J.F. Blandez et al. / Journal of Molecular Catalysis A: Chemical 412 (2016) 13–19
15
Fig. 2. XRD and Raman spectrum for the Ni/G sample used as catalyst.
the present study, MNPs of Cu, Ni and Pd supported on various Gs
were prepared. The Cu/G and Pd/G catalysts correspond to those
samples previously reported in the literature [9,10]. G-supported
catalysts were characterized by: (i) chemical analysis to determine
the metal content, that was 3.2 wt%, (ii) TEM allowed to determine
the morphology and average MNP size, and (iii) XPS was used to
establish the oxidation state of Ni. The single layer morphology of
Ni/G was established by AFM.
Fig. 1 shows two representative TEM images recorded for Ni/G
and the histogram of the Ni NP size distribution that gives an
average dimension of 4 nm. The average particle size estimated by
statistical analysis of TEM images coincide with the average particle
the most intense (1 1 1) peak corresponding to Ni metal by applying
the Scherrer equation.
Besides on G, Ni NPs were also supported on (N)G and (B)G. In
the literature there are theoretical calculations as well as experi-
strong anchoring of Ni NPs on G and modulating the electronic den-
can act as active centers in the reaction mechanism cooperating to
the catalysis [24–29]. For the sake of comparison, the present study
also includes Cu NPs supported on (N)G and (B)G that correspond
to the samples already reported [9].
3.1. Catalytic activity
In the initial stage of our work, the addition of dimethylphenylsi-
silane (3a) was selected and proceeded to optimization of the
reaction conditions and screening of the catalyst activity of the
Cu/G has been found previously a good catalyst for the dehydro-
genative silylation of alcohols [9] and, therefore, it was an obvious
candidate to check as catalyst for aldehyde hydrosilylation. As it
can be seen in Table 1, while under certain conditions Cu/G can
the selectivity toward the target compound was always unsatisfac-
tory due to the formation of disiloxane (4a). Under other conditions,
selectivity to the addition product 3a using Cu/G could be high (see
The use of N(G) or B(G) as supports instead of G does not appear
to play a crucial role enhancing the performance of Cu. In con-
trast to Cu catalysts, Pd/G was able to achieve complete conversion
lead to high yields and selectivity toward 3a. Aimed at this purpose
the activity of Ni/G was screened at temperatures between 80 and
140 ◦C and loadings from 0.012 to 0.06 mol% (Table 1, entries 9–17).
As it can be seen in Table 1, using Ni/G at 120 ◦C and working at
0.06 mol% of Ni, very high conversions with almost complete selec-
tivity were attained already at 3 h reaction time, conversion and
selectivity increasing slightly from 3 to 5 h reaction time (Table 1,
entries 10 and 11). Fig. 4 shows the temporal evolution of 1a conver-
sion and 3a yield using Ni/G as catalyst (0.06 mol%) under optimal
conditions. Decreasing the temperature results not only in lower
conversion for 24 h reaction time, but also in a lower selectivity
to 3a due to the formation of disiloxane (4a). Decreasing Ni to
substrate mol ratio from 0.06 to 0.012 leads to a remarkable high
XPS measurements showed the presence of Ni and C in the Ni/G
sample. Fig. 3 presents the experimental high resolution C 1s and
Ni 2p recorded for Ni/G and the best deconvolution to individual
components. According to this analysis there are three types of C at
binding energy (BE) values of 287.7, 284.5 and 282. 5 eV in a atomic
proportion of 7, 41 and 37%, respectively. While the two compo-
nents with the higher BE can be safely attributed to C atoms bonded
to O and graphenic C, respectively, the component with the low-
est BE value is unusual. We attribute this component to graphenic
C interacting with Ni NPs and having higher electron density than
expected for G. This assignment is in agreement with the observa-
tion in XPS that the BE values for Ni atoms is higher than for metallic
Ni. Thus, the high resolution Ni peak in XPS could be resolved into
two peaks at BE values of 855.7 and 854.0 eV with a relative atomic
proportion of 0.2 and 0.1%, respectively. These BE values are unusu-
ally high for Ni(0) that should appear at about 852 eV. Thus, the
data of XPS suggesting Ni(II) does not seem to fit with those of XRD
indicating Ni(0). One possibility to reconcile these two conflicting
experimental data for the Ni oxidation state is to assume that XPS is
probing the external layers of Ni NPs that have become oxidized by
ambient O2. However this external NiO passivating Ni NPs should
be very thin compared to the size of metallic Ni(0), since NiO is
undetectable in XRD. Therefore, XRD will report on the majority
of Ni atoms and XPS on the thin shell. Alternatively, it could be
that the charge transfer that causes a 2 eV shift to lower BE in one
component of graphenic C (37%) would be also responsible for the
apparent 2 eV higher value of Ni(0). This proposal will imply an
interaction between Ni NPs and G, strong enough to shift the BE
value of certain C and Ni atoms in close contact. Whatever the rea-
son, it appears that the Ni supported on G has electron deficiency
and has positive character.