L. Li et al. / Journal of Catalysis 314 (2014) 56–65
59
The physicochemical features of the XS-Sn-MCM-41 materials
were studied by means of a combination of characterization tech-
niques. The complete characterization of three representative sam-
nanoparticles reach their critical size, while longer synthesis time
favors the aggregation of the particles.
2
In agreement with the characterization by TEM and N -physi-
ples (A,
C
and E) will be discussed in detail, while the
sorption, X-ray diffraction (XRD) analysis of XS-Sn-MCM-41-A
shows the typical pattern of MCM-41 with an intense d100 peak
and two smaller d110 and d200 signals (Fig. 3a), while for the mate-
rials characterized by smaller particles (XS-Sn-MCM-41-B to F)
only a broad d100 peak is observed (Figs. 3b, c and S4, SI). The larger
peak width observed for sample E could arise from the higher
degree of aggregation between the particles observed by TEM
and consequent decrease in long-range ordering.
characterization data of all the other materials of the series can
be found in the Supporting Information (SI). Transmission electron
microscopy demonstrated the presence of small nanoparticles and
proved the mesoporous nature of all samples, with the regular hex-
agonal organization typical of MCM-41 materials (Figs. 1 and S1 in
the SI). The particle size of the XS-Sn-MCM-41 materials is sub-
stantially smaller than that of a conventional Sn-MCM-41 refer-
ence sample (Sn-MCM-41-LP), which consists of irregular
particles with a typical size of few hundred nanometers (Fig. S2
in the SI). XS-Sn-MCM-41-A presents a relatively narrow particle
size distribution centered at 118 nm (Table 1 and Fig. 1a). The sam-
ples prepared with higher loading of tin display an even smaller
particle size: for example, XS-Sn-MCM-41-C shows particles in
the range between 20 and 60 nm (Table 1 and Fig. 1b), indicating
a slight change in the formation mechanism of the nanoparticles
with a preference of nucleation compared to growth. This may be
due to a decrease in pH value as a consequence of the increased
The synthesis of mesoporous Sn-silicates proceeds through the
hydrolysis of the precursors, followed by condensation with the
formation of Sn–O–Si and Si–O–Si bonds (and ideally no Sn–O–
Sn bond). The degree of condensation of the materials was studied
2
9
by solid-state Si NMR (Fig. 4a), which shows a broad band that
can be deconvoluted into a mixture of Q [(SiO)
3
SiOH] and Q4
3
3
4
[(SiO) Si] signals. The elevated contribution of Q compared to
standard MCM-41 materials is attributed to the extra-small dimen-
sion of the XS-Sn-MCM-41 solids, which implies a high surface-to-
volume ratio and thus a larger population of surface silanols.
Ideally, Sn should be incorporated as single site with tetrahedral
coordination in the silica framework. The nature of the Sn sites in
the XS-Sn-MCM-41 materials was studied by means of solid-state
4
concentration of SnCl in the reaction medium: the hydrochloric
acid generated upon hydrolysis of the tin precursor partially neu-
tralizes the NaOH present in solution. Notably, TEM revealed that
the additional thermal treatment of the reaction mixture and the
longer reaction time (samples XS-Sn-MCM-41-C to E) favor a mod-
erate increase in the particle size but also the formation of aggre-
gates. Particularly, the TEM image of XS-Sn-MCM-41-E evidenced
the presence of zones of condensation between the XS particles
1
19
Sn NMR and UV–Vis spectroscopy. It should be noted that,
1
19
although the isotopic abundance of the
Sn is high (compared
1
3
29
to C or Si), the detection of this element by Magic Angle Spin-
ning (MAS) NMR is hindered by its long spin-lattice relaxation time
and low wt% in the prepared catalysts. Despite these intrinsic lim-
itations and the high Si/Sn ratio of the samples, a noisy 1 Sn signal
centered at around ꢁ700 ppm could be detected for the materials
displaying higher tin loading (XS-Sn-MCM-41-C and F) after 3 days
19
(Fig. 1c and d). Interparticle condensation was also observed,
though to less extent, in samples C, D and F (Figs. 1b and S1 in
the SI).
1
19
Analysis of the series of XS-Sn-MCM-41 solids by nitrogen
physisorption isotherms reveals that all the prepared materials
have high specific surface area and display a type IV isotherm with
a step at low relative pressure corresponding to a narrow pore size
distribution centered at 2.3 nm (Table 1, Figs. 2 and S3, SI). These
features are characteristic of the long-range order of MCM-41
structures, in agreement with the TEM analysis. All XS-Sn-MCM-
of acquisition (Figs. 4b and S5, SI). This
Sn signal is attributed to
4
+
tetrahedrally coordinated Sn ions connected to four silicon atoms
through oxygen bridges within the silica framework [36,37] or to
hydrated framework Sn(IV) species with an extended coordination
shell including two water molecules [38,39]. Octahedrally coordi-
nated tin in SnO
42]. This peak was not observed in our samples, though the poor
signal-to-noise ratio of the spectra does not allow excluding the
2
gives a sharp peak at around ꢁ600 ppm [40–
4
1 materials display higher specific surface area compared to the
conventional Sn-MCM-41-LP. The values of surface area vary
throughout the series of materials, reaching a remarkable value
2
presence of small amounts of SnO .
Diffuse reflectance UV–Vis spectroscopy allowed highlighting
further the coordination of tin in the XS-Sn-MCM-41 materials.
Metal atoms that isomorphously substitute silicon atoms in the
framework of MCM-41 acquire the typical tetrahedral coordination
of silicate units. Therefore, their absorption in the UV–Vis region is
generally easily distinguished from that due to extra-framework
species. The UV–Vis spectrum of XS-Sn-MCM-41-A reveals a main
absorption band centered at 208 nm corresponding to Sn4+ in tet-
rahedral coordination [36,43,44] (Fig. 5a), evidencing that at low
metal loading the incorporation of tin in the structure is mainly
achieved as single site species. Samples B and C present two addi-
tional signals at 245 and 280 nm (Figs. 5b and S6, SI). The assign-
ment of the band at 245 nm is still a matter of debate: this signal
has been attributed to distorted tetrahedral and penta-coordinated
2
ꢁ1
of 1111 m g for sample XS-Sn-MCM-41-A. A slight decrease in
the specific surface area was observed when increasing the amount
of Sn present in the structure (Table 1, compare XS-Sn-MCM-41-A
and B). A significant drop in surface area was detected for the solid
prepared with a long reaction time (compare XS-Sn-MCM-41-D
and E in Table 1). The decrease in surface area in the XS-Sn-
MCM-41 series is accompanied by an increase in the pore volume
(
Table 1). This trend is attributed to the presence of large interpar-
ticle meso- and macropores, as indicated by the hysteresis loop at
higher relative pressure observed in the N adsorption–desorption
isotherms of all the nanoparticles except XS-Sn-MCM-41-A
Figs. 2b, c and S3, SI). Accordingly, a broad signal in the range
0–70 nm is observed in the pore size distribution of samples
XS-Sn-MCM-41-B to F, being particularly evident for sample E
Fig. 2c). The presence of these disordered interparticle cavities
2
(
2
framework tin sites [44] but also to small extra-framework SnO
2
(
domains [38,45]. The broad absorption around 280 nm has been
assigned to hexa-coordinated polymeric Sn–O–Sn type species
[36,38,43]. The presence of these two additional species in samples
B and C is ascribed to the higher amount of tin precursor and to the
sequential method used for adding the Si and Sn precursors to the
reaction mixture. On the other hand, the UV–Vis spectra of samples
D to F do not exhibit the additional peaks at 245 and 280 nm, indi-
cating that the incorporation of tin in tetrahedral coordination is
can be related to the appearance of zones of condensation between
the particles as observed by TEM. These interparticle voids are
expected to contribute scarcely to the surface area but relevantly
to the pore volume. In order to test this hypothesis, the pore vol-
ume was recalculated by excluding the contribution of the larger
0
pores, i.e. those corresponding to p/p from 0.8 to 1.0 (Table 1).
These values give an estimation of the internal mesopore volume
and, as anticipated, follow the same trend as the surface areas.
These findings suggest that after 2 h at room temperature, the
more efficient if TEOS and SnCl
being added to the reaction solution (Figs. 5c and S6, SI). Although
4
ꢀ5H
2
O are mixed together before