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formed with the DMFit program.[53] ToF-SIMS experiments were
performed with a TOF.SIMS 5 instrument from ION-TOF GmbH by
using a 25 keV bismuth liquid metal ion gun (LMIG). The primary
ion beam of 25 keV Bi3+ was operated in a static mode with a pri-
mary pulsed beam current of 2.5 pA. Appropriate charge neutrali-
zation (20 eV electronic flood gun) was used to avoid charging of
the samples during data collection. The detection was performed
in the mass range from 1 to 800 mu. With a data acquisition time
of 100 s, the total fluence did not reach 1012 ionscmÀ2, ensuring
static conditions. The XPS measurements were performed with a
Thermo Scientific ESCALAB 250 by using monochromatic AlKa
(1486.6 eV) radiation with a spot size of about 600 mm. The high-
resolution spectra were collected with 20 eV pass energy at a take-
off angle of q=908, and the C 1s peak position of 284.6 eV was
used to calibrate the spectra. After Shirley background subtraction,
XP spectra were deconvoluted into Gaussian–Lorentzian compo-
nents.
Immobilization of catalysts on titanium oxide-based parti-
cles
AgBF4 (0.06 mmol) was added to a solution of [Rh(COD)Cl]2
(14.8 mg; 0.03 mmol) in THF (5 mL).[40] The mixture was stirred
overnight and then filtered through a Millipore apparatus to
remove AgCl. The filtrate was then added to the desired ligand
(0.12 mmol) suspended in 5 mL of water, and the mixture was
stirred for 48 h at room temperature. Then titanium tetraisoprop-
oxide (0.4 mL) and 1m sodium hydroxide (0.5 mL) were added and
the mixture was stirred for two additional days. The reaction
medium was then centrifuged, and the collected solid was washed
four times with distilled water in centrifugation tubes and then
twice with acetone. After filtration, the supported catalysts were al-
lowed to dry at room temperature, and an amount of 400–450 mg
of solid was typically obtained, depending on the nature of the
ligand used (i.e., mono- or bis-functionalized). From the amount of
rhodium/bipyridine complex immobilized on each supported cata-
lyst (see Table 1), the calculated rhodium loading was about
0.25 mmol Rh per gram of catalyst. A full analysis of the chemical
composition was performed for one of the supported catalysts by
elemental analysis (C, H, N) and ICP-MS (Na, P, Rh, Ti). The 6,6’-C12
compound was selected, and the experimental values allowed an
approximate formula for this material to be proposed:
TiO1.5(OH)·3H2O·0.3iPrOH·Na0.33·[Rh(PO3(CH2)12ON=CH-bpy-CH=
Qualitative elemental analysis by SEM-EDX was performed with a
JEOL JSM 5800 LV scanning electron microscope with SAMx SDD
EDS instrument. ICP-AES was performed with a Thermo Fisher Sci-
entific iCAP 6300 instrument. For the calibration curve, solutions at
different concentrations of rhodium were prepared from a com-
mercial ICP standard solution of Rh at 1000 mgmLÀ1 in a 1% aque-
ous solution of nitric acid.
NO(CH2)12PO3)2]0.04. The resulting experimental and calculated
values are the following: Ti (calcd 20.7%, exptl 20.6%), Rh (calcd
1.8%, exptl 1.7%), Na (calcd 3.3%, exptl 3.3%), P (calcd 2.2%, exptl
2.3%), N (calcd 1.9%, exptl 1.9%), C (calcd 19.6%, exptl 18.8%), H
(calcd 6.0%, exptl 5.5%).
Computational studies
First-principles calculations were performed in the framework of
DFT by using the VASP code.[54] The generalized gradient approxi-
mation (GGA) was adopted to treat the exchange-correlation term
with the Perdew, Burke, and Ernzerhof (PBE) functional.[55] Projected
augmented wave (PAW) potentials were used to describe core
electrons.[56] During the geometry optimization, valence electrons
were expanded with a plane-wave basis set by using a 400 eV
energy cutoff. Dispersion corrections were included by using DFT-
D2,[57] that is, an empirical dispersion term was directly added to
the Kohn–Sham energies. Atomic positions of all systems were op-
timized with a total energy threshold of 10À3 eV while taking into
account only the G-point for the Brillouin zone sampling. For the
TiO2 surface, a (101) anatase slab with two stacked O-Ti-O layers
was considered. This thickness was proven to be sufficient to
model anatase surfaces.[58,59] The slab was built with dimensions of
2119 in the xy plane. The size of the slab was chosen to pro-
vide sufficient separation between periodic images when the opti-
mized isolated molecule was adsorbed, in order to avoid spurious
interactions. Indeed, the adsorbate–adsorbate distance was greater
than 14 in the x and y directions, while the minimum adsorbate–
surface distance was 24 in the z direction. The structural optimi-
zations of the slab for the bare surface and hybrid systems were
performed by moving the atoms of the top layer in direction (001)
only, while the bottom layer was kept fixed. The molecules were
chemisorbed onto the surface by bonding its oxygen atoms to the
unsaturated titanium ions of the surface. Depending on the
degree of coordination, the dissociated proton(s) from the mole-
cule was(were) transferred to the surface and bonded to an
oxygen atom with a distance of 8 from the adsorption site in
order to prevent any influence on the intersystem interaction. The
chemical-shift calculations were performed with a higher 500 eV
energy cutoff for the plane-wave basis set. A denser 221 Mon-
khorst–Pack k-points grid was also adopted for these calculations.
The shifts were calculated by considering only the valence contri-
bution; the core contribution was kept frozen.
General procedure for the hydrogenation of alkenes
The appropriate amount of catalyst (i.e., ca. 40 mg corresponding
to 9.5 mmol of rhodium, vide supra) was transferred to a 30 mL
glass-coated stainless steel autoclave. Methanol (3 mL), 1m aque-
ous sodium hydroxide solution (47.5 mL; NaOH/Rh=5) were then
added. The autoclave was purged six times with argon and then
three times with hydrogen, and the final H2 pressure was adjusted
to 40 bar. The mixture was stirred for 4 h in a sand bath at 308C.
After this time, the pressure of the autoclave was released, and 6-
methyl-5-hepten-2-one (0.95 mmol, rhodium/substrate ratio:
1.0 mol%) was added. Then, the autoclave was purged six times
with argon and then three times with hydrogen, and the final H2
pressure was adjusted to 40 bar. The mixture was stirred in a sand
bath at 308C for the desired reaction time and then centrifuged.
The liquid phase was then isolated and analyzed by gas chroma-
tography to determine the conversion, the nature of the reaction
products, and their yields. These measurements were performed
with a Hewlett-Packard HP 6890 chromatograph with a J&W Scien-
tific DB-1 column (l=30 m, i.d.=0.25 mm, film thickness=
0.25 mm), equipped with
a FID detector (H2 as carrier gas
(1.5 mLminÀ1); temperature program: 608C (1 min), 808C
(2.58CminÀ1). Retention times: 6-methylheptan-2-one (5.25 min), 6-
methylheptan-2-ol (5.72 min), 6-methyl-5-hepten-2-one (6.05 min),
6-methyl-5-hepten-2-ol (6.43 min).
Acknowledgements
P. Janvier is gratefully acknowledged for his help with the ICP-
AES measurements and analysis of the phosphorus content in
solution using the Ames method. F. X. Lefvre is gratefully ac-
knowledged for his help with the SEM observation of the sup-
Chem. Eur. J. 2018, 24, 2457 –2465
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