G Model
JPC 9938 No. of Pages 6
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A. Fukatsu et al. / Journal of Photochemistry and Photobiology A: Chemistry xxx (2015) xxx–xxx
Fig. 5. Thin layer cyclic voltammograms (d = 0.25 mm) of Fe(tpp)Cl (1 mM) in a 0.1 M TBAP / DMF solution with photoirradiation in various light intensities (red,150 W; green,
300 W) and without photoirradiation (blue) under a CO2 atmosphere (WE: GC; CE: Pt wire; RE: Ag+/Ag, scan rate: 20 mV sꢀ1). (a) Voltammograms showing a catalytic current.
(b) Enlarged voltammograms focusing on Fe(III)/Fe(II) and Fe(II)/Fe(I) redox waves. (For interpretation of the references to color in this figure legend, the reader is referred to
the web version of this article.)
It should be noted that the intensity of the irreversible wave at
Epa = ꢀ1.7 V, which was observed in the measurements under dark
conditions, dramatically decreased in the voltammogram under
photoirradiation. These results clearly indicated that photo-
irradiation largely affected the redox properties of Fe(tpp)Cl
under a CO2 atmosphere.
To further understand this phenomenon, several electrochemi-
cal measurements were performed in thin-layer conditions under
a CO2 atmosphere. First, chronoamperometry was performed both
under photoirradiation and in the dark. The solution of Fe(tpp)Cl
(1 mM) in DMF containing TBAP (0.1 M) was electrolyzed at the GC
electrode with a cell operating potential of ꢀ2.3 V vs. Fc+/Fc while
keeping the layer thickness as 0.25 mm. As shown in Fig. 3,
constant currents flowed during the 300 s of electrolysis, and the
intensities of the currents were almost the same irrespective of the
photoirradiation. From these results, it was assumed that the
catalytic current of CO2 reduction catalyzed by Fe(tpp)Cl was not
affected by photoirradiation.
Second, the origin of the irreversible peak at approximately
ꢀ1.7 V under the dark conditions was investigated by changing the
negative edges of the potential sweep. Fig. 4 shows the voltammo-
grams of Fe(tpp)Cl for which the negative edges of the potential
sweep were ꢀ2.5 (blue line), ꢀ2.2 (green line) and ꢀ2.1 V (red line).
Although the shapes of the voltammograms were almost the same
when the measurements were performed under photoirradiation,
a clear difference was observed in the measurement under the dark
condition. For the negative edge located at ꢀ2.1 V, which was more
positive than the CO2 reduction potential catalyzed by Fe(tpp)Cl,
the second redox wave was reversibly observed. By shifting the
negative edges to the negative region, the irreversible peak at
ꢀ1.7 V gradually appeared, and the intensity of the peak at
Epa = ꢀ1.5 V decreased. These observations suggested that the flow
of the large catalytic current induced the generation of the
irreversible peak at ꢀ1.7 V.
peak around ꢀ1.7 V was presumed to be effectively suppressed by
photoirradiation.
The aforementioned observations enabled us to describe the
effect of photoirradiation on the redox properties of Fe(tpp)Cl in
combination with the proposed catalytic cycle. The proposed
reaction mechanism of electrocatalytic CO2 reduction by Fe(tpp)Cl
was reported by Costentin et al. [6] and is summarized in
Scheme 1. Initially, Fe(tpp)Cl is reduced from Fe(III) to Fe(0) by the
sequential one-electron reduction processes; these processes
were observed in the measurement under an Ar atmosphere
(vide supra). The generated Fe(0) species react with CO2, and the
CO2-bound complexes forms. Subsequent adduction of acid (in
this case, the hydrated water of the catalyst) and the CꢀꢀO bond
cleavage reaction in coordination with proton transfer result in
the formation of the CO-bound complex. Further reaction with the
Fe(0) species leads to the generation of CO. It was also reported
that CO generated by the catalytic reaction could bind to catalysts
with the Fe(I) state as the side reaction of the CO2 reduction
reaction by Fe(tpp)Cl (I in Scheme 1), and the electrochemical
response corresponding to this side reaction was observed at
approximately ꢀ1.7 V. Similarly, the irreversible peak, which was
attributed to the side reaction, was detected at ꢀ1.7 V in our
experiments using the TLCV technique in the dark condition.
Furthermore, we found that the intensity of the peak decreased
upon photoirradiation and, in some conditions, the electrochemi-
cal response of the side reaction could be suppressed.
A
reasonable explanation of this phenomenon is given by consider-
ing the photoinduced decarbonylation from carbonyliron tetra-
phenylporphyrin [7]. The oxidative Fe–CO reassociation
([FeI(tpp)]ꢀ + CO ! [FeII(tpp)CO] + eꢀ, I in Scheme 1) occurs at
E ꢁ ꢀ1.7 V regardless of photoirradiation. Under photoirradiated
condition, the photoinduced decarbonylation reaction of [FeII(tpp)
CO] proceeds to afford [FeII(tpp)] ([FeII(tpp)CO] + h
n
! [FeII(tpp)] +
CO) [7]. The photochemically generated [FeII(tpp)] is successively
Finally, the dependence of the generation of the irreversible
peak on the light intensity was investigated. Fig. 5 shows the cyclic
voltammogram of Fe(tpp)Cl under photoirradiation with different
intensities of light (150 and 300 W). When the light intensity was
increased, the peak height of the irreversible wave at ꢀ1.7 V
decreased, and the original re-oxidation wave at Epa = ꢀ1.5 V
increased. From these results, the generation of the irreversible
reduced ([FeII(tpp)]
+
eꢀ
!
[FeI(tpp)]ꢀ, E1/2 ꢁ ꢀ1.5 V, II in
Scheme 1). As a result, the current attributed to the oxidative
Fe–CO reassociation (I in Scheme 1) is offset by the current
attributed to the reduction of the photochemically generated
[FeII(tpp)] (II in Scheme 1). In total, the electrochemical response
of the side reaction in the catalytic system could be hindered by
photoirradiation.
Please cite this article in press as: A. Fukatsu, et al., Electrochemical analysis of iron-porphyrin-catalyzed CO2 reduction under photoirradiation,