R. Xi, et al.
CatalysisTodayxxx(xxxx)xxx–xxx
Table 1
Specific surface areas, lattice parameters and Raman quantification results of the fresh and spent catalysts.
Samples
Surface area (m2 g−1
)
A1/A1g
α=β=γ = 90°, a = b≠c (Å)
Fresh
Spent
Fresh
Spent
Fresh
Spent
SnO2
30
9
28
7
a = b = 4.735
a = b = 4.740
a = b = 4.765
a = b = 4.782
c = 3.178
a = b = 4.733
a = b = 4.739
a = b = 4.806
–
c=3.176
c=3.175
c=3.204
–
0
0
BaF2:SnO2 = 1:1
BaCl2:SnO2 = 1:1
BaBr2:SnO2 = 1:1
c = 3.177
c = 3.186
c = 3.193
0.06
0.08
0.17
0.10
0.20
–
7
5
4
3
a
Calculated using the Scherrer equation.
The initial BaBr2 and SnO2 phases can hardly be observed, indicating
that solid phase reaction occurred between SnO2 and BaBr2 during the
high temperature OCM process. To verify the formation of BaSnO3, a
pure BaSnO3 sample was also prepared intentionally by the same
method described in the experimental section, but using Ba(NO3)2 and
SnO2 as the precursors. XRD results in Fig. S1 (c) have proved that
BaSnO3 phase has indeed formed in BaBr2:SnO2 = 1:1 catalysts.
Compared with pure SnO2, the 2θ diffraction peaks of the SnO2
phase in the fresh BaX2/SnO2 catalysts shift more or less to lower an-
gles, which accompany the increase of the side lengths of the unit cell in
the order of BaF2 < BaCl2 < BaBr2, as listed in Table 1. This indicates
that the addition of barium halides has enlarged the unit cell volume of
SnO2 phase in the modified samples, especially for BaCl2 and BaBr2
modified catalysts. This enlargement effect of SnO2 cell may be a result
of anion substitutions. It is known that Sn4+ in SnO2 lattice is 6-fold
coordinated with a radius of 0.69 Å, and the 6-fold coordinated Ba2+
has a radius of 1.35 Å. Therefore, it is impossible for Ba2+ to substitute
Sn4+ in SnO2 lattice to form a solid solution structure [24,25].
Whereas, the radius of O2− in SnO2 lattice is 1.40 Å, and the radius of
F-, Cl- and Br- is 1.33, 1.81 and 1.96 Å, respectively, in the range to be
able to replace partially the lattice O2−. Therefore, It is rational to
propose that during the calcination process, a certain amount of O2−
anions in the SnO2 lattice could be replaced by the X- anions with larger
radii, hence expanding the SnO2 cell volume and side lengths [23]. As a
neutrality, which is beneficial to generate surface mobile oxygen sites.
For BaCl2:SnO2 = 1:1 catalyst, Its side lengths of SnO2 phase become
evidently bigger after OCM reaction, indicating that the anion sub-
stitution continued during the reaction process [23].
BaF2:SnO2 = 1:1 and BaCl2:SnO2 = 1:1 catalysts, no obvious phase
change can be observed after OCM reaction, well consistent with the
XRD results. Nevertheless, it is apparent that significant phase change is
detectable for the spent BaBr2:SnO2 = 1:1 catalyst. To clarify this, the
Raman spectroscopy of the pure BaSnO3 compound was collected and
compared with the spent BaBr2:SnO2 = 1:1 catalyst in Fig. S2(c).
It was previously reported that in a perfect cubic BaSnO3 perovskite
structure with space group of Pm3m, three IR active modes with F1u
symmetry can be detected, but no Raman active modes can be observed
[29,30]. As hown in Fig. S2(c), the Raman bands observed for BaSnO3
and the spent BaBr2:SnO2 = 1:1 catalyst are likely to present defects in
the samples, which may locally lower the internal symmetry of the
perovskite phase, thus leading to unexpected Raman modes. A sharp
peak at 1060 cm−1 is observed, which is ascribed to the BaCO3 phase
[29,30]. Because the defective cubic BaSnO3 perovskite structure is an
A-site Schottky type disorder, which possesses an A-site vacancy cou-
pled with an oxygen vacancy [29]. In this case, the elimination of the
structure Ba cations happens, which would eventually convert into
BaCO3 in contact with the atmosphere CO2 or OCM byproduct CO2.
Except for the Raman peaks of BaSnO3, some Raman peaks belonging to
BaBr2 can be observed for the spent BaBr2:SnO2 = 1:1 catalyst, sug-
gesting that solid phase reaction between SnO2 and BaBr2 is not very
complete during the high temperature OCM process.
Compared to pure SnO2, all the fresh BaX2/SnO2 catalysts exhibit a
new peak at 575 cm−1, which can be attributed to interface or surface
phonon modes corresponding to lattice disorder and oxygen vacancies
[24,25]. We hence quantified the integrated area ratios (A1/A1g) of the
ratios
follows
the
of
BaBr2:SnO2 = 1:1 >
The specific surface areas of the catalysts were analyzed with N2-
BET. As displayed in Table 1, the addition of barium halide has de-
creased the specific surface area of the modified catalysts in comparison
with the individual SnO2. Compared with the fresh catalysts, after OCM
reaction, all the samples have only insignificant surface area decrease,
indicating that these SnO2-based samples are stable during the high
temperature reaction.
BaCl2:SnO2 = 1:1 > BaF2:SnO2 = 1:1 > SnO2, indicating that the addi-
tion of barium halide to SnO2 can improve the vacancy amount on the
catalyst surface. For the spent catalysts, except for BaBr2:SnO2 = 1:1, it is
obvious that the A1/A1g ratios are larger than the corresponding fresh
catalysts
and
follow
the
order
of
BaCl2:SnO2 = 1:1 >
BaF2:SnO2 = 1:1 > SnO2. This supports the XRD results to testify that
anion substitution occurs to the modified catalysts, which also continues
during the OCM process. The presence of surface vacancies/defects are
believed to be favorable for the generation of surface active sites, such as
electrophilic oxygen species [16,17].
3.2. Raman spectra characterization of the catalysts
Raman technique was also used to investigate the compositions and
properties of the catalysts. For comparison, the spectra of individual
barium halides and BaSnO3 were also collected and shown in Fig. S2.
Compared with fresh barium halides, the Raman spectra of the spent
ones have no any change in Raman modes, testifying that they are
chemically stable during OCM process, well consistent with the XRD
results.
3.3. Reaction performance of the catalysts
The reaction performance of the catalysts has been evaluated for
OCM, with the results displayed in Fig. 3 and Table 2. For comparison,
displays that all of them have poor reaction performance.
As formerly reported, SnO2 with a rutile crystalline phase belongs to
As depicted in Fig. 3, pure SnO2 exhibits constant CH4 conversion
around 10 % from 600 to 800 ℃, but has low selectivity to C2 products.
In contrast, all the BaX2/SnO2 catalysts exhibit evidently lower activity
than pure SnO2 below 650 ℃. But starting from 700 ℃, the reaction
performance of these modified catalysts begins to output it. Above this
temperature, the CH4 conversion, C2 product selectivity and yield im-
prove quickly with the increasing of the temperature. Obviously, the
D144h space group, whose active Raman modes can be distributed as B1g
,
Eg, A1g and B2g according to the group theory [24,25]. For the fresh
bration modes at 478 cm−1, 633 cm−1 and 774 cm−1 corresponding to
Eg, A1g and B2g modes can be obviously observed, which indicates that
SnO2 is the major phase in all the catalysts [24,25]. For spent
3