G.X. Wang et al. / Journal of Alloys and Compounds 299 (2000) L12–L15
L13
ders were characterized by X-ray diffraction on a Philips
PW 1730 diffractometer with a Cu-Ka radiation.
5–10 nm, using the Scherrer formula: d 5 Kl
Y
b Cos u
The Cu6Sn5 electrodes were prepared by dispersing 97
wt% Cu6Sn5 powders and 3 wt% polyvinylidene fluoride
(PVDF) binder in dimethyl phthalate to form a slurry,
which was spread on to the copper foil. No carbon
additives were added because Cu6Sn5 alloy has good
electrical conductivity and also in order to eliminate the
ambiguity caused by the insertion of lithium into carbon.
The typical Cu6Sn5 electrode contains about 1 mg active
materials and 80 mm in thickness. Li/Cu6Sn5 coin cells
(CR2032) were assembled. The electrolyte was 1 M LiPF6
in EC (ethylene carbonate) and DMC (dimethyl carbonate)
(Battery grade, MERCK KGaA, Germany). The cells were
charged and discharged at a constant current density of
0.20 mAh/cm2.
[11]. However, a small amount of tin or copper oxides
were formed during the long term ball-milling, probably
due to the very active nature of the nanosize Cu6Sn5 alloy
and traces of oxygen present in the ball-milling vial.
The Li/Cu6Sn5 cells were cycled between 0 and 1.5 V
at a constant current density of 0.20 mA/cm2. The lithium
insertion into and extraction from Cu6Sn5 alloy are defined
as discharge and charge respectively. The first discharge
and charge profiles of Cu6Sn5 alloy electrodes are shown
in Fig. 2. The ball-milled nanosize Cu6Sn5 electrode
demonstrated markedly different behaviour for lithium
insertion compared to that of the sintered crystalline
Cu6Sn5 alloy. In the first discharge, nanosize Cu6Sn5 alloy
electrode delivered a capacity of 688 mAh/g, corre-
sponding to approximately 25 moles of lithium insertion
per mole of Cu6Sn5 alloy. Provided lithium alloys with Sn,
the maximum lithium insertion achievable theoretically is
that each mole of Cu6Sn5 alloy can combine with 22
moles of Li to form Li4.4Sn alloy, with a capacity of 608
mAh/g. As shown in Fig. 1, a small amount of Sn and Cu
oxides are generated during the long term ball-milling. The
extra lithium insertion capacity of 80 mAh/g observed
might be caused by lithium reacting with Sn or Cu oxides
to form Li2O. And this part of lithium cannot be extracted
again, which is similar to the behaviour of tin based glass.
A reversible capacity of 412 mAh/g was achieved in the
first charging which is 60% of the initial discharge
capacity. However, the first discharge capacity for sintered
Cu6Sn5 alloy was only 284 mAh/g. The theoretical
capacity for lithium insertion into Cu6Sn5 to form
Li13Cu6Sn5 (isostructural with Li2CuSn) is 358 mAh/g.
Here, we did not achieve the theoretical capacity, possibly
due to the relatively large particle size. With the scrutiny of
the differential capacity vs. voltage profiles (the insets in
Fig. 2), it might be seen that the ball-milled nanosize
Cu6Sn5 electrode shows several reduction peaks, corre-
sponding to the formation of Li2O and various LixSn
alloys, which is similar to the behaviours of Sn, SnO, SnO2
and SiSnO3 electrodes [12]. By contrast, the crystalline
Cu6Sn5 alloy electrode only shows one sharp reduction
peak, which corresponds to the topotactic insertion of
lithium into Cu6Sn5 alloy structure to form LixCu6Sn5.
This is in agreement with the report from K.D. Kepler et
al. [10]. Consequently, the two different mechanisms for
lithium reaction with ball-milled nanosize and sintered
crystalline Cu6Sn5 alloys are proposed, as follows:
After cycling, the cells were dismantled in an argon
filled glove-box (Unilab, Mbraun, USA) and the Cu6Sn5
electrodes were taken out. The Cu6Sn5 electrodes were
covered by a plastic film for ex-situ X-ray diffraction.
3. Results and discussion
The eta-Cu6Sn5 alloy has a hexagonal structure with a
space group of P63 /mmc. It can be synthesized by either
sintering the mixture of Cu and Sn powders or ball milling
Cu and Sn powders. Fig. 1 shows X-ray diffraction
patterns of Cu6Sn5 alloys. The sintering process produced
a typical crystal Cu6Sn5 alloy with a small amount of
impurity phase of the unreacted Sn, while the ball-milling
generated fine Cu6Sn5 alloy powders. As the ball-milling
time was increased, the diffraction peaks became
broadened, indicating a decrease of the particle size. When
ball-milled for 110 h, very broad diffraction peaks were
observed, from which the grain size was calculated to be
→
22Li 1 Cu Sn (nanosize) 5Li4.4Sn 1
←
6
5
6Cu (Alloying process)
(1)
13Li 1
Fig. 1. X-ray diffraction patterns of eta-Cu6Sn5 alloys. (a) Cu6Sn5 alloy
prepared by sintered process. (b) Cu6Sn5 alloy prepared by ball-milling
for 18 h. (c) Cu6Sn5 alloy prepared by ball-milling for 46 h. (d) Cu6Sn5
alloy prepared by ball-milling for 110 h. * a-Sn, . Cu2O or SnO2.
→
Cu Sn (crystalline) Li Cu Sn (Topotactic insertion p-
←
6
5
13
6
5
rocess)
(2)