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3008C for 30 min, respectively, with a heating rate of 58Cminꢀ1
.
Synthesis of Sn-containing materials
FTIR spectra were recorded in situ at these temperatures. Back-
ground correction was performed by subtracting the spectrum of
the dehydrated wafer recorded at 1008C. Integration of the signals
for determining the amount of Lewis and Brønsted acid sites was
performed by using the Fityk curve fitting program. 1H NMR and
119Sn MAS NMR spectra were recorded by using a Bruker DMX-500
NMR spectrometer with a 4 mm zirconia rotor at a spinning rate of
Sn-Beta zeolite synthesized in fluoride media (Sn-BEA-HF)[18] and
Sn-MCM-41[46] were synthesized according to established proce-
dures. Nanosized Al-Beta zeolite precursors with synthesis Si/Al
ratio of 25, 50, and 100, denoted as BEA-25, BEA-50, and BEA-100,
respectively, were prepared according to a modified procedure re-
ported by Mintova et al.[35] A solution of TEAOH in water (28.1 g)
and Al(OiPr)3 were added Ludox SM-30 (37 g) and the mixture was
stirred for 20 h, after which a clear to slightly opaque (for higher
amounts of Al precursor) solution was formed. The mixture was
subsequently transferred to a Teflon-lined steel autoclave and
placed in an oven at 1008C for 18 days under static conditions.
The resulting zeolites were collected by centrifugation, washed
thoroughly with water, and dried in air. The zeolites were calcined
at 400 and 5508C (both 18Cminꢀ–1, 10 h), successively. Dealumina-
tion was performed by heating in 65% HNO3 (50 mLgꢀ1) at 1108C
overnight. Residual HNO3 was removed by thorough washing with
demineralized water until the pH of the washings was neutral. The
resulting materials are denoted as Deal-BEA-25, Deal-BEA-50, and
Deal-BEA-100. Prior to modification with Sn, the dealuminated BEA
zeolites were dried in vacuo at 1708C for 3 h in a Schlenk flask. Sn
was incorporated by adding an excess of approximately three sila-
nol nest equivalents of anhydrous SnCl4 at 1008C under an Ar at-
mosphere and the mixtures were stirred overnight. To remove un-
reacted SnCl4 from the zeolite pores, the materials were thorough-
ly washed with methanol at least six times and dried in air. To
remove residual chloride and to complete the condensation of the
Sn centers into the framework, the materials were recalcined at
5508C (18C minꢀ1, 5 h). The final Sn-modified catalysts are denoted
as Sn-BEA-25, Sn-BEA-50, and Sn-BEA-100.
1
10 kHz. H chemical shifts were referenced to Si(CH3)4, 119Sn chemi-
cal shifts were referenced to SnO2 (d=ꢀ604 ppm).
Catalytic activity measurements
DHA was dissolved in methanol (0.25m) and 2.5 mL of the solution,
together with the catalyst (40 mg), was added to a 4 mL thick-
walled glass vial. Reactions were performed at 708C under stirring
(500 rpm) and mixtures were analyzed by GC-FID with n-decane as
an external standard on a Shimadzu GC-17 A apparatus equipped
with a Restek Rxi-5 ms column (30 mꢁ0.25 mm, df =0.25 mm). Re-
actions used to determine the activation energy of the reaction
were performed at 50, 60, and 708C. Identification of unknown
compounds was performed on
a Shimadzu QP5050 GC-MS
equipped with a Stabilwax column (30 mꢁ0.32 mm, df =0.5 mm).
Recycle experiments were performed in a 12 mL screw-capped
glass vial. The catalyst was recovered by centrifugation after each
cycle, washed twice with methanol, and dried in air.
Computational details
DFT calculations were performed by using the Vienna ab initio Sim-
ulation Package (VASP 5.2).[47] The generalized gradient exchange-
correlation PBE functional was used.[48] The electron–ion interac-
tions were described by the projected augmented wave (PAW)
method.[49] Geometry optimization was performed with a plane-
wave basis set with a cut-off of 400 eV. The calculations were as-
sumed to be converged, when the forces on each atom were less
than 0.05 eVꢂꢀ1. Brillouin zone-sampling was restricted to the G
point. Optimized cell parameters for all-silica zeolite Beta are a=
b=12.66 ꢂ, c=26.40 ꢂ. Two candidate active sites for Sn-Beta
were considered. One is the closed SnIV site (Sn(OFSiF)4, OF and SiF
represent the framework oxygen and silicon atoms, respectively).
The other is generated by H2O dissociation over the framework Sn-
O-Si moiety, resulting in the open (SiFOF)3SnOH···HOFSiF active site.
Sn atoms were introduced at T6 tetrahedral site of the BEA frame-
work. The R-HMP and R-methyl lactate were used as the initial and
final states to study the mechanism of the intramolecular hydride-
shift reaction. The minimum reaction energy path and correspond-
ing transition state were determined by using the nudged-elastic
band method (NEB) with improved tangent estimate.[50] The maxi-
mum energy geometry along the reaction path obtained with the
NEB method was further optimized by using a quasi-Newton algo-
rithm. In this step, only the extraframework atoms and the atoms
in the first coordination sphere of Sn were relaxed. Frequency anal-
ysis of the stationary points was performed by means of the finite
difference method as implemented in VASP. Small displacements
(0.02 ꢂ) were used to estimate the numerical Hessian matrix. The
transition states were confirmed by the presence of a single imagi-
nary frequency corresponding to the reaction coordinate. To ac-
count for the van der Waals (vdW) interactions between zeolite
voids and carbohydrates, all calculations were carried out with the
DFT-D2 method[51] as implemented in VASP 5.2.
Characterization
X-ray diffraction patterns were recorded on a Bruker D4 Endeavor
diffractometer by using CuKa radiation in the 2q range 5–608 with
a scanning speed of 0.018sꢀ1. Elemental analyses were carried out
by using a Spectro Ciros CCD ICP optical emission spectrometer
with axial plasma viewing. For analysis of the materials HF/HNO3/
H2O 1:1:1 was used as matrix. Thermogravimetric analyses to deter-
mine the water content of the solid samples were performed on
a Mettler TGA/DSC-1 apparatus using 70 mL alumina crucibles.
Helium was used at a gas flow rate of 40 mLminꢀ1. Argon physi-
sorption measurements were performed at ꢀ1868C on a Micromer-
itics ASAP2020 apparatus in static measurement mode. In a typical
experiment, a zeolite sample (typically 100 mg) was outgassed at
2008C for 8 h prior to the measurement. The Brunauer–Emmett–
Teller equation was used to calculate the specific surface area from
the adsorption data in the p/p0 range 0.05–0.35. The mesopore
volume was calculated by applying the Barrett–Joyner–Halenda
(BJH) method on the adsorption branch of the isotherm and the
micropore volume was calculated by using the t-plot method. FTIR
spectra of pyridine adsorbed to the zeolites were recorded by
using a Bruker Vertex V70v system. The spectra were acquired as
an average of 32 scans at a resolution of 2 cmꢀ1 The samples were
prepared as thin self-supporting wafers of 5–15 mgcmꢀ2 density
and placed inside a controlled-environment infrared transmission
cell. Prior to pyridine adsorption, the catalyst wafer was heated to
5508C at a rate of 28Cminꢀ1 under vacuum (p<5ꢁ10ꢀ6 mbar) and
maintained at this temperature for 3 h. After cooling to 1008C, pyr-
idine was introduced in the cell in static vacuum for 30 min. Physi-
sorbed pyridine was removed in vacuo for 30 min. The evacuated
sample containing chemisorbed pyridine was subjected to a tem-
perature-programmed desorption sequence at 100, 200, and
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