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and STEM/EDX images are shown characterizing the FeRu NPs
synthesized in the presence of HDA. Interestingly, these NPs
presented a different morphology: a wormlike irregular shape.
We have previously demonstrated that HDA promotes the coa-
lescence of Ru NPs to lead to a wormlike morphology as
a result of weak coordination of HDA on the metal surface.[17]
The mean diameter of the worms is approximately 2–3 nm,
which allows characterization by STEM/EDX. The cartography
of elements revealed that Fe and Ru are both present in the
same particles and confirmed the bimetallic nature of the FeRu
NPs.
atomic number has been shown to be a direct proof of segre-
gation in the particles. In the present case, such scaling strong-
ly indicates that FeRu/HDA NPs, although bimetallic as ob-
served by STEM/EDX, are actually not alloyed but organized as
Ru@Fe core–shell particles.
For the other samples, a much smaller and nearly constant
amplitude could be observed. In addition, RDF patterns are
very similar for all compositions with no significant shift of the
first interatomic distance, indicating an average bond length
nearly independent from the Ru/Fe ratio. This pattern is also
very close to the one previously observed for pure Fe particles
prepared by using similar conditions.[18] All these results
strongly suggest that most of the order in the FeRu PVP sam-
ples, as observed by using X-ray scattering, is derived from the
same small particles in all four cases, namely Fe NPs adopting
the manganese beta structure, all with a coherence length of
approximately 1.5 nm. This structure does not exclude a bimet-
allic character of the particles, which would explain the dis-
crepancy between the nearly constant coherence length and
the different sizes observed by TEM. Considering the large
atomic number of Ru compared to that of Fe and the lack of
distances clearly related to the bigger Ru atoms, these results
exclude any kind of extended structure involving Ru, for exam-
ple, Janus-like organization.
Owing to the small size of these NPs, X-ray diffraction meas-
urements only provided broad peaks, which did not allow
a clear understanding of the structure of our NPs. Therefore,
wide-angle X-ray scattering (WAXS) analyses were performed,
which provided more information (see Figure 4).
In summary, the WAXS studies evidence the presence of
a well-ordered core–shell structure Ru@Fe in the presence of
HDA and a more disordered but also core–shell structure of
the type Fe@Ru in the absence of HDA, with a core structure
similar to the one observed for pure iron NPs. The origin of
this discrepancy is not clear but is probably related to the ac-
cessibility of Ru surface to HDA during the initial steps of the
growth of Ru NPs, which then coalesce as in the case of pure
Ru NPs.[17] In the case of the particles prepared in the absence
of HDA, the core is clearly essentially composed of Fe NPs on
which Ru is adsorbed in a disordered way. One explanation for
this surprising reversal of reactivity could be the fact that Ru-
(COD)(COT) reacts in the absence of added amine with aromat-
ic solvents at elevated temperature under H2 to give stable
(arene)(COD) ruthenium(0) species much more stable than Ru-
(COD)(COT).[20] If an excess of HDA is present in the solution, it
coordinates on ruthenium, hence preventing the formation of
the ruthenium–arene complex. This demonstrates once more
the importance of the organometallic chemistry present in so-
lution prior to the formation of NPs.[21] For the purpose of our
catalytic studies, we did not consider the Fe/Ru/HDA system,
which is too different, and concentrated on the NPs obtained
in the absence of additional ligand. It is, however, necessary to
gain more evidence for the presence of increasing quantities
of Ru on the surface of the Fe NPs. For this purpose, surface
and magnetic studies were performed.
Figure 4. WAXS analyses of FeRu NPs with b) 0.2, c) 0.5, and d) 1 equiv. of
Ru, e) in the presence of HDA, and their comparison with a) the experimen-
tal function obtained for pure Fe NPs[18,19] and f) the function computed
from the Fe1Ru1 structure (expanded by 3% for comparison purposes).
r=Coherence length.
The observed coherence length, which corresponds to the
size of crystalline domains, is close to 1.5 nm for FeRu NPs pre-
pared in the absence of HDA. It exceeds 2 nm for the NPs pre-
pared in the presence of HDA. These values are in good agree-
ment with the observations made by TEM/HRTEM analyses.
The structure of the particles prepared in the presence of HDA
(FeRu/HDA) appears very similar to that of both bulk Fe1Ru1
alloy and pure hexagonal close-packed (hcp) ruthenium. Thus,
the obtained radial distribution function (RDF) of FeRu/HDA is
close to the one computed from a model based on the struc-
ture of Fe1Ru1. The coherence length is above 2 nm and a sig-
nificant deviation from the perfect hexagonal structure can be
observed at increasing distances. The average bond length es-
timated on the RDF is, however, larger than the one in the
Fe1Ru1 alloy (0.2624 nm) by a 3% expansion factor, which
makes the average bond length in FeRu/HDA almost identical
to the value in pure ruthenium (0.2705 nm). In previous WAXS
studies on different bimetallic NPs,[19] scaling of all the intera-
tomic distances on the parameter of the species of higher
Surface state studies
We performed first the titration of hydrides present at the sur-
face of the FeRu NPs. The general procedure for the quantifica-
tion of hydrogen atoms adsorbed onto the surface of metallic
NPs through hydrogenation of 2-norbornene has been previ-
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