Takeo
Arai
ab,
Shunsuke
Sato
ab and
Takeshi
Morikawa
ab
aToyota Central R&D Labs., Inc., 41-1 Yokomichi, Nagakute, Aichi 480-1192, Japan. E-mail: takeo-arai@mosk.tytlabs.co.jp
bJST, ACT-C, 4-1-8 Honcho, Kawaguchi, Saitama 332-0012, Japan
First published on 27th May 2015
A solar to chemical energy conversion efficiency of 4.6% was demonstrated for CO2 photoreduction to formate utilizing water as an electron donor under simulated solar light irradiation to a monolithic tablet-shaped device. The simple CO2 photoreduction system was realized by exploiting the effect of the carbon substrate on selective CO2 reduction in the presence of oxygen and selective H2O oxidation over IrOx catalysts in the presence of formate.
In the present study, we demonstrate a simple CO2 photoreduction reaction that utilizes a monolithic tablet-shaped device. The device is composed of a porous ruthenium complex polymer (p-RuCP) as a CO2 reduction catalyst, iridium oxide (IrOx) as a water oxidation catalyst, and a triple-junction of amorphous silicon-germanium (SiGe-jn, Fig. S1, ESI†) as a light absorber. p-RuCP was developed by chemical polymerization of RuCP on a porous carbon substrate (see the ESI†) and connected to the stainless steel side (narrower bandgap side of the junction) of the SiGe-jn. An IrOx nanocolloid containing no organic substances was synthesized according to a previously reported method14 and coated on the indium tin oxide (ITO) surface of the SiGe-jn (see the ESI†). These components were functionally coupled to realize CO2 photoreduction with a high solar-to-chemical conversion efficiency in a single-compartment reactor. Two essential technologies were developed to realize the monolithic tablet-shaped device for CO2 photoreduction; selective CO2 reduction, even in the presence of H2O and O2, and selective H2O oxidation, even in the presence of organic substances. Without separation functions, such as in the photosynthesis of plants, the organic substances produced from CO2 in a liquid phase can be re-oxidized and competes with the H2O oxidation to O2 reaction. This is also the case for the other side reaction, in which H+ and O2 produced from H2O can be reduced and compete with the CO2 reduction reaction in a single compartment reactor. Both these reactions cancel the products generated at both sides; therefore, selective CO2 reduction and H2O oxidation are necessary for the artificial photosynthesis system to produce liquid chemicals from CO2 and H2O in a single-compartment reactor.
The first key technology is the selective CO2 photoreduction in aqueous media, which was established using the semiconductor–metal-complex hybrid system. We have previously reported the combination of a band-controlled semiconductor for visible-light excitation with a metal-complex to catalyze selective CO2 reduction, in which photoexcited electrons are transferred from the conduction band of the semiconductor to the lowest unoccupied molecular orbital (LUMO) of the metal-complex catalyst within tens of picoseconds, which resulted in highly selective CO2 photoreduction.15,16 Because the concept of the semiconductor–metal-complex hybrid catalyst is highly versatile, we have constructed the InP/RuCP photocathode catalyst for CO2 reduction.17
The CO2 reduction potential (ECR) of p-RuCP was estimated to be −0.18 V (vs. RHE) (Fig. S2 and Table S1, ESI†), which is substantially lower than that of metal electrodes. For example, the CO2 reduction potential for formate generation over an indium electrode was reported to be −0.90 V (vs. RHE).13 This is the advantage of using a metal-complex catalyst, but there still remain issues such as the competing reduction reaction of O2 evolved simultaneously over the water-oxidation site with the CO2 reduction reaction over InP/RuCP. O2 is more easily reduced than CO2 and the elimination of O2 is thus necessary for CO2 reduction using a metal complex catalyst.
As evidence, the current efficiency ηC, for formate formation over InP/RuCP in the presence of O2 is shown in Fig. 1A (see Table S2, ESI,† for details). The InP/RuCP photocathode was used as the working electrode in a three-electrode configuration. The Pt wire and a Hg/Hg2SO4 electrode were used as counter and reference electrodes, respectively. 0.1 M phosphate buffer was used as the electrolyte. Gaseous CO2 containing various concentrations of oxygen was continuously bubbled into the reactor during the reaction, and the CO2 photoreduction reaction was conducted at +0.21 V (vs. RHE) for 1 h. ηC was significantly decreased from 93% (at 0% O2) to 6% (at 7% O2) with an increase in the oxygen concentration due to selective O2 reduction (O2 → O2−) competing with CO2 reduction. Therefore, a system was developed to enhance the CO2 reduction selectivity over RuCP, even in the presence of O2. A porous carbon cloth (CC) sheet made of carbon fiber was applied, which possesses a low activity for hydrogen generation (Fig. S3, ESI†), and a surface area that is two orders of magnitude larger than that of the flat and smooth surface of a conventional semiconductor film. ηC for formate formation over RuCP coated onto CC (CC/p-RuCP) is also shown in Fig. 1A. CO2 photoreduction reaction was conducted at +1.41 V (vs. RHE). An ηC of 76% was observed, even in the presence of 7% O2. Comparison of the current–potential characteristics of CC under Ar and CO2 atmospheres suggested preferential adsorption of CO2 on the CC (Fig. S4, ESI†). It was thus assumed that gaseous CO2 in aqueous solution was concentrated adjacent to the CC on which RuCP was polymerized. When the RuCP was applied onto the surface of the stainless-steel side (lower bandgap side) of the SiGe-jn, where H2 generation is preferential (Fig. S3, ESI†), ηC for formate generation was only 0.3%, while it significantly improved to 94 ± 5% when using CC/p-RuCP (Table S3, ESI†).
The second key technology is highly selective H2O oxidation, even in the presence of formate. Photoreduction of CO2 to liquid organic products in a single-compartment cell is difficult because the products accumulated in the liquid phase can be re-oxidized to CO2 on the surface of water oxidation catalysts such as TiO2, as previously reported.11 Iridium oxide, an excellent catalyst for H2O oxidation,18 is reported to oxidize formic acid on Ti/IrO2 electrodes in perchloric acid.19 In the present study, formate was not decomposed in the oxidation reaction over the IrOx catalyst in a phosphate buffer solution. Fig. 1B shows the photodegradation of formate over the IrOx/SiGe-jn photoanode performed in 0.1 M phosphate buffer electrolyte containing ca. 27 μmol (ca. 1.4 mM) of formate with a three-electrode configuration at −0.25 V (vs. RHE). The bias voltage was set at the operation point of the present device estimated with a two-electrode configuration (details are provided later). Even though the total charge of 4 C observed during the photoanodic reaction over the IrOx/SiGe-jn photoanode was sufficient to decompose ca. 21 μmol formate (calculated value in Fig. 1B), the amount of formate decreased was negligible, which indicates that the IrOx catalyst has very low activity for the photodegradation of formate. It was also reported that the current efficiency for formate degradation over Ti/IrO2 in a perchloric acid electrolyte decreased from over 90% to less than 10%, according to the decrease in the concentration of formate from ca. 550 mM to ca. 30 mM, which indicates that the applied current exceeds the mass transport limit of formate.17 Therefore, it is supposed that the anodic photocurrent over the IrOx/SiGe-jn photoanode also exceeded the mass transport of formate on the surface of the IrOx catalyst and generated oxygen from water. The negligible photodegradation of formate over the IrOx/SiGe-jn photoanode was also observed in sulfate, borate and carbonate solutions (Fig. S5, ESI†).
SiGe-jn was selected as the semiconductor for photoexcitation, as employed in the previous report.20 SiGe-jn has an open circuit voltage (VOC) of 2.1 V, which is thermodynamically adequate to oxidize water and extract electrons (approximately 1.4 V), and the p–i–n and tunnel junctions in SiGe-jn facilitate the charge separation and transfer of photoexcited electrons and holes.21 The conduction band minimum (ECBM) of SiGe-jn was estimated to be −0.52 V (vs. RHE) from the current–potential characteristics (Fig. S6, ESI†). The ECBM of SiGe-jn is more negative than the ECR of −0.18 V (vs. RHE, see Fig. S2, ESI†) over p-RuCP; therefore, electron transfer from SiGe-jn in a photoexcited state to p-RuCP is thermodynamically possible. Furthermore, the valence band maximum (EVBM) of SiGe-jn was estimated to be 1.58 V (vs. RHE) by subtracting VOC from ECBM. The onset potential estimated from the current–potential curve for water oxidation (EWO) over IrOx was also estimated to be 1.5 V (vs. RHE) (Fig. S7, ESI†). Thus, the EVBM of SiGe-jn is also more positive than the EWO over IrOx, so that IrOx/SiGe-jn can facilitate H2O oxidation. The semiconductor–metal-complex hybrid system employs a technical advantage of the Ru-complex catalyst, i.e., a low potential required for CO2 reduction; therefore, the system using the SiGe-jn can demonstrate CO2 reduction to formate coupled with water oxidation reaction with a very low voltage of less than 2.1 V.
Based on these two key technologies, the IrOx/SiGe-jn/CC/p-RuCP monolithic tablet-shaped device was constructed. A schematic illustration of the device is shown in Fig. 2A. The CO2 photoreduction reaction was conducted by immersing the device in an aqueous phosphate buffer solution saturated with gaseous CO2 (pH 6.4) in a single-compartment reactor under irradiation with solar simulated light (1 sun, AM1.5, Fig. S8, ESI†). Formate as a liquid organic substance was generated from only CO2 and H2O raw materials using sunlight as an energy source. The time course for the generation of formate during the CO2 photoreduction reaction using the monolithic device with the best performance under simulated solar light irradiation (through a square-shaped slit of 0.25 cm2) is shown in Fig. 2B. Formate was generated continuously during irradiation for 6 h and the solar-to-chemical conversion efficiency was calculated to be 4.6% from the rate of formic acid generation (μmol HCOOH s−1) multiplied by the change in Gibbs free energy per mole of formic acid formation from CO2 and water (at 298 K, ΔG = 270 kJ mol−1) according to a previous report.22 This result is supported by the photocurrent observed at the operation point shown in the current–potential characteristics of the IrOx/SiGe-jn photoanode and the CC/p-RuCP cathode in the three-electrode configuration (Fig. S9, ESI†). A similar photocurrent was also observed at zero bias (vs. counter electrode) with the two-electrode configuration using the IrOx/SiGe-jn and CC/p-RuCP electrodes (Fig. S10, ESI†). The solar-to-chemical conversion efficiency for the present CO2 reduction is comparable to that observed for solar hydrogen production utilizing a similar light absorber20 and also reached a level comparable to the theoretical maximal photosynthetic energy conversion efficiency for C3 crops (e.g., rice and wheat), estimated to be 4.6%.23 This reaction was also confirmed to be reproducible. The mean value of the solar-to-chemical conversion efficiency utilizing three monolithic devices was 4.3%.
To verify a stoichiometric reaction, the quantity of oxygen molecules generated over IrOx/SiGe-jn/CC/p-RuCP during CO2 photoreduction was determined from in situ measurements. The experiment was conducted in a flow reactor equipped with a single-compartment Pyrex glass cell and a gas chromatograph. The IrOx/SiGe-jn/CC/p-RuCP monolithic device was immersed in 0.1 M phosphate buffer saturated with gaseous CO2 (flow rate 20 mL min−1). A solar simulator equipped with an AM1.5 filter was also used as the light source. The irradiation conditions were different from that used in Fig. 2B due to the experimental setup (see the ESI† for details). During light irradiation, oxygen bubbles were clearly observed at the IrOx surface. The total amount of oxygen generated after 2 h irradiation was 26.4 μmol (Fig. 3A), which corresponds to 105.6 μmol of photoexcited holes, while 50.2 μmol of formate in the liquid phase and 3.6 μmol of hydrogen in the gas phase were generated simultaneously after 2 h irradiation, which accounts for 107.6 μmol of photoexcited electrons. The amount of electrons was approximately equal to that of photoexcited holes, which strongly suggest that stoichiometric CO2 reduction is achieved using electrons extracted from water molecules. Furthermore, the ratio of the number of electrons consumed to generate formate to that for the total reduction products was 93%, which is in good agreement with the current efficiency for formate production observed in a half reaction over the SiGe-jn/CC/p-RuCP photocathode (Table S3, ESI†).
In addition, isotope tracer analysis was conducted using the IrOx/SiGe-jn/CC/p-RuCP device in 0.1 M phosphate buffer saturated with gaseous 13CO2 (flow rate 20 mL min−1) to avoid the possibility of experimental error warned by Mul and colleagues.22 Ion chromatography interfaced with time-of-flight mass spectrometry (IC-TOFMS) was used to clarify the formation of H13COO− (m/z = 46) (Fig. 3B, mass spectra are shown in Fig. S11, ESI†), which confirmed that the carbon source for formate was the CO2 molecules. Thus, formate was generated from only CO2, H2O and solar energy over the monolithic device.
Footnote |
† Electronic supplementary information (ESI) available: Experimental procedure, current–potential characteristics for various measurements, current efficiency for formate production and a simulated solar light spectrum. See DOI: 10.1039/c5ee01314c |
This journal is © The Royal Society of Chemistry 2015 |