R.A. Garcia et al. / Journal of Catalysis 274 (2010) 221–227
223
unit. Previously, the samples were outgassed at 200 °C for 4 h un-
der nitrogen flow. The surface area measurements were performed
according to the BET method from nitrogen adsorption points in
the range P/P0 = 0.05–0.2. Pore size distribution was determined
applying the Barrett–Joyner–Halenda model (BJH) to the adsorp-
tion branch of the isotherm, assuming cylindrical pore geometry.
For each sample, the average pore size was estimated as the diam-
eter corresponding to the maximum of the pore size distribution
curve. Total pore volume was taken at a relative pressure P/P0 of
0.985
the chiral tartrate derivative employed as chiral precursor,
protected L-(+)-dimethyl tartrate (DMT), is mixed with the
(N-methyl-3-aminopropyl)trimethoxysilane under the weak acidic
conditions needed for synthesizing
a SBA-15-like framework
material, a transamidation reaction takes place, leading to the
bis-silylated chiral precursor. Besides, the presence of 1,2-bis(tri-
ethoxysilyl)ethane (BTSE) and the copolymer Pluronic P123
triblock copolymer provides the mesoscopic ordering to the final
material. Therefore, during the in-situ transamidation reaction,
the hydrolysis of the chiral and non-chiral bis-organosilane silica
precursors and the condensation of these latter species around mi-
celles formed by the structure-directing agent are readily accom-
plished leading to a chiral PMO material.
X-ray powder diffraction patterns were collected on a Philips
X’pert diffractometer equipped with an accessory for low-angle
measurements. XRD analyses were recorded using the Cu K
a line
in the 2h range from 0.5° to 10° with a step size of 0.02° and a
counting time of 10 s.
After the optimization of the aging time and the hydrolysis and
condensation stage, the progressive incorporation of higher
amounts of protected DMT was carried out. Thus, Table 1 summa-
rizes the physico-chemical properties of the obtained chiral PMOs.
Fig. 1 shows the N2 adsorption–desorption isotherms for the
synthesized materials. BET surface, pore size distribution (inset
in Fig. 1) and total pore volume are obtained by processing the
adsorption branch of the collected isotherm data. Chiral PMO-10,
20, 30 and 50 materials show type IV nitrogen adsorption–desorp-
tion curves, according to the IUPAC classification, which are typical
of mesoporous solids. The steep adsorption step detected around P/
P0 = 0.65–0.70, corresponding to the capillary condensation of
nitrogen in uniform pores, evidences the formation of well-struc-
tured solid materials with narrow pore sizes distributions, as it is
derived from the BJH analysis shown in the onset. On the other
hand, the ordering degree seems to be influenced by the content
of the organic functionality. Although the width of the pore size
distributions seems not to be greatly modified, the area below
the pore size distribution, which is the total pore volume, or at
least the mesopore volume, decreases when increasing the organic
ligand loading. Besides, the mean pore size is slightly shifted to
lower values because of the same reasons already exposed. Finally,
chiral PMO-70 exhibits a negligible yield to solid, indicating that
higher loadings of bis-organosilane inhibit the formation of these
materials. Thereby, a significant amount of BTSE must coexist in
the media besides the chiral precursors to provide enough meso-
scopic ordering to the final chiral PMO SBA-15-type materials.
Nevertheless, chiral periodic mesoporous solid materials with a ra-
tio BTSE/DMT as high as 50:50 have been synthesized, which,
according to the earlier reports, is the highest organic chiral load-
ing incorporated into the three-dimensional structure of a PMO
material, to the best of our knowledge. Although for this 50:50
precursor mixture, the incorporation of chiral functionality suffers
a slight decline compared to sample S20, as shown in Table 1
(HCNS column), it is still high enough and the material sufficiently
ordered, as to endorse the previous comment.
Fig. 2 displays the XRD patterns of the template-free synthe-
sized chiral PMOs at increasing chiral organic precursor loadings.
The presence of the characteristic diffraction at 2h = 0.8–0.9°, cor-
responding to the d100 basal plane of SBA-15-type materials, con-
firms the formation of a mesoporous structure for those solids.
These materials preserve the periodic structure even after template
P123 removal by washing with ethanol, related probably to the
beneficial action of hydrothermal treatment during the framework
consolidation.
As displayed in Table 1, a reduction in the BET surface area and
pore size diameter occurs as the chiral organic precursor loading is
increased. Additionally, and excepting the PMO-10 sample that
shows a slight decrease, the general trend points out to wall thick-
ness reinforcement as the pore size diameter declines, which is in
accordance with results previously described for other PMO mate-
rials [14]. The observed tendency may provide an idea of the
importance of the organic moiety in the final materials ordering.
FTIR analyses were collected, using the KBr buffer technique, on
a Mattson Infinity series apparatus in the wavelength range from
4000 to 400 cmÀ1 with a step size of 2 cmÀ1 and collecting 64 scans
for each analysis. The samples were also placed in a catalytic cham-
ber HVC-DPR (Harrick Scientific Company) where they were
heated at different temperatures under vacuum (<10–4 mbar) with
a 1.5 °C/min heating rate.
Solid-state 13C and 29Si MAS NMR experiments were performed
on a Varian Infinity 400 MHz spectrometer fitted with a 9.4 T mag-
net. These nuclei resonate at 100.53 and 79.41 MHz, respectively.
An H/X 7.5 mm MAS probe and ZrO2 rotors spinning at 6 kHz were
used. On CP experiments, the cross-polarization time was deter-
mined to guarantee the total proton polarization verifying the
Hartmann–Hann condition. For 13C acquisition,
of scans, repetition delay and contact time were 4.25
scans, 3 s and 1 ms, respectively. The 29Si CP experiments were
performed for 3000 scans, /2 pulse of 3.5 s and 15 s of repetition
p/2 pulse, number
l
s, 2000
p
l
time, while the contact period was 10 ms since cross-polarization
depends upon heteronuclear dipolar interaction, the greater dis-
tance the larger cross-polarization time. 13C and 29Si chemical
shifts were externally referenced to adamantane and tetramethyl-
silane, respectively.
2.4. Catalytic tests
Reaction tests for the asymmetric oxidation of sulfides were
carried out under a nitrogen atmosphere using standard Schlenk
techniques (Scheme 2). The PMO used as solid chiral ligand was
previously outgassed and dried in a Kugelrohr apparatus at
130 °C under vacuum (1 torr) overnight before being employed in
the catalytic tests. Inert conditions were ensured by passing a
continuous nitrogen stream through the reactor, which was main-
tained during the overall operation. Freshly distilled dichlorometh-
ane (50 mL) was then transferred into the reactor via syringe, and
the mixture was magnetically stirred. Titanium isopropoxide
(0.056 mmol) and 2-propanol (0.224 mmol) were added drop by
drop to the resultant suspension. The mixture was then aged for
2 h in order to promote the contact between the titanium species
and the chiral ligand sites present in the PMO material. After the
aging step, both cumyl hydroperoxide (CHP, 0.56 mmol) and
thioanisole (0.56 mmol) were added separately by dropping onto
the catalytic suspension. Sample aliquots were collected in order
to assess the evolution of the reaction. The mixture was allowed
to react for 24 h.
3. Results and discussion
The mesostructured organosilicas with chiral ligands incorpo-
rated into the framework were obtained following a new and easy
methodology, the procedure being represented in Scheme 1. Once