8
Li et al. Sci China Chem
4
4], whereas the formation of CH CH OH is rather rare.
3 2
There are several possible pathways for CO hydrogenation
2
reactions towards CH on Cu, including the formate and
4
reverse water gas shift (RWGS) pathways, both via an
*
H CO intermediate (from *H COOH→*H CO and
2 2 2
*
CHO→*H CO, respectively) [45]. The former is much
2
more accepted as the formation of CH via CO hydro-
4
2
genations is found experimentally to be much faster than the
conversion via CO hydrogenations over the Cu/ZnO cata-
lysts [46]. The latter pathway is suggested to be inhibited for
the catalytic reactions over pure Cu, as the *CHO, precursor
intermediate for *(H CO), tends to dissociate into *CO and
2
*
H [47]. The IF and SA sites are significantly different from
the surface sites of clean Cu crystals. For the low-coordinate
IF and SA sites, the RWGS pathways may present with the
formation of a comparatively stable *CHO intermediate,
while the formate pathway can be suppressed as the formate
pathway involves more than one Cu sites and bidentate ad-
sorption. The SA sites have no neighboring Cu, whereas SA
Cu sites of Cu@C have approximately half of maximally
allowed the number of surface Cu neighbors, which may
suppress the formate pathway, especially for the second C1
intermediate adsorbate. The question is whether the terminal
product *CO for pure Cu can further react to form more
reactive intermediates on Cu@C and hence extend the
RWGS pathway. To find this out, the activation barriers for
Figure 6 (a) Predicted reaction energy and activation barriers for the
dissociation reactions of CHO at the IF site of Cu@C and at the Cu(111)
site at the DFT level. (b) The optimized geometry for the *CHO, *CO+*H,
and the transition state (TS) for CHO dissociations. (c) Predicted reaction
energy and activation barriers for the coupling reaction of two CHO ad-
sorbates at different Cu sites of Cu@C and Cu crystals at the DFT level. (d)
The optimized geometry for the *(CHO) , *(OHC–CHO), and the transition
2
state (TS) for CHO-CHO coupling. The Cu site at the Cu(111) surface, two
interfacial sites (IF and IF′) of Cu@C nanobelts, and a single-atom (SA)
site of Cu@C nanobelts are considered. Color codes: O, red; H, white; C,
gray; Cu, orange (color online).
riers in the range of 0.3–0.4 eV, which are much lower than
the rating limiting barrier heights along the formate or
RWGS pathways towards the formation of CH (~1.5 eV)
4
*
CHO dissociation into *CO and *H were predicted for
[19,48]. Thus, the critical CHO-CHO coupling elementary
step in the proposed reaction mechanism for the formation of
Cu@C is likely viable.
Cu(111) and the IF site of Cu@C. The results readily show
that the CHO dissociation barrier is considerably higher for
the IF reaction than that for the Cu(111) reaction (0.39 eV vs.
Last, we need to address whether the CO hydrogenation at
2
0
.22 eV). In addition, the dissociation at the IF sites of
Cu@C exhibits a lower exothermicity (−0.33 eV vs.
0.66 eV). These predictions suggest that, in contrast to the
the low-coordinate Cu sites produces CH OH. The reaction
3
energy profile of the CO hydrogenation towards CH OH at
2
3
−
the IF site of Cu@C is given in Figure S8. Despite that the
reaction pathway is exothermic for all elementary steps, the
Cu(111) reaction, *CHO could be a reaction intermediate at
the IF sites of Cu@C which may lead to the key *(OHC-
CHO) species in our proposed mechanism, as well as the
further hydrogenation, in contrast to the pure Cu cases. The
comparatively high stability of *CHO on Cu@C is also
suggested by the predicted CHO binding energies, as given
in Table S3. The binding of CHO at the low-coordinate sites
of Cu@C is found to be much stronger than the binding of
CHO on Cu(111). The CHO binding is strongest at tshe IF
site (among the investigated sites), at which the binding
energies are evaluated to be 2.34 and 1.60 eV for *CHO and
reaction is most likely inhibited, as the *H CO intermediate,
2
which is required by both formate and RWGS pathways, is
not bound to Cu. We suggest that H CO can only be adsorbed
2
at multiple-Cu sites. Thus, even if H CO is produced at low-
2
coordinate Cu sites of Cu@C, they could migrate to the Cu
nanoparticle surface and become an intermediate for the
CH OH formation on the Cu nanoparticle surface, but such
3
contributions are expected to be small. Experimental results
show that CH OH is also significantly produced from the
3
catalytic reaction over Cu@C. From TEM images (Figure 1
(d)), we clearly see defined Cu(111) crystal facets of the
*
(CHO) , versus the values of 1.15 and 1.10 eV for the
2
corresponding species for Cu(111).
embedded Cu nanoparticles, which produces CH OH as the
3
To further show that the stabilized *CHO on Cu@C can
main product. The CH OH could result from the formate
3
lead to the formation of C products, we calculated the ac-
pathways at these Cu(111) sites.
2
tivation barriers for the CHO-CHO coupling reactions at IF
sites, IF' (a second interfacial site with different coordina-
tions from IF), and SA of the nanobelt structures (Figure 6).
It is shown that the CHO-CHO coupling reactions at the IF
and SA sites only require surmounting low activation bar-
4 Conclusions
We report a novel Cu-based catalyst, that is, Cu nanoparticles