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water and dried, then were calcined at 560 uC in air for 6 h with a 1
3
. Results and discussion
21
uC min ramping rate. The resultant materials were designated
as xTi–Si-y, where x is the Ti/Si molar percentage in the gels and y
is the molarity of the HCl solution. For comparison, another series
of Ti-incorporated SBA-15 materials, shortly termed xSi–Ti-y, were
3.1 Material characterization
The small-angle XRD patterns of the Ti-incorporated SBA-15
materials prepared by different combination sequences in 2 M
HCl medium, namely xTi–Si-2 and xSi–Ti-2, respectively, show
three distinct diffraction peaks, corresponding to the (100), (110)
and (200) planes of 2D hexagonal p6mm structure. They also show
steep H hysteresis loops at P/P = 0.6–0.8, suggesting that both
7,8
prepared based on the procedures of literature reports, which
were similar to those of xTi–Si-y samples except that TEOS was pre-
assembled with P123 micelles in the synthesis solution for 3 h
before the addition of TTIP.
1
0
series of Ti-incorporated SBA-15 materials possess well-ordered
2
.2 Characterizations
13
and narrowly-distributed mesopores (Fig. S1 and S2, ESI
Moreover, no diffraction peaks of crystalline TiO are observed in
the wide-angle region (Fig. S3, ESI ), implying that Ti should be
homogeneously incorporated in SBA-15.
Table 1, as well as Table S1 (ESI ), show that both series of Ti–
SBA-15 materials have high surface areas (796–896 m g ), large
3
).
Powder X-ray diffraction (XRD) patterns were measured by a
Philips X’pert Pro diffractometer using Cu-Ka radiation operated
at 40 mA and 45 kV. The divergent slits of 1/32 and 1/2 were set for
collecting small- and wide-angle XRD patterns, which showed 2h
regions of 0.5–5u and 15–80u, respectively. Nitrogen physisorption
isotherms were measured by a Micromeritics Tristar 3000
instrument at liquid nitrogen temperature (77 K). Materials were
degassed in vacuum (10 torr) for more than 6 h before the
measurement. The specific surface area was calculated by the
Brunauer–Emmett–Teller (BET) method in the P/P region of 0.05–
2
3
3
2
21
3
21
pore volumes (0.97–1.1 cm g ) and ordered nanopores (ca. 6
nm), akin to those of conventional SBA-15 (entry 1). The Ti
loadings in the solids were analyzed by ICP-MS technique, and
only ca. 5–12.8 mol% of Ti in the synthesis solutions was
incorporated in SBA-15. These results are consistent with previous
reports that Ti is difficult to incorporate in mesoporous silica
23
0
0.25. The pore size distributions (PSDs) were calculated by the
8
prepared in a strong acidic environment. However, the xTi–Si-2
Barrett–Joyner–Halenda (BJH) method using the desorption
branch of the isotherm. The materials were photographed with
a Hitachi S-800 Field Emission Scanning Electron Microscope
samples (entries 2–6), prepared by assembling a Ti precursor with
P123 micelles first, have slightly lower Ti loadings than xSi–Ti-2
(
entries 7–11), which was prepared by adding a Si precursor first.
For xSi–Ti-2 samples where TEOS is pre-hydrolyzed, the soft SBA-
5 mesostructure is formed prior to the addition of the Ti
(SEM), a JEOL JSM-7600F Field Emission Scanning Electron
Microscope (FE-SEM) and a Hitachi H-7100 transmission electron
microscope (TEM). Ti K-edge X-ray absorption spectra were
obtained at the Beamline 17C of National Synchrotron Radiation
Research Center (NSRRC) facility in Hsinchu, Taiwan. The
standard operating conditions were 1.5 GeV and 350 mA. The
photon energy was calibrated with a metallic Ti foil (K-edge, 4966
eV). The diffuse-reflectance (DR) UV-Vis spectra were obtained
with a Hitachi U-3310 spectrometer equipped with an integrating
sphere detector. Barium sulfate (Acros, 99 + %) was used as the
reference. The elemental contents in the bulk were obtained by
inductive-coupled plasma-mass spectrometry (ICP-MS) using a
Perkin Elmer SCIEX ELAN 5000 ICP-MS instrument. Prior to
measurement, the dried samples (ca. 20 mg) were dissolved in a
1
precursor, TTIP. When TTIP is added, the condensation between
Ti–OPr groups and silanol groups on the SBA-15 mesostructure
would form Ti–O–Si bonds and Ti is incorporated into the silica
matrix. In contrast, in xTi–Si-2 samples where TTIP is pre-
2
hydrolyzed first, the hydrolysis product TiOCl is soluble in acid.
The TiOCl species, which interacts with P123 micelles before the
2
addition of TEOS, is probably less effective when condensed with
Si–OEt groups on TEOS. As a result, a lesser amount of Ti is
incorporated into the silica framework of the xTi–Si-2 samples.
The morphology and pore structure of these materials were
photographed by high-resolution scanning electron microscopy
3
(HRSEM) using a retarding technique (Fig. S4, ESI ). The HRSEM
mixed HF–HNO solution and diluted to ppb level.
3
photos show that both series of Ti–SBA-15 materials are rod-like
aggregates in the micrometer level. Indeed, all of the xTi–Si-2 and
xSi–Ti-2 samples with different Ti loadings have rod-like
morphology 1–2 micrometers in size, similar to that of conven-
tional SBA-15. The channeling pores are well-aligned along the
long axis of the particles, and the pore mouths and concave
channels are seen on the top of particles, which are the superficial
2
.3 Catalytic reaction
Liquid phase oxidation of TMP (C
out in a 3-necked round bottom flask (50 mL) connected to a water
cooling condenser and a thermometer. The Ti-incorporated SBA-
9
H12O, Acros, 99+ %) was carried
1
5 catalyst was pre-dried at 200 uC overnight. Typically, a solution
of 0.16 g of TMP in 12 mL CH CN (Acros, 99+ %) was refluxed at
2 uC before adding 0.16 g of the catalyst and 0.408 g of H
Acros, 35%) as the oxidant. The TMP to catalyst weight ratio was
kept at 1, and the H O /TMP molar ratio was kept ca. 3.5. The
17–20
3
features of mesoporous silica templated by block copolymers.
8
(
2
O
2
Fig. 1 compares the DR UV-vis spectra of xTi–Si-2 and xSi–Ti-2
materials. All the spectra possess an intense band centered at 205–
209 nm, which is assigned to the ligand to metal charge transfer
2
2
4,12
products were separated by HP6890 Gas Chromatography (GC)
and qualitatively identified with a HP5973 mass selective detector.
The quantitative analyses of the products were carried out by a
Chrompack 9000 GC instrument equipped with a RTX-5 capillary
column (60 m in length, 0.53 mm in diameter) and a flame
ionization detector (FID), and toluene was used as an internal
standard.
(LMCT) from O to isolated Ti in tetrahedral coordination.
The
intensity of the O A Ti(T ) LMCT increases with the Ti loadings,
d
suggesting that more isolated Ti species are incorporated. When
the Ti/Si ratio in gels is increased to ca. 8–12.5 mol%, two weak
bands appear at ca. 240 and 300 nm. They are assigned to the
LMCT from O to Ti in octahedral coordination and the band gap
transition of TiO
2
nanocrystallites, respectively. These two bands
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RSC Adv., 2013, 3, 12604–12610 | 12605