Article
Figure 6. XPS spectra of Ni 2p (a) and Fe 2p (b) regions in different catalysts.
assuming that the metal sites in Ni Fe @COF-SO are active
times improvement. This strongly proves that the remarkably
x
1−x
3
(
Figure 5e). Remarkably, the TOF value of Ni Fe @COF-
enhanced OER activity in bimetallic COF (Ni Fe @COF-
0
.5 0.5
0.5 0.5
−
1
SO reaches 0.1442 s , which is about 17.59-, 103-, 17.59-,
SO ) relative to monometallic COF (Fe@COF-SO ) is
3
3
3
4
.29-, and 9.74-fold higher than those in Ni@COF-SO
attributed to not only the increased ECSA, but probably also
the strong electronic effect between Ni and Fe sites, which
would result in the increased intrinsic catalytic activity.
Taking into account that the durability of electrocatalysts is
3
−
1
−1
(
0.0082 s ), Fe@COF-SO (0.0014 s ), Ni Fe @COF-
3
0.2 0.8
−1
−
1
−
SO (0.0082 s ), Ni Fe @COF-SO (0.0336 s ), and
3
0.8 0.2
3
−
1
commercial IrO2 (0.0148 s ), respectively, exhibiting a
significant bimetallic synergistic effect. Based on the activity
metric mentioned above (e.g., overpotential, Tafel slope, mass
activity, and TOF), it can be reasonably concluded that
bimetallic COFs possess better OER activity relative to
monometallic COFs, and Ni Fe @COF-SO is the best
one among Ni Fe @COF-SO (x = 0, 0.2, 0.5, 0.8, 1.0)
electrodes and even superior to the commercial IrO2
benchmark.
22a
of crucial importance for practical applications, the long-
term stability of Ni Fe @COF-SO was evaluated by a
0
.5 0.5
3
chronoamperometric (i−t) measurement at different poten-
tials. Impressively, Ni Fe @COF-SO can maintain the
0
.5 0.5
3
−
2
current densities of 20, 50, and 100 mA cm at three
different applied potentials (Figure 5i), respectively, exhibiting
excellent stability. Besides, the PXRD pattern demonstrates
that Ni Fe @COF-SO after chronoamperometric measure-
0.5 0.5
3
x
1−x
3
0
.5 0.5
3
To determine the reason for the enhanced OER activity in
bimetallic COFs, the possible factors that may affect the
performance were carefully explored. First, electrochemical
impedance spectra (EIS) of different samples were measured.
As revealed by Nyquist plots (Figure 5f), the semicircle
diameter of Ni Fe @COF-SO is smaller than those of other
ment still can keep its initial crystalline structure without the
S10 and S11). The nanofiber network structure of Ni Fe @
0
.5 0.5
COF-SO and the uniform distribution of different elements in
3
the binding energies of Ni 2p and Fe 2p in Ni Fe @COF-
0
.5 0.5
3
samples, proving more highly efficient electron transport at the
0
.5 0.5
1
9
electrolyte−electrode interface, which will promote the
electrocatalytic OER process. Second, the electrochemical
active surface area (ECSA) is determined based on the double-
SO after OER stability tests shift to higher values compared to
3
those in fresh Ni Fe @COF-SO , which should be due to
0
.5 0.5
3
22b
layer capacitance (C ) estimated by the simple cyclic
dl
2
0
voltammogram (CV) method.
Clearly, the Cdl in
X-ray photoelectron spectroscopy (XPS) characterization
was carried out to disclose the electronic interaction between
−
2
Ni Fe @COF-SO (0.237 mF cm ) is higher than those
0
.5 0.5
3
−
2
23
in Ni Fe @COF-SO (0.163 mF cm ), Ni Fe @COF-
Ni and Fe sites on OER activity. In the case of NiFe-based
0
.8 0.2
3
0.2 0.8
−2
−
−2
SO3 (0.103 mF cm ), Ni@COF-SO (0.084 mF cm ), and
bimetallic electrocatalysts, Ni is generally regarded as the
3
−
−2
24
Fe@COF-SO3 (0.077 mF cm ) (Figure 5g). The best OER
activity in Ni Fe @COF-SO may be related to the largest
mainly active sites for the OER, while the incorporation of Fe
can modulate the electronic state of Ni, leading to the shift of
Ni 2p binding energy to a higher value and thus enhancing the
0
.5 0.5
3
ECSA. CV curves measured in the non-Faradaic potential
are presented in Figure S9. Moreover, the relationship of
current density at the overpotential of 400 mV with ECSA in
different COFs was also investigated. As shown in Figure 5h,
the samples possessing larger ECSA exhibit higher current
density, further confirming that the ECSA of catalysts is
actually a vital contributor for improving the OER perform-
25
OER performance. From the Ni 2p spectra (Figure 6a), it
can be seen that these COFs present two typical peaks at about
856 and 874 eV, which are assigned to Ni 2p and Ni 2p1/2
3
/2
26
electronic configurations, respectively. Obviously, the bind-
ing energy of Ni 2p in bimetallic COFs is higher than that of
monometallic COF (Ni@COF-SO ) while the binding energy
3
of Fe 2p in bimetallic COFs transfers to a lower value
compared to that in Fe@COF-SO3 (Figure 6b), which
indicates that incorporating Fe can change the coordination
environment of Ni species and thus promote the formation of
strong Ni−Fe electronic interactions. Among the bimetallic
COFs, Ni Fe @COF-SO shows the highest Ni 2p binding
2
1
ance. However, after investigating this result carefully, we can
find that the ECSA has more than a 3-fold increase from 0.154
−
2
−2
mF cm in Fe@COF-SO to 0.474 mF cm in Ni Fe @
3
0.5 0.5
COF-SO , while the corresponding current density increases
3
from 4.66 to 48.66 mA, showing significantly an almost 11
0
.5 0.5
3
F
Inorg. Chem. XXXX, XXX, XXX−XXX