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tions has not yet been reached owing to experimental
elevated pressure. The results show that under the same
conditions small clusters exhibit significantly higher catalytic
activity than lager ones. The turn-over frequency (TOF) of
the hydrogenation of 1-hexene catalyzed by 6-nm clusters at
20 bar of hydrogen is about 2100 hꢀ1. Under the same
conditions, 3-nm clusters catalyze the hydrogenation of 1-
hexene at a TOF of 3600 hꢀ1. The same trend is also seen in
the hydrogenation of benzene. Nitrobenzene is reduced to
aniline (TOF = 600 hꢀ1 at 608C, 80 bar H2-pressure, 3-nm
clusters).
Herein we have shown that the water-soluble rhodium(I)
complex 2 can be reduced by hydrogen. In this reaction,
rhodium clusters of narrow particle size distribution are
formed which can be isolated and are redispersible in water
without coagulation. The outstandingly high stability is
caused by the electrostatic repulsion of the double negative
charge of the phosphonate ligands covering the clusters. The
mechanistic role of the phosphinophosphonic acid ligands in
the reduction of rhodium is not fully understood, since more
phosphane is oxidized to phosphane oxide than would be
needed for the formal reduction of rhodium(I) to rhodium(0).
The elucidation of the reaction mechanism and stabilization
of water-soluble clusters of other metals by phosphinoposph-
onates are subject of current research.
difficulties. The 2-nm diameter rhodium clusters with their
narrow particle size distribution that we have obtained could
be suitable particles for studying magnetic properties. None of
the samples, however, gave an indication of superparamag-
netic behavior. The temperature dependence of the measured
magnetic moments is dominated by diamagnetic contribu-
tions and contributions from spin-orbit coupling (see Sup-
porting Information). In the group of clusters investigated the
solid-state character clearly dominates over the surface
properties. We are now looking for ways to get ligand-
stabilized clusters in the subnanometer range.
The clusters presented herein are air stable and their
catalytic hydrogenation activity is virtually independent of
the presence of air. To date we have no information on the
oxidation state of the rhodium surface atoms and whether
oxide ions are present on the cluster surface. The character-
ization of cluster surfaces is a general problem which is very
often not addressed. X-ray photoelectron spectroscopy (XPS)
is a suitable method for analyzing surfaces. XPS provides
information on the oxidation states of the detected elements
when suitable reference standards are available. We used
metallic rhodium and RhCl3·3H2O as references und deter-
mined the position of the Rh 3d5/2 line (see Supporting
Information). The energies determined are in good agree-
ment with the values found in the literature. The Rh 3d5/2 line
of 6-nm rhodium clusters was determined to be at EB =
308.2 eV, it is shifted by DE = 1 eV relative to metallic
rhodium. Clearly, the electronic structure of clusters, even
of this size, is different from that of rhodium metal.[13] The
reason for not being able to get any distinct information on
the surface atoms of the clusters using XPS lies in the
dimensions of the clusters. A wavelength of l = 3.29 nm is
calculated for the photoelectrons of the Rh 3d5/2 signal with
Experimental Section
1H and 31P NMR spectra were recorded on a Bruker spectrometer
DRX200, 13C NMR spectra on a Bruker DRX500. For HRTEM
imaging electron microscopes JEOL 2000F and Philips TEM CEM-
200 FEG were available. In the Figures we have given the mean
values and standard deviations of the cluster diameters. The HRTEM
experiments were carried out using an acceleration voltage of 200 kV.
The element specific analyses were performed using a built-in EDX
system (EDAX). The images were taken using a CCD camera
(Gatan). Susceptibilities were measured in the temperature range 4 to
pffiffiffiffiffiffiffiffi
[14]
E
kin = 1179.2 eV by using the relation l = 0.096 Ekin
.
This
result means that XPS does not characterize the cluster
surface but measures the electronic state of the whole cluster!
The HRTEM and electron diffraction data show that the
rhodium clusters virtually exist as single crystals. The
interplanar spacing according to the contrast maxima and
electron diffraction diagrams are in accord with the structural
data for metallic rhodium. Experiments using locally resolved
element-specific energy-dispersive X-ray (EDX) analysis
(EDAX system) give evidence for the presence of a phos-
phorus-containing ligand shell surrounding the rhodium
nanoclusters.
300 K using
a MPMS-XL5-SQUID magnetometer (Quantum
Design), the applied magnetic field was 1 T. Data were corrected
for the diamagnetic contribution of the sample holder. XPS measure-
ments were performed on an ESCALAB 200x. AlKa radiation (hn =
1486.6 eV) was used as excitation source.
The synthesis of the phosphane ligand was carried out under a dry
nitrogen atmosphere using Schlenk technique according to the
procedure outlined by Roundhill and co-workers.[15] The detailed
synthesis procedure as well as NMR spectroscopic data are given in
the Supporting Information. The reaction vessels used for cluster
synthesis were cleaned using aqua regia to eliminate any metallic
impurities.
2: A solution of Na2-1·2H2O (0.30 g, 0.80 mmol) in methanol
(20 mL) was added to a stirred suspension of [{Rh(cod)Cl}2] (0.20 g,
0.40 mmol) in methanol (20 mL). The mixture was stirred for 20 min.
The rhodium complex dissolves and NaCl precipitates causing a slight
clouding. The precipitate was removed by filtration using a glass frit.
The resulting solution was evaporated in vacuo to yield 0.40 g (90%)
of a powdery yellow solid. 31P{1H}-NMR (81 MHz, D2O): [ABX]-spin
The data on the catalytic activity of the clusters is shown in
Table 1. All the experiments on biphasic catalysis were
performed in a stainless steel autoclave with glass insert at
Table 1: Hydrogenation of 1-hexene and benzene at 208C using rhodium
clusters of varying size as catalysts.
system d = 23.3 (3JP, P = 11.4 Hz, PV), 22.2 ppm (3JP, P = 11.4 Hz, PIII
;
1-Hexene
H2 pressure
[bar]
Benzene
H2 pressure
[bar]
1JP, Rh = 154.8 Hz, PIII); H NMR (500 MHz, CD3OD): d = 7.8–7.3 (m,
10H; C6H5), 5.5–5.0 (m, 2H; CH trans to P), 2.9–2.7 (m, 2H; CH trans
to O), 2.5–1.7 ppm (m, 12H; CH2); IR (KBr): n˜ = 3421br, 3054w,
2918w, 1632br, 1483s, 1435m, 1159s, 1099m, 1041s, 744m, 696 cmꢀ1 s;
MS (FAB+, NBA): m/z 527 (73.6, [M+H]+), 549 (7.5% [M+Na]+.
Rhodium cluster (6 nm): 2 (0.16 g, 0.30 mmol) was dissolved in
water (15 mL). The solution is stirred at ambient temperature for 2–
1
Cluster size
[nm]
TOF
[hꢀ1
TOF
]
[hꢀ1
]
6.2
3.1
2.0
20
20
20
2100
3600
5700
20
20
20
1
50
80
1166
ꢀ 2007 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2007, 46, 1164 –1167