ’00
from the New Energy and Industrial Technology Development
Organization (NEDO) of Japan, the Iwatani Naoji Foundation’s
Research Grant, and Yazaki Memorial Foundation for Science and
Technology.
tern of Figure 2, the product consists of single crystalline particle
oxide. Most of particles have smoothly developed edges and cor-
ners. The particle size distribution was 0.5–1.5 µm in diameter
from TEM observation. It is interesting to note that the colors of
calcined powder changed from a tone of brown to olive green with
increasing calcination temperature from 700 to 925 °C. During the
heat-treatment, there must happen changes in band gap between
conduction and valence bands. From XRD and TEM experiments,
the emulsion drying method is how effective to intermix the cations
homogeneously in atomic scale, leading to highly fine single crystal
particle oxide.
References and Notes
1
2
3
4
L. Croguennec, P. Deniard, and R. Brec, J. Electrochem. Soc., 144,
3323 (1997).
G. Pistoia, A. Antonini, and D. Zane, Solid State Ionics, 78, 115
(1995).
J. N. Reimers, E. W. Fuller, E. Rossen, and J. R. Dahn, J.
Electrochem. Soc., 140, 3396 (1993).
Y.-I. Jang, B. Huang, H. Wang, D. R. Sadoway, and Y.-M. Chiang, J.
Electrochem. Soc., 146, 3217 (1999).
Figure 3 shows charge–discharge curves and their correspon-
ding cyclability of the o-LiMnO calcined at 925 °C for 12 h in Ar
2
atmosphere. The cell showed two potential plateaus (3.7 and 4.1 V)
in the initial charge process. It was thought that phase transforma-
tion to spinel might occur during electrochemical lithium deinterca-
lation, leading to much faster phase transformation to reach highest
capacity upon cycling. As cycle goes by, 4-V subplateaus and 3-V
plateau are getting longer, meaning that activation of the oxide
derived from the phase transformation is in progress to show high
5
6
7
S.-T. Myung, S. Komaba, and N. Kumagai, Chem. Lett., 2001, 80.
S.-T. Myung and H.-T. Chung, J. Power Sources, 84, 32 (1999).
S.-T. Myung, H.-T. Chung, N. Kumagai, S. Komaba, and H.-B. Gu,
J. Power Sources, 90, 103 (2000).
8
9
S.-T. Myung, N. Kumagai, S. Komaba, and H.-T. Chung, Solid State
Ionics, 139, 47 (2001).
S.-T. Myung, S. Komaba, and N. Kumagai, J. Electrochem. Soc., 148,
A482 (2001).
4,13
capacity, as reported previously.
During the activation to pro-
10 Joint Committee on Powder Diffraction Standards, File no. 24-0734.
11 V. R. Hoppe, G. Brachtel, and M. Jansen, Z. Anorg. Allg. Chem., 417,
duce high capacity derived from phase transition from orthorhom-
bic to cycled-induced spinel like phase, the charge–discharge curves
confirm that structural reordering from orthorhombic to spinel
LiMn O occurs to result in higher capacity. Indeed, ex-situ XRD
1
(1975).
1
2
M. M. Thackeray, M. F. Mansuetto, and J. G. Bates, J. Power
Sources, 68, 153 (1997).
2
4
13 I. M. Kötschau and J. R. Dahn, J. Electrochem. Soc., 145, 2672
experiment showed close result to refs 4 and 13 that the original o-
(1998).