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L. Dussault et al. / Journal of Physics and Chemistry of Solids 67 (2006) 1162–1167
Table 1
with a value of x located in the range 0.1–0.2. According to
TPR and XRD results (not shown here), the reduced catalysts
prepared at 1023 K are composed of Cu0, Ni0, possibly Ni–Cu
alloy, MgO, NiAl2O4 and MgAl2O4.
Structural parameters of carbon nanofilaments: interlayer distance d002, average
size of coherently scattering domains along the normal to graphene layers (Lc)
and in the graphene plane (La) from XRD
x
0.2
0.1
0.1
Preparation method
d002 (nm)
Regular
0.331
8.3
Regular
0.334
5.9
Colloid mill
3.2. Carbon nanofilament growth
0.338
5.6
Lc (XRD) (nm)
La (XRD) (nm)
ID/IG (Raman)
La (Raman) (nm)
In agreement with the literature [7], an excess content of
copper dramatically decreases the carbon yield and the
catalysts with xS0.5 show very little activity. Just as Al, Cu
is relatively non-catalytic and has a dilution effect on the active
sites of Ni. However, it enhances both the carbon diffusion and
reaction rates and thus promotes the catalytic activity when it is
incorporated in small quantities. In agreement with the
literature [7], the maximal carbon yield is reached with
Ni0.9Cu0.1MgAl, i.e. 3.8 wt% of Cu (Ni0.8Cu0.2MgAl, i.e.
7.6 wt% of Cu and Ni0.95Cu0.05MgAl, i.e. 1.9 wt% of Cu, are
slightly less active).
7.3
6.2
4.2
2.4
1.3
1.7
1.8
3.4
2.6
La from Raman spectra is calculated with ID/IGZ4.4/La [15].
In particular, the ratio ID/IG is inversely proportional to the
dimension La, i.e. the average planar size of the perfect
graphenes [15]. The values reported in Table 1 indicate that the
CNFs produced with Ni0.8Cu0.2MgAl have a higher disordered
structure (smaller La) than those obtained with Ni0.9Cu0.1-
MgAl. The discrepancy between La values obtained from XRD
and Raman spectroscopy comes from the underestimation of
values obtained with Raman due to the dominant effect of the
smallest coherent domains [14]. The larger difference between
the results of the two techniques for CNFs from Ni0.8Cu0.2-
MgAl indicates that they present a higher dispersion of
crystallite sizes although the average polyaromatic coherent
domains are larger (following both dimensions La and Lc).
Fig. 2a shows typical TEM images of the CNFs formed over
either Ni0.8Cu0.2MgAl or Ni0.9Cu0.1MgAl. Nanofilaments
actually nanofibers (i.e. not hollowed) are frequently attached
to the catalyst particle where they have grown from (Fig. 2a).
The metallic Ni–Cu particle is detached from the support
possibly because it is pushed up by the fiber during its growth
[4]. Octahedral or cubo-octahedral catalyst particles of
relatively large size (100–400 nm) were found well crystal-
lized, giving rise to sharp and bright dots in electron diffraction
patterns (Fig. 2b, arrows), and to lattice fringes in high-
resolution TEM images (Fig. 2e). The sample appeared quite
homogeneous (a very large majority of the filaments are from
the same type) with only a scarce occurrence of other filament
types (herringbone type, not illustrated). Fig. 2d indicates that
the graphene layers are oriented parallel to the particle surface,
making them perpendicular to the filament axis (‘platelet’
texture). Actually, arrows in Fig. 1a indicate the very location
where the nanofilament was about to split, due to easy gliding
resulting from the weak van der Waals forces between stacked
graphenes. Square-like particles that make up most of the
specimen after the TEM preparation procedure (grinding) are
therefore merely platelet-CNF fragments (not illustrated), most
of them exhibiting the same graphene display. Interestingly,
such a graphene display implies that the fiber surface is actually
made of free-graphene edges, meaning that high surface
reactivity and surface energy are expected. As stated by
numerous Bragg fringes (dark contrasts), the carbon nanofila-
ments decorated with the nanotexture are quite high. Electron
diffraction patterns (Fig. 2b) exhibit rather sharp and dotted
reflections together with multiple order reflections (e.g. 002,
004, 006) which both indicate large coherent domains, which is
The XRD patterns of the reaction products (not shown here)
correspond exactly to the superposition of the diffractogram of
reduced catalyst and of polyaromatic carbon typical of
graphene-based materials such as carbon nanofibers and
multi-walled nanotubes. Thus, it seems that the catalysts do
not suffer any degradation during the first hours of reaction and
sharpness of the related peaks indicates that the carbon formed
presents a relatively high nanotexture, which corresponds to
relatively large defect-free graphenes.
Beside its doping character, copper has a strong effect on the
lifetime of the catalysts. This is shown by the comparison of
carbon growth rates on Ni0.9Cu0.1MgAl (xZ0.1) and NiMgAl
(xZ0). While the latter decreases only after 15 min and is close
to zero after 1 h, the former is quasi-constant during the whole
duration of the test showing a high stability. The benefit of Cu
has already been noted in the case of hydrogenation catalysts.
Indeed, Cu favors a higher hydrogen mobility, it has high
affinity with graphene-based structures, and tends to inhibit the
encapsulation of Ni active sites by polyaromatic carbons [13].
3.3. Nanofilament features
Because of their very low yield, we have not examined the
carbon products formed using the high Cu content catalysts,
but only those obtained with Ni0.8Cu0.2MgAl and Ni0.9Cu0.1-
MgAl synthesized with both methods. In agreement with the
previous observations, the size of the catalyst particle and, in
consequence, the diameters of the nanofilaments are smaller
when a lower Cu content catalyst is used and this effect
increases for the catalysts prepared with the colloid mill
method. The filaments generally show a diameter in the
range 60–100 nm (with some thicker ones up to 400 nm) for
Ni0.8Cu0.2MgAl from both preparation methods, 30–50 nm for
Ni0.9Cu0.1MgAl (traditional preparation mode) and 20–50 nm
for Ni0.9Cu0.1MgAl (from colloid mill).
The graphene-based structure of the nanofilaments observed
in XRD patterns is confirmed by the Raman spectra (not shown
here). The frequency and intensity of the D- and G-Raman
bands provide information about the crystallinity of CNFs [14].