X. Zhang, et al.
Applied Catalysis A, General 590 (2020) 117313
Table 1
Textural chemical and basic properties of various CaO-ZrO
2
catalysts.
Pore volume
Sample
Ca2+:Zr4+ atomic ratio
d
XRD (Å)c
S
BET (m2 g−1
)
Average pore diameter
(nm)
Number of basic sites (μmol g−1) and contributiond
3
−1
(
cm
g
)
Initiala
In solidb
Total
W.
M.
S.
ZrO
2
–
–
2.9453
2.9511
2.9513
2.9587
2.9607
252
243
212
167
87
0.28
0.33
0.37
0.32
0.49
4.6
5.4
8.3
9.2
10.1
43
88
113
138
104
18.3 (42.6)
37.4 (42.5)
35.8 (31.7)
36.1 (26.1)
34.3 (33.0)
21.7 (50.4)
40.6 (46.1)
51.5 (45.6)
63.6 (46.1)
34.1 (32.8)
3.0 (7.0)
0.2CaO-ZrO
0.4CaO-ZrO
0.6CaO-ZrO
0.8CaO-ZrO
2
2
2
2
0.2: 1
0.4: 1
0.6: 1
0.8: 1
0.08:1
0.36:1
0.55:1
0.73:1
10.0 (11.4)
25.7 (22.7)
38.3 (27.8)
35.6 (34.2)
a
b
c
The nominal atomic ratio in the mother solution.
Measured by ICP for the final solid catalysts.
Based on the XRD peak at 30.2°.
d
The value in parentheses is the contribution of single basic sites to the total number of total basic sites. W.: Weak sites; M.: Medium basic sites; S.: strong basic
sites.
from 0.2 to 0.6. In light of the fact that the divalent alkali-earth metal
2
minor carbonate species [45]. As illustrated by the following CO -TPD
4
+
ions could substitute Zr
solution, the absence of separated CaO peak could be explained by the
formation of CaO-ZrO solid solution when n was varied from 0.2 to 0.6
37–39]. Nevertheless, due to the limited capacity of ZrO for in-
in the host lattice to generate a stable solid
characterization, their basic strength was determined by the amount of
Ca content. Considering that a stronger basic strength would result in
the formation of carbonate species with a higher stability, and thus, the
2
[
2
2
catalyst 0.8CaO-ZrO showed the most intense peak at 289.5 eV, owing
corporating CaO dissolution into its lattice, two featured diffraction
to its superior basic strength than other samples. Apart from this, the
peaks assigned to CaO were observed (JCPDS No. 48-1467) at 37.3° and
gradual rise of binding energy from 289.1 to 289.5 eV with a rise of n
5
3.8° as n was further increased to 0.8. Noting that the width of peaks
also pointed the incorporation of Ca2+ into ZrO
2
lattice. The typical Zr
3d spectra are presented in Fig. 3 (b). For pristine ZrO , there appeared
2
+
became smaller after insertion of Ca , the average crystallite sizes
2
were thus calculated based on 2θ of 30.2° by the Scherrer formula. The
two peaks at 184.2 and 181.8 eV with a high intensity, which were
associated with Zr 3d5/2 and Zr 3d3/2 energy states of Zr(IV) oxide
species, respectively [46]. The intensity of these two reflections gra-
dually decreased with an increase of Ca content. Meanwhile, it is worth
crystallite sizes of ZrO
2 2 2 2
, 0.2CaO-ZrO , 0.5CaO-ZrO , 0.6CaO-ZrO , and
0
.8CaO-ZrO were 12.8, 16.9, 15.5, 14.8 and 11.5 nm, respectively. At
2
the same time, the following TEM measurement further affirmed that
these samples consisted mainly of crystals with a size of 5–20 nm,
suggesting that they were a class of nano-catalysts. Fig. 1(b) gives the
noting that adding Ca into ZrO
2
support could give rise to a continue
increase of Zr 3d binding energy. These observations also support that
2+
low-angle XRD patterns of nCaO-ZrO
2
catalysts. It could be seen that all
Ca
2
had entered into the t-ZrO lattice, creating a solid solution.
the catalysts show a sharp and symmetric peak at about 2θ = 1°, which
Fig. 3(c) displays the Ca 2p spectra of these catalysts, and the XPS
spectrum of single CaO is also presented for a comparison. When
n < 0.8, all the catalysts exhibited a broad and intense band centered at
346.1 eV related to the emission from Ca 2p3/2 of Ca2 in oxide state
was corresponding to their mesoporous structure [39]. As discussed
2
+
above, the addition of excessive Ca
pearance of free CaO phase, which was adverse to the generation of a
uniformly mesoporous framework. As a result, ZrO exhibited the
highest intensity of diffraction, whereas Ca-rich sample (0.8CaO-ZrO
into the system induced the ap-
+
2
2
[46,47]. In the case of sample 0.8CaO-ZrO , its spectral profile was
2
)
similar to that of CaO, in which an additional peak was observed at
about 350.5 eV. According to the previous work, this satellite peak can
be assigned to Ca 2p1/2 state of Ca2+ [46,47]. More importantly, the
binding energies of Ca 2p2/3 in all the mixed oxides were lower than
presented the lowest one. This is consistent with the results of these
kinds of Zr-based solid bases in previous literature [37,39].
It was accepted that Raman analysis was an effective technique to
study the microstructure of Zr-containing materials. Raman spectra of
that of pure CaO, because the nCaO-ZrO
sessed a solid solution structure. Fig. 3(d) depicts the O1 spectra of
these materials. For samples ZrO , 0.2CaO-ZrO , 0.4CaO-ZrO and
0.6CaO-ZrO , the Ca content did not influence the shape of the O1s
2
-containing materials pos-
nCaO-ZrO
2
, pure ZrO
2
and CaO are shown in Fig. 2. Apparently, bare
at
69, 314, 460 and 645 cm , but also the typical reflections to
ZrO support presented not only the characteristic peaks of t-ZrO
2
2
2
2
2
−1
2
2
−1
monoclinic ZrO
2
phase at 331, 380, 536 and 559 cm
[40,42]. This
cures largely. Precisely, only a sharp peak appeared at about 529.7 eV.
According to Pradhan et al., this peak was ascribed to the lattice oxygen
fact is in line with its XRD result in Fig. 1(a). In contrast, samples of
.2CaO-ZrO , 0.4CaO-ZrO and 0.6CaO-ZrO demonstrated the peaks
attributed to t-ZrO only. No Raman lines due to m-ZrO or CaO were
detected. These also suggested that doping a foreign Ca atom could
covert ZrO from a monoclinic to a tetragonal phase. In addition, it
0
2
2
2
of the CaO-ZrO
O1s peak also implied that strong Lewis basic sites were present at their
surfaces [6], being in line with the following CO -TPD characterization
results. As to the Ca-rich sample (0.8CaO-ZrO ), beside this peak, a new
2
solid solution [42]. Moreover, the appearance of this
2
2
2
2
2
should be noted that the peaks of these Ca-modified samples widened
one with a mild intensity emerged at 531.2 eV, which was consistent
obviously, due to the existence of oxygen vacancy which was resulted
with the O1 s spectrum of pure CaO [48]. This result can be explained
as follows: all the Ca ions were introduced into t-ZrO lattice without
2
2
+
2+
from the incorporation of Ca
more, the peaks at 269 and 645 cm
venumbers for mixed oxide catalysts with a rise of Ca content, further
affirming that they possessed a stable structure of CaO-ZrO solid so-
lution. Nevertheless, a new reflection corresponding to CaO emerged at
into the ZrO
2
lattice [43,44]. Further-
−1
had a slight shift to lower wa-
creation of any free CaO when n < 0.8, and thus only the O1S peak
related to the lattice oxygen appeared. The catalyst 0.8CaO-ZrO also
2
2
had a counterpart of CaO oxygen due to the existence of separated CaO,
judging from the XRD results. Thus, these two O1S reflections were
clearly detected. At the same time, this also provided a strong support
−1
2
2
89 cm for 0.8CaO-ZrO sample due to that some free CaO particles
were formed on its surface (see Fig. 1(a)).
To further verify the generation of CaO-ZrO
2
for the conclusion that CaO-ZrO was in a solid solution state for
2
solid solution, all the
samples of 0.2 ≤ n ≤ 0.8. Additionally, in the case of Ca concentration
for these mixed oxide samples, the measured XPS values were higher
than those from the ICP measurements, implying that their surface was
enriched in Ca (see Fig. S1 in Supplementary Material).
samples were analyzed in-depth by the XPS measurements. For pure
ZrO , its C 1s spectra gave an intense reflection at 284.5 eV and a
2
shoulder peak at 289.1 eV (see Fig. 3(a)). The former one was attributed
to the adventitious carbon, while the latter one was originated from the
2
Textural properties of the nCaO-ZrO catalysts are evaluated by an
4