ARTICLE IN PRESS
Y. Ni et al. / Journal of Solid State Chemistry 178 (2005) 908–911
909
2. Experimental procedure
All reagents were commercially available and used
without further purification. In a typical experiment,
metallicMg powder (0.206 g, 99%), AlCl (0.210 g) and
3
C2Cl6 (0.980 g) were added into a vitreous conical flask
[17]; 10 mL C6H6 was filled in and the mixture was
stirred uniformly. Then the flask was put in an autoclave
of about 50 mL capacity. The reactor was sealed and
maintained at 200 1C for 12 h and then allowed to cool
down to room temperature naturally. The dark resultant
was collected, washed with absolute ethanol, HCl
solution (about 2 mol Lꢀ1), and distilled water. Finally,
it was dried in a vacuum at 60 1C for 6 h and about
0.08 g samples were obtained.
10
20
30
40
50
60
70
2θ(degree)
The phase and crystallography of the products were
characterized by X-ray diffraction (XRD) pattern,
which was recorded by using a Shimadzu XRD-6000
X-ray diffractometer equipped with CuKa radiation
(l ¼ 0:15406 nm), and the scanning rate of 0.05 1 sꢀ1 was
applied to record the pattern in the 2y range of 10–701.
The transmission electron microscope (TEM) image
was taken with a Hitachi Model H-800 TEM, using an
accelerating voltage of 200 kV to determine the mor-
phological features. The high-resolution transmission
electron microscope (HRTEM) image was investigated
with a JEOL-2010 TEM, using an accelerating voltage
of 200 kV.
Fig. 1. The XRD pattern of as-prepared products, which indicates a
hexagonal phase of carbon.
about 3.8 nm. The exact graphitic sheet number could
not be counted for most of them were entangled
together.
Further evidence for the purity of products was
obtained through the Raman spectrometer. Fig. 3 shows
that there exist two strong peaks at 1596 and 1360 cmꢀ1
.
The peak at 1596 cmꢀ1 corresponds to an E2g mode of
graphite, related to the vibration of sp2-bonded carbon
atoms in a two-dimensional hexagonal lattice, such as in
a graphite layer. The peak at 1360 cmꢀ1 is associated
with vibrations of carbon atoms with dangling bonds in
plane terminations of disordered graphite [19]. This
peak is quite broadened, which means that in the basal
plane there exists two-dimensional disorder, which is to
be expected, as the reaction temperature is low.
Raman spectrum was measured on a Spex 1403
Raman spectrometer at ambient temperature, employ-
ing an argon ion laser at an excitation wavelength of
514.5 nm.
3. Results and discussion
A possible mechanism of reaction was proposed.
Magnesium, as an active metal, easily forms Grignard
reagent with the organic-chloride as RCl+Mg-
RMgCl. Grignard reagent will react with the chlorides
of all elements below magnesium in the electromotive
series, usually by replacing the chlorine with alkyl
group, similar to the reaction RMgCl+AlCl3-
R3Al+MgCl2. Here, Grignard reagent, functioning as
a strong base, is attracted to electron-deficient centers
AlCl3, and obtains intermediate products R3Al [20].
In this method, AlCl3 also plays another role of
importance. It can polarize the chlorine atom to aid
the attraction on the highly stabilized material
C2Cl6 according to the route RCl+AlCl3-
[AlCl3 Á Clꢀ]+[R+]. Although the intermediated cation
The XRD pattern of the products (Fig. 1) shows the
presence of reflections characteristic of carbon hexago-
nal phase. Reflections in the figure can be indexed to
(002) and (101). The (002) peak is strong while (101) is
weak and wide. Compared with the reported data of
graphite (JCPDS Card Files, No. 41-1487), the position
of the (002) peak shifts a little angle from 2y ¼ 26.41 to
26.21, probably owing to the increase in the spacing
between sp2 carbon layers from 0.337 nm for graphite to
0.341 nm for HCSs [18].
The typical morphology of the samples is presented in
Fig. 2 via TEM observations. From Figs. 2a and b, it
can be seen that most of them are hollow nanospheres
with diameter of 30–60 nm. The strong contrast between
the dark edge and pale center is the evidence of its
hollow nature. The inset in Fig. 2a is the selected area
electron diffraction (SAED) pattern of the HCSs, which
can be indexed as (002) reflection of the graphite.
Fig. 2c shows the wall structure of typical HCSs
observed by HRTRM. The whole sheets thickness is
R
+ is stabilized to a degree, it is a higher-energy species
than the fully conjugated structure of the unsubstitued
chloride carbon. So, the R3Al is easily attacked by an
electrophile R+, to give an intermediate, and obviously,
an electrophile eventually must be released from the
intermediate to produce a neutral molecule R–R as the