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of 7
LI ET AL.
citric acid increased, it could be observed that when
the mole ratio of citric acid and Mo reached 1, all of the
peaks were corresponding to MoO . This illustrated that
3
[14]
the formed molybdenum‐citrate complex
did not react
with sulfur ion to generate MoS but decomposed into
2
MoO under this condition. The MoO could not be fully
3
3
sulfurized by H S under 400 °C. Since it is generally
2
accepted that MoS is the active site for sulfur‐resistant
2
CO methanation process, it is easy to understand why CO
methanation activity became worse with the increasement
of citric acid content.
In complementary with XRD, Figure 3 showed the
FTIR spectra of different catalysts. Just as delivered in
‐
1
‐1
Figure 3(a), for Cat‐1, the peaks at 988 cm , 874 cm and
6
‐1
01 cm were assigned to Mo=O stretch vibration mode,
asymmetric Mo‐O bond and Mo‐O‐Mo bonding vibration
[
18]
mode of MoO , respectively.
1
Besides, the absorption at
3
635 cm‐ was attributed to the asymmetric stretching
vibrations of C=O in carboxyl groups (‐COO ). No peak
at 700‐690 cm was detected which was considered as anti-
symmetric vibrations of the non‐linear Mo‐O‐Mo bridge in
1
‐
[19]
‐1
[14]
dimers,
indicating that molybdenum‐citrate complex
had been decomposed under the hydrothermal condition.
The FTIR spectra was in good consistent with the above
XRD analysis results.
We speculated that hydroxylamine hydrochloride
could inhibit molybdenum‐citrate complex from reacting
with sulfur ion to form MoS species. Therefore, verifica-
2
tion experiment without hydroxylamine hydrochloride
added was conducted and the obtained product of Cat‐1‐
N was analyzed by XRD and FTIR spectra. As observed in
Figure 2(d), the main peaks were corresponding to
FIGURE 3 FTIR spectra of as‐prepared products (a: Cat‐1, b: Cat‐
1‐N)
the peaks of 2H‐MoS , which indicated that molybde-
2
num‐citrate complex had reacted with sulfur ion under
this condition. Sulfur ion substituted the oxygen in
Mo=O bond of the molybdenum‐citrate complex and
the newly generated complex was transformed into
[
5,20]
catalyst.
Therefore, the Cat‐1‐N with rich sulfur
vacancy structure displayed a better methanation perfor-
mance. Another proof could be observed in FTIR spectra.
As depicted in Figure 3 for Cat‐1‐N sample, there was no
peak at 700‐690 cm which was assigned to the antisym-
metric vibration of non‐linear Mo‐O‐Mo bridge in dimers,
indicating that the newly generated sulfur complex had
been decomposed to MoS
To further investigate the morphology and particle
size of the obtained MoS catalyst Cat‐1‐N, SEM image
was also carried out. As shown in Figure 4, the obtained
MoS catalyst exhibited uniform MoS cluster structure
MoS under the hydrothermal condition. By comparing
2
‐
1
the XRD patterns of Cat‐0 (Figure 2a) and Cat‐1‐N
(Figure 2d), we found that Cat‐0 was well crystallized,
while the Cat‐1‐N had a poorly crystallized structure
since peaks for Cat‐1‐N were weaker and more broad-
ened. In addition, calculating the crystal particle size of
.
2
MoS (002) plane by XRD spectra, we found that it was
2
2
5
.6 nm and 2.2 nm for Cat‐0 and Cat‐1‐N, respectively.
It was widely recognized that a decrease in crystallite size
2
2
of MoS (002) plane means a deterioration in crystallinity
with the diameter of about 900 nm. The magnified image
revealed that the cluster was consist of several nanosheets
with the thickness around 20‐30 nm.
2
of the catalyst and decreased MoS stacking layers based
2
[5]
on the same lattice spacing. So, it could be concluded
that Cat‐1‐N had a lower crystallinity and fewer MoS2
stacking layers than the Cat‐0. The poorly crystallized
structure would generate more sulfur vacancies, which
were generally considered as the active sites of MoS2
To better understand the MoS microstructure of Cat‐
2
1 and Cat‐1‐N, HRTEM characterization was also carried
out. As shown in Figure 5(a), the as prepared Cat‐1‐N cat-
alyst had typical multi‐layered MoS structure, while in
2