REVIEW ARTICLE

Recent advances in solar cells and photo-electrochemical water splitting by scanning electrochemical microscopy

  • Xiaofan ZHANG , 1,2 ,
  • Man LIU 1 ,
  • Weiqian KONG 1 ,
  • Hongbo FAN 2
Expand
  • 1. Henan Provincial Key Laboratory of Nanocomposite and Applications, Institute of Nanostructured Functional Materials, Huanghe Science and Technology College, Zhengzhou 450006, China
  • 2. School of Environment and Civil Engineering, Dongguan University of Technology, Dongguan 523808, China

Received date: 11 Jul 2018

Accepted date: 20 Sep 2018

Published date: 21 Dec 2018

Copyright

2018 Higher Education Press and Springer-Verlag GmbH Germany, part of Springer Nature

Abstract

Investigation on the mechanism and kinetics of charge transfer at semiconductor/electrolyte interface is significant for improving the photoelectric conversion efficiency and developing novel and high-efficiency photovoltaic devices. Scanning electrochemical microscopy (SECM), as a powerful analytical technique, has a potential advantage of high spatial and temporal resolution. It has been expanded into a broad range of research fields since the first inception of SECM in 1989 by Bard groups, which includes biological, enzymes, corrosion, energy conversion and storage (such as solar cells, hydrogen and battery). Herein, we review the basic principles and the development of SECM, and chiefly introduce the recent advances of SECM investigation in photoelectrochemical (PEC) cells including solar cells and PEC water splitting. These advances include rapid screening of photocatalysts/photoelectrodes, interfacial reaction kinetics and quantitation of reaction intermediates, which is significant for evaluating the performance, choosing catalysts and developing novel composite photoanodes and high efficiency devices. Finally, we briefly describe the development trends of SECM in energy research.

Cite this article

Xiaofan ZHANG , Man LIU , Weiqian KONG , Hongbo FAN . Recent advances in solar cells and photo-electrochemical water splitting by scanning electrochemical microscopy[J]. Frontiers of Optoelectronics, 2018 , 11(4) : 333 -347 . DOI: 10.1007/s12200-018-0852-7

Introduction

Developing of a long-term, sustainable energy economy is one of the most important technical issues facing humanity [1]. Solar energy is abundant (90 PW), inexhaustible and fairly well distributed over the planet [2]. Solar energy can be converted into usable energy via photoelectrochemical (PEC) cells which can be divided into two categories: regenerative solar cells and photosynthetic cells (e.g., hydrogen) [3]. Regenerative solar cells (e.g., dye-sensitized solar cells (DSSCs), perovskite solar cells (PSCs) and organic solar cells) can convert solar energy to electricity. Photosynthetic cells such as hydrogen can be obtained through PEC water splitting approach, which has been widely investigated since the first demonstration in 1972 by Fujishima and Honda [4]. For these devices, the semiconductor/electrolyte interface (SEI) investigation plays a vital role in improving charge carrier separation, transport and recombination pathways. Up to date, some in situ techniques have been developed to probe the dynamics of SEI reactions on the surface of electrodes or solar cells devices, such as photoelectrochemical impedance spectroscopy (PEIS) [57], intensity modulated photocurrent or photo-voltage spectroscopy (IMPS/IMVS) [8], transient absorption spectroscopy (TAS) [9,10], scanning-probe measurement (SPM) [11] and synchrotron-based X-ray techniques [12], and so on. Cen et al. reviewed the in situ techniques for PEC water splitting and summarized the advantages and limitations of these techniques [13]. Among them, SPM techniques, using a probe to scan the surface of samples, can provide the information of the interactions between the probe and the surface of samples, although they exhibit limited temporal resolution [14]. Thus the SPM techniques such as atomic force microscopy (AFM), scanning tunneling microscopy (STM) can be utilized to characterize different surface properties of the samples [1518]. And the most popular SPM techniques for in situ PEC studies are scanning photocurrent microscopy (SPCM) [19] and scanning electrochemical microscopy (SECM) [20]. Among them, SECM overcomes many typical problems, for example the effects of the resistive potential drop in solution (iR drop), and charging current. SECM is a “non-contact” scanning probe technique, which can provide chemical and/or topographic information about surfaces immersed in a solution. Therefore, SECM cannot only analyze the local chemical and PEC activity of sample surface, but also can be utilized to investigate the surface reaction intermediates and its kinetics as well as screen the active center. Hence, analytical measurements can be performed in the interfacial region. Besides, the researchers have also integrated SECM with alternating current (AC) impedance spectroscopy [21], atomic force microscopy (AFM) [22] and scanning ion-conductance microscope (SICM) [23] to investigate different properties.
In this review, we will describe the basic principle and the development of SECM, and chiefly introduce the recent advances in solar cells and PEC water splitting based on the different operation modes of SECM.

Basic principles of scanning electrochemical microscopy (SECM)

Instrument constitutes

SECM is based on these changes of the faradaic current when the SECM tip is moved across the surface of a sample, which is useful in obtaining topographic and surface reaction kinetic information. Figure 1 shows the typical structure of SECM equipment which includes six components (bipotentiostat, piezoelectric controller or positioning system, probe, electrolytic cell, substrate and computer). Among them, the bipotentiostat is used to precisely measure and control the current and potential of the probe and substrate (or the test samples). A high resolution three-dimensional positioning system is controlled by piezoelectric controller, which allows for accurate movement of the probe and sample using x, y, z stages. Another very important component is the probe or SECM tip (e.g., ultra-microelectrode (UME)), which can offer high mass transport rates, low ohmic effects, low double layer charging [24,25]. UME is optimal for many applications from kinetics measurements to electrochemical imaging. Furthermore, the electrolyte cell provides the reaction site, where the substrate is placed.
Fig.1 Simple schematic of a SECM instrument (WE: working electrode, RE: reference electrode, CE: counter electrode)

Full size|PPT slide

Working modes of scanning electrochemical microscopy (SECM)

SECM measurements can be performed using different working modes. After the first report on SECM in 1989 which introduced feedback and generation/collection (G/C) modes [26,27], a variety of new operation modes have been developed in order to expand its application, such as surface interrogation mode, ion transfer feedback mode, potentiometric detection mode, constant current mode, reverse imaging mode, redox competition mode and direct mode, and so on [28]. Among them, the feedback mode, G/C and surface interrogation (SI) modes are widely used in the fields of PEC cells to study the imaging and interfacial kinetics.

Feedback mode

SECM in feedback mode shows the great advantages in detecting active sites of the surface. In general, the SECM experiment is performed under four-electrode system, in which SECM tip usually serves as one of the dual working electrodes, and the substrate acts as the other one. These electrodes are all immersed in the solution containing redox mediators. The basic principle of the feedback mode is shown in Fig. 2. When the positive potential is applied to the SECM tip, the mediators will take place an oxidation reaction as the following Eq. (1),
R ne O.
Here, R and O represent a reduced and oxidized species in the solution, respectively. On the contrary, a reduction reaction will occur when the negative potential is applied. When the tip is far from the substrate, the steady-state current (iT,) can be given from Eq. (2),
i= T,4 nDFca β,
where n is the number of the electrons of electrode, F is the Faraday constant (96485 A·s·mol-1), D is the diffusion coefficient, c is the concentration of the reactant, a is the radius of the UME tip, and b is a geometric co-efficient [28]. When the tip is close to a conductive substrate or electrochemical active species substrate, the oxidized species formed in reaction (1) diffuse to the substrate and can be reduced back to R (Fig. 2(a)). In this condition, the flux of R to the tip is increased, and iT>iT,. This phenomenon is termed “positive feedback” (Fig. 2(c)). On the other hand, if the substrate surface is an insulator, the electron cannot recycle in the redox reaction (iT<iT,, Fig. 2(b)), that is to say, “negative feedback” appears (Fig. 2(d)). If a steady-state is established, the normalized current becomes independent of the ratio of diffusion coefficients and depends only on the tip/substrate distance (d). Moreover, larger iT is obtained when the d value is smaller. And the approach curve can be presented in form of iT/iT, vs. L (here L = d/a, and d is the distance between the tip and the substrate), which provides information on the kinetics of the process at the substrate.
Fig.2 Basic principle of the feedback mode

Full size|PPT slide

Generation/collection (G/C) mode

The generation/collection mode includes the substrate generation/tip collection (SG/TC) and tip generation/substrate collection (TG/SC) mode. In these modes, both SECM tip and substrate are working electrodes, and one generates some species which can be collected by the other [28]. In SG/TC mode, the electro-active species are generated at substrate and collected by SECM tip according to the following Eqs. (3) and (4),
R ne O substrate reaction ,
O + ne R tip reaction .
However, the reaction occurs in TG/SC mode is counter to SG/TC mode, as exhibited in Eqs. (5) and (6),
O + ne R substrate reaction ,
R ne O tip reaction .
Typically, SG/TC mode is used for the measurements of concentration profiles or chemical flux from a substrate. And the TG/SC mode is predominantly used to study reaction kinetics or perform modifications to the substrate.

Surface interrogation (SI) mode

The surface interrogation mode of scanning electrochemical microscopy (SI-SECM) is a new in situ electrochemical technique based on SECM operating in a transient feedback mode [29], which is developed by Bard and coworkers [28] and can be used to analyze, detect and quantify the adsorbed surface species on the electrode. The SI-SECM mode consists of a specific application of the feedback mode under transient conditions that allows for the quantification of finite amounts of reacting species on the surface of substrate. Different from the feedback mode, the reactive species (A) are absorbed at the substrate electrode in SI-SECM mode [28,30]. Figure 3 illustrates the schematic of the mechanism of the surface interrogation mode. First, the substrate is pulsed or scanned to a potential where oxidation occurs and an adsorbed species A is formed. At this time, the tip is kept at open circuit (OC), and the solution only contains the initial mediators in oxidized states (O) (Fig. 3(a)). Figure 3(b) shows the substrate is taken to OC and the tip is pulsed and reduces O to R. Then O can be regenerated via the diffused R reacting with adsorbed species A which is consumed and transferred to final product P. Ideally, regeneration of O should only be obtained through reaction with A. Figure 3(c) exhibits the final state of the system, which shows that all A is depleted and O reacts at the tip at the rate governed by the hindered diffusion into the tip-substrate gap. In summary, the SI mode acts as a transient feedback mode, in which a SECM tip is used to generate a titrant R which can react with A to regenerate O, producing positive feedback. Finally, a negative feedback can be detected as A is depleted from the surface.
Fig.3 Schematic diagram of mechanism for the surface interrogation (SI) mode [31,32] (OC is denoted as open circuit)

Full size|PPT slide

Based on these different operation modes, many excellent works have been carried out in various fields such as solar cells, water splitting and battery as listed in Table 1.
Tab.1 Application of SECM based on the above modes
applications measurement mode Refs.
dye-sensitized solar cells dye regeneration kinetics feedback mode [3335]
dye-sensitized solar cells imaging feedback and SG/TC mode [36]
perovskite solar cells kinetics feedback mode [37]
oxygen reduction reaction detect hydrogen peroxide TG/SC mode [38]
hydrogen evolution reaction kinetics SG/TC mode [39]
formic acid oxidation electrocatalytic activity TG/SC mode [40]
oxygen reduction reaction mechanism SG/TC mode [41]
Li-ion batteries Li-ion intercalation SG/TC mode [42,43]
supercapacitor charge transfer kinetics feedback mode [44]
corrosion localized corrosion TG/SC mode [45]
photoelectrochemical kinetics SI-SECM mode [46]
photocatalysis screening TG/SC mode [31,47]
electroreduction of CO2 CO2 reduction SG/TC mode [32]
hydrogen evolution reaction kinetics feedback mode [48]
decomposition of formic acid quantification of adsorbed hydrogen SI-SECM mode [49]

Application of scanning electrochemical microscopy (SECM)

Since the first introduction in the 1990s, SECM has been widely used to characterize hydrogen oxidation reaction (HER), oxygen evolution reaction (OER), and CO2 reduction via electrochemical or PEC technologies [5052]. As the hot topic, application of SECM in solar cells and PEC water splitting has attracted more attention for researchers described as follows.

Nanostructured solar cells

With the development of PEC technology, more and more new technology is applied to solve relevant scientific problem. Charge transfer process in solar cells is a field worthy of extensive study topic, which includes the regeneration process of the photosensitizers, photoelectric catalyst, and the transfer behavior of photo-generated electron and hole pairs at the interface of photoelectrode/electrolyte. These processes are the necessary steps for generating photocurrent, and paly an essential role in improving the photoelectric conversion efficiency of device. Due to the reaction occurring in the PEC interface is a fast charge transfer process, some conventional research methods cannot be able to monitor real time information under working condition. Attributed to the high time and spatial resolution, and sensitivity, SECM is very suitable to detect the trace change of electrochemical active material or chemical group located at the micro-region, which has been proven to be an effective method and plays unique role in studying the interfacial charge transfer kinetics of solar cells.

Dye-sensitized solar cells (DSSCs)

SECM acting as an elegant tool was used to directly determine the mobility of charge carriers and diffusion constant within dye-sensitized nanostructured semiconductors in 2006 [53]. Hence the PEC parameters including conductivity under illumination or heterogeneous kinetics could be obtained by means of SECM. In the field of DSSCs, SECM has been used to investigate the dye regeneration and charge transfer kinetics in the interface of dye/electrode. For example, Wittstock group developed a series of study on dye regeneration kinetics based on the feedback mode of SECM, and distinguished the luminous region using G/C mode, including D149 sensitized ZnO and N719 sensitized TiO2 solar cells [5456]. Similarly, Martin group investigated the charge transfer kinetics constants of N719 and N749 sensitized TiO2 solar cells using SECM [35]. Shen group from Huazhong University of Science and Technology has also developed much valuable research since the first collaboration with Wittstock group [57], in which the charge transfer kinetics between I- and Eosin Y+ dye adsorbed on ZnO was first investigated and demonstrated the viability of SECM for understanding DSSCs under working conditions. Later, they extended SECM to investigate the dye-regeneration process based on feedback mode [30,34,58], and dye regeneration process with different mediator concentrations and light intensities. First, they investigated the reaction kinetics of n-type dye sensitized solar cells and studied the influence of redox shuttles [Co(bpy)3]3+/[Co(bpy)3]2+, I3-/I- on the dye regeneration kinetics of C106TBA and LD14. This work interpreted the essential rule for the effects of PEC reaction kinetics on the n-type photovoltaic device properties [48]. Furthermore, they also investigated the reaction kinetics at the photo-cathode/electrolyte interface of p-type devices. They studied the influence of redox shuttles T2/T-, I3-/I- on the dye regeneration kinetics of P1 [59]. Both these works investigated the back transfer ability of the photo-generated electrons at photo-anode/electrolyte interface with different redox electrolyte, which was very helpful for assessing the interfacial recombination behavior of the photogenerated charges. Taking n-type TiO2 and p-type CuCrO2 for an example, Fig. 4 showed the basic principle of SECM and the reaction mechanism of different types DSSCs under short-circuit condition. The photoanodes (for example TiO2/C 106TBA and TiO2/LD 14) were placed in the presence of the oxidized species of redox couple and the photocathode (CuCrO2/P1) with reduced species of redox couple. As shown in Fig. 4(a), under illumination, dye generated hole/electron pairs after absorbed the incident light. Then the holes (D+/TiO2) reacted with redox species Co2+ regenerated dye (D/TiO2) accompanied by the production of Co3+ which could be detected by the UME. Finally, Co2+ species was regenerated by given potentials relative to Co2+/Co3+. Therefore, the SECM feedback approach curves can be obtained and fitted, which could relate the tip current to the surface’s heterogeneous electron or hole transfer kinetics and eventually obtained the normalized apparent charge-transfer constant (k). To determine the apparent standard hetero-generous rate constant k0, the effective rate constant (keff) values were plotted in Fig. 4(c) as a function of the corresponding over-potential (h, where h = EsubstrateEredox,solution1/2). For p-type (CuCrO2/P1) DSSCs, the mechanism was similar as illustrated in Fig. 4(b) and the apparent standard hetero-generous rate constant k0 also could be given from Fig. 4(c). It was observed that k0 for fluorine-doped tin oxide (FTO)/TiO2 was slower in electrolyte I3-/I- than that of Co3+/Co2+, and the hole transfer kinetics constant k0 for FTO/CuCrO2 in the case of T2/T- was slower than that of I3-/I-. Further comparison showed the recombination rate constant in p-type DSSCs was much higher than n-type devices, and the interfacial charge recombination kinetics constant were much smaller than the dye-regeneration kinetic constants. This ensures effective charge collection in the DSSC devices. These works may offer some new complementing aspects to establish methods for DSSCs.
Fig.4 Basic arrangement for probing the heterogeneous reaction at the (a) n-type dye-sensitized semiconductor (TiO2) and (b) p-type dye-sensitized semiconductor (CuCrO2) interface in the feedback mode of SECM under short-circuit conditions. The mediator couple is Co3+/Co2+ and T2/T, respectively (Ref: reference electrode, Aux: auxiliary electrode, WE-1: working electrode 1, WE-1: working electrode 2). Plot of ln(keff) vs. h for (a) FTO/TiO2 electrodes in acetonitrile corresponding to the reduction with I- and Co2+ and for (b) FTO/CuCrO2 electrodes in acetonitrile corresponding to the oxidation with T2 and I3[59]. Copyright © 2014, John Wiley and Sons

Full size|PPT slide

Quantum dots sensitized solar cells

Except for DSSCs, inorganic semiconductor quantum dots (QDs) have attracted more interest due to their unique optoelectronic properties derived from the quantum confinement effect. Many narrow band gap QDs (such as CdS, PbS/CdS, CdSe/CdTe and CuInS2) are suitable for sensitized solar cells (QDSSCs) because they can transfer electrons to large band gap semiconductors in order to further increase the charge separation and transfer efficiencies. Compared to DSSCs, the efficiency of QDSSCs is still very low. Up to now, the main factor restricting the improvement efficiency of QDSSCs is the hole-transfer process namely the regeneration process of QDs sensitizers which depends on the selection of redox electrolytes. Therefore, the investigation of the QDs regeneration process will be significant for improving the efficiency of such devices. Some novel technologies (such as nanosecond laser transient absorption spectroscopy (TAS)) have been used to measure the rate of quantum dots regeneration. In contrast to TAS, SECM is suitable to monitor the fast electron/hole transfer process in devices in working devices. So Shen group employed SECM to scrutinize the influence of redox couples (T2/T-, [Co(bpy)3]3+/[Co(bpy)3]2+, I3-/I-) on the quantum dots regeneration rate (CdSe and CdS) [33]. The measurement is also based on monitoring the feedback current, which is related to the small change in the concertation of the redox shuttle under the active area of UME probe caused by QDs regeneration. The results revealed that the kinetics of QDs regeneration depends on the nature of the QDs and the redox shuttles presented in QDSSCs. This work offers some new complementing aspects to establish the methods for QDSSCs characterization.

Perovskite solar cells

As the new star in the field of photovoltaic, perovskite solar cells, traced back to 2009 [60], has possessed a higher efficiency up to ~23%. However, one of the main restricting factors is the relative poor stability for the environment and optical which are directly related to the interface. To further increase the efficiency of PSCs, it is crucial to select of interface materials, increase the interfacial charge separation and transportation efficiency except for developing new materials and optimizing of preparation technology. Based on the advantage of SECM, Hsu et al. prepared a variety of PbI2/MAPbI3 perovskites and determined how excess PbI2 affects its PEC properties via a rapid screening technique using a modified SECM [61]. Subsequently, Wang group investigated the regeneration kinetics at perovskite/oxide interface with SECM [62]. However, the application of SECM in PSCs is only a few and still needs to be explored might due to the instability of PSCs in moist environment or solution.

Photoelectrochemical water splitting

To efficiently and sustainably split water via PEC technology, several key criteria must be met simultaneously. For instance, (1) the light absorption, the semiconductor should have an adequate band gap (1.8−2.2 eV) so as to absorb a significant portion of the solar spectrum especially the visible light [63,64], (2) the appropriate band edge potentials which must straddle the hydrogen and oxygen redox potentials, (3) efficient charge transfer and separation process, (4) long-term stability in the electrolyte solution and low cost and so on [65]. However, no single semiconductor satisfies all of the above requirements for practical hydrogen production. Therefore, various strategies have been developed in order to improve the PEC activity, such as doping [6668], constructing hetero-junction [6971], coupling with co-catalysts [72,73], surface modification [7477] as well as integrating with solar cells to forming tandem cells [7880]. Among the factors affecting the PEC performance, the light absorption depends on the band gap of semiconductor, which is its intrinsic property. The application of SECM in PEC water splitting mainly includes the SECM imaging, kinetics investigation and quantitation of reaction intermediates.

Screening of photocatalysts/photoelectrodes

As we all know, the solar to hydrogen efficiency (STH) of the photoelectrodes is still too low to practical application. Attributed to the varieties of photoelectrode materials, it is still a challenge to rapidly screen photocatalysts in order to economize the evaluation time and cost. Up to dates, many in situ technologies have been introduced into PEC field as described in Introduction section. Screening of catalysts for PEC application by SECM has drawn wide attention of many researchers.
Doping has been widely used to extend the light absorption and improve the conductivity of photo-electrodes. However, the essential relation between doping element or content and PEC activity is not investigated in detail. Previously, SECM was used to search for more efficient doped Fe2O3 photocatalysts which doped with different elements Sn, Ti, Be, Al [81]. For the screening of single dopants, the array pattern was prepared as shown in Figs. 5(a) and 5(b). Figure 5(c) shows a typical SECM image obtained from a photocatalyst spot array under visible light (l≥420 nm). The dark brown color (Red dotted box in Fig. 5(c)) implied a largest photocurrent which was obtained from 4% Sn-Fe2O3. Similarly, Fig. 5(d) shows the SECM image obtained from photocatalyst spot arrays consisting of Fe, Sn, and Be under visible light illumination. The highest photocurrent (130 nA) was observed at the composition of the 6% Be−4% Sn-Fe spot. The photocurrent then decreased gradually with further increase of the amount of Be. Lately, Bard group extended SECM to investigate PEC performance by screening various dopants for BiVO4 [82]. The results demonstrated the photocurrent of W or Mo doped BiVO4 was more than 10 times higher than undoped BiVO4.
Fig.5 Dispensed pattern of photocatalyst spot array with different mol % of Sn in Fe2O3 (a) and Be in 4% Sn-Fe2O3 (b). SECM image of (c) Sn doping Fe2O3 and (d) Be doping Sn-Fe2O3 measured with spot arrays at 0.2 V vs. Ag/AgCl in 0.2 mol NaOH under visible light irradiation (l≥420 nm) [81]. Copyright © 2009, American Chemical Society

Full size|PPT slide

Leonard et al. reported a rapid screening technique based on the SG/TC mode of a modified SECM to study how metal doping affects its PEC properties [83]. As shown in Fig. 6(a), the colors represented the photocurrent for sulfite oxidation at 0.2 V vs. Ag/AgCl in which browns represented higher currents and greens represented lower currents. From the SECM screening, we could see that a maximum photocurrent occurred at a 9% atomic ratio of Zn/W, which was consistent with the LSV results under chopped light (Fig. 6(b)). The results demonstrated SECM can act as a tool to choose the photoelectrodes with better PEC performance.
Fig.6 (a) SECM images for the typical photocurrent response of Zn/WO3 composites under full UV irradiation and with a 420 nm long-pass filter. (b) PEC response of electrodes with chopped light under full UV irradiation at 20 mV/s [83]. Copyright © 2013, American Chemical Society

Full size|PPT slide

Except for doping, coupling semiconductor (SC) with electro-catalyst is also a common method to improve photo-catalytic (PC) and PEC performance. However, we cannot randomly couple SC with an excellent electro-catalyst as co-catalyst to expect a higher PC or PEC performance. Ye et al. developed some co-catalysts (IrOx, Pt, Co3O4) dropped onto the W doped BiVO4 for PEC water oxidation, which was quickly identified the effect of co-catalysts on W doped BiVO4 by the optical fiber-SECM technique [84]. Fig. 7 shows the principle of SECM and the corresponding image results of the electrocatalyst Ir/Co oxides Co3O4 and Pt. The optical fiber-modified SECM technique was used to quickly identify the effect of various electrocatalysts for PEC water oxidation. The experimental results demonstrated Pt and Co3O4 were effective on BiVW-O films, while IrOx was not active, even though IrOx films showed the highest electrocatalytic activity for water oxidation as electrocatalyst. This work inspired us that the SECM method can be used to optimize electro-catalysts rapidly, e.g., by investigating different compositions with mixed electro-catalysts and by changing their thickness by dispensing blank solutions or with changing concentration of precursor solutions. Subsequently, Bard group also recently reported a new combinatorial methodology using a modified SECM technique for rapid preparation and screening of semiconductor photo-catalysts [85], which is analogous to the SECM for screening of other electro-catalysts.
Fig.7 (a) Operation principle of SECM and the corresponding image results of the electrocatalyst (b) Ir/Co oxide array, (c) photocurrent at Co3O4 spot, and (d) photocurrent at Pt spot [84]. Copyright © 2011, American Chemical Society

Full size|PPT slide

Overall, SECM technique is extremely useful in mapping of photoelectrode surface, which can provide valuable spatially resolved information on the process kinetics occurring at the SEI of a PEC system. However, the resolution achieved by this technique is limited by the dimension of the UME. New developments in electrode design will be able to improve the special resolution of this technique.

Investigation on the kinetics of charge transfer at semiconductor (SC)/electrolyte interface (SEI) with scanning electrochemical microscopy (SECM)

Fast charge transfer kinetics at the photoelectrode/electrolyte interface is critical for highly efficient PEC water splitting. SECM is a powerful approach for measuring the kinetics of heterogeneous electron transfer, which can be determined with high lateral resolution while scanning a tip parallel to the surface. Lu group described the electron transfer kinetics at interfaces using SECM in details [86]. Bard group performed surface-selective and time-dependent redox titrations to directly measure the surface OER kinetics of NiIV and FeIV in NiOOH, FeOOH, and Ni1−xFexOOH (0<x<0.27), which were popular co-catalyst used in PEC water system [87]. The results concluded that the remarkable OER activity of Ni1−xFexOOH arising from the fast OER kinetics on Fe sites in NiOOH with a rate constant of 1.7 s-1. Currently, we studied the interfacial charge transfer kinetics in PEC system by SECM based on its feedback mode as show in Fig. 8(a) [88]. For investigating the catalytic reaction kinetics (reaction 1 in Fig. 8(b)) of BiVO4 at the electrode/electrolyte interface, an extra Pt wire was ultrasonically welded on the substrate electrode FTO with ohmic contact (i.e., FTO/BiVO4 was named as photoanode) as indicated as connection style 1 in Fig. 8(a). Thus, the PEC cell was operated in short-circuit condition. SECM revealed the surface reaction kinetics constant of BiVO4 was 9.30´107 mol-1·cm3·s-1. And the ratio of rate constant for hole to electron for Mo:BiVO4 is ~30 times larger than that of BiVO4. The results reveal that the Mo element can significantly improve the transfer property of the photo-generated holes and suppress the transfer of photo-generated electrons at the photo-anode/electrolyte interface when doped into BiVO4. This study will provide new ideas for designing and choosing the materials with high performance, and allows us to make a comprehensive analysis of interfacial charge transfer kinetics in PEC system. Subsequently, SECM has also been used for recording the photo-induced charge transfer reactions at BiVO4 at chemically polarized liquid/liquid (L/L) interfaces [89].
Fig.8 (a) Basic principles for investigating of interfacial reaction kinetics in PEC water splitting under the feedback mode of SECM (Ref: reference electrode, Aux: auxiliary electrode, WE-1: working electrode 1, WE-1: working electrode 2). The semiconductor photocatalyst is BiVO4 and the redox probe is [Fe(CN)6]3/[Fe(CN)6]4 (named Fe3+/Fe2+). (b) Energy scheme of BiVO4 system on electrochemical and vacuum scale at pH 7.0. Reaction 1 is the catalytic reaction, and reaction 2 is back reaction at interface [88]. Copyright © 2016, American Chemical Society

Full size|PPT slide

Quantitation of reaction intermediates

Considering the complex process of water oxidation, quantitative of the reaction intermediates (such as H2O2, OH⋅) is very important which is useful for understanding the mechanism. Previously, Ahn and Bard investigated the surface cobalt sites and the intermediates of the electrocatalyst CoPi by surface interrogation scanning electrochemical microscopy (SI-SECM), in which CoPi was a universal co-catalyst for PEC water splitting [90]. Currently, SI-SECM was widely used to detect and quantify the intermediates of photoelectorde during PEC water splitting. For instance, Zigah et al. quantified adsorbed hydroxyl radical OH(ads) generated photoelectrochemically at the surface of a nanostructured TiO2 substrate electrode [91]. In this study, the geometry of the simulation space was depicted in Fig. 9(a) and it was adjusted for the experimental conditions, where a tip radius a = 50 m and RG = 3, and the substrate was modeled as an active subdomain of radius b = 150 m and depth d′ = 10 m. The interelectrode distance d was adjusted to 27 m. Fig. 9(b) described the mode of operation of SI-SECM for the generation and the detection of OH(ads) on the TiO2 substrate. Finally, the typical ⋅OH(ads) saturation coverage of 338 mC·cm-2 was found in nanostructured samples. The decay kinetics of ⋅OH(ads) by dimerization to produce H2O2 were studied through the time dependence of the SI-SECM signal and the surface dimerization rate constant was found to be ~ kOH = 2.2´103 mol-1·m2·s-1. Subsequently, this group investigated the reaction kinetics and surface coverage of water oxidation intermediates (H2O2) at the W/Mo-BiVO4 photoanode using SI-SECM [92]. Besides, Cho et al. studied the PEC water oxidation of doping BiVO4 and detected the oxygen evolution with using optical fiber incorporating a ring electrode via SECM [93].
Fig.9 (a) Description of the general SI-SECM simulation space and conditions. All geometries are in axial 2D and described by z and r were shown. Boundary types: i, insulation; ii, bulk concentration (semi-infinite); iii, flux at the tip; iv, concentration of hydroxyl radical OH at the substrate; v, insulation. (b) Description of the surface interrogation technique for the reduction of ⋅OH(ads) on TiO2. ① No ⋅OH(ads) on TiO2; ②⋅OH(ads) are generated on TiO2 through surface irradiation. ③ Light is turned off, interrogation of ⋅OH(ads) takes place by reduced species generated at the tip [91]. Copyright © 2012, Royal Society of Chemistry

Full size|PPT slide

As a promising narrow semiconductor, the PEC performance of Fe2O3 was mainly limited by slow water oxidation and severe recombination in the surface states. Therefore, in order to better understand the pathway of PEC reaction and further improve the PEC performance, it is essential to quantitative analyze of the reaction intermediates of the surface states. Krumov et al. used SI-SECM mode to quantitatively in situ probe the reactivity and coverage of reactive surface states in Fe2O3 during PEC water oxidation [94]. Besides, they also detected the evolution of H2O2 (1.0 mmol·m-2) during the decay process based on the SG/TC mode of SECM, which provided strong evidence for the existence of the ⋅OH(ads) intermediate on Fe2O3 and clearly showed a mechanism for the generation of unwanted products in PEC cells. This study demonstrated how SI-SECM enabled direct observation of multiple adsorbates and reaction pathways on operating photoelectrodes. Bard group also quantified the density of photoactive sites (Fe4+ species) on the surface of Fe2O3 based on the SI-SECM [95]. In addition, the PEC water oxidation reaction dynamic was elucidated by time-dependent redox titration experiment which was similar to Krumov et al. [94].

Conclusions

In summary, we elaborated and summarized the basic principle and application of SECM in PEC fields in recent years. Particularly, discussion is focused on the screening, kinetics and quantitation of reaction intermediates in solar cells and PEC water splitting based on the different modes of SECM. Attributed to its better sensitivity, spatial resolution and more accurate control of the position of the probe, the application of SECM is continuously expanded to various areas up to now. However, it still has some disadvantages such as its spatial resolution is not high enough. So SECM has more and more commonly combined with other instruments, such as AFM and SICM, surface plasma resonance, and so on. And thus it will continue to broaden the scope of the study, and will become a more important electrochemical technique in the future.

Acknowledgements

This work was supported by the National Natural Science Foundation of China (Grant No. 51602120), Natural Science Foundation of Education Department of Henan Province (No. 17A430023), and the opening project of Henan Provincial Key Laboratory of Nanocomposites and Applications (No. hkd20170106).
1
Holdren J P. Energy and sustainability. Science, 2007, 315(5813): 737

DOI PMID

2
Lianos P. Review of recent trends in photoelectrocatalytic conversion of solar energy to electricity and hydrogen. Applied Catalysis B: Environmental, 2017, 210: 235–254

DOI

3
Li D, Shi J, Li C. Transition-metal-based electrocatalysts as cocatalysts for photoelectrochemical water splitting: a mini review. Small, 2018, 14(23): 1704179

DOI PMID

4
Fujishima A, Honda K. Electrochemical photolysis of water at a semiconductor electrode. Nature, 1972, 238(5358): 37–38

DOI PMID

5
Klotz D, Grave D A, Dotan H, Rothschild A. Empirical analysis of the photoelectrochemical impedance response of hematite photoanodes for water photo-oxidation. Journal of Physical Chemistry Letters, 2018, 9(6): 1466–1472

DOI PMID

6
Wang M, Chen P, Humphry-Baker R, Zakeeruddin S M, Grätzel M. The influence of charge transport and recombination on the performance of dye-sensitized solar cells. ChemPhysChem, 2009, 10(1): 290–299

DOI PMID

7
Klotz D, Ellis D S, Dotan H, Rothschild A. Empirical in operando analysis of the charge carrier dynamics in hematite photoanodes by PEIS, IMPS and IMVS. Physical Chemistry Chemical Physics, 2016, 18(34): 23438–23457

DOI PMID

8
Tsyganok A, Klotz D, Malviya K D, Rothschild A, Grave D A. Different roles of Fe1−xNixOOH co-catalyst on hematite (a-Fe2O3) photoanodes with different dopants. ACS Catalysis, 2018, 8(4): 2754–2759

DOI

9
Berera R, van Grondelle R, Kennis J T. Ultrafast transient absorption spectroscopy: principles and application to photosynthetic systems. Photosynthesis Research, 2009, 101(2-3): 105–118

DOI PMID

10
Pei G X, Wijten J H J, Weckhuysen B M. Probing the dynamics of photogenerated holes in doped hematite photoanodes for solar water splitting using transient absorption spectroscopy. Physical Chemistry Chemical Physics, 2018, 20(15): 9806–9811

DOI PMID

11
Wang M, Alemu G, Shen Y. Scanning probe microscopy investigation of metal oxides nanocrystalline. In: Current Microscopy Contributions to Advances in Science and Technology, Chapter 3, 2012, 1377–1386

12
Esposito D V, Baxter J B, John J, Lewis N S, Moffat T P, Ogitsu T, O’Neil G D, Pham T A, Talin A A, Velazquez J M, Wood B C. Methods of photoelectrode characterization with high spatial and temporal resolution. Energy & Environmental Science, 2015, 8(10): 2863–2885

DOI

13
Cen J, Wu Q, Liu M, Orlov A. Developing new understanding of photoelectrochemical water splitting via in-situ techniques: a review on recent progress. Green Energy & Environment, 2017, 2(2): 100–111

DOI

14
Miki T, Yanagi H. Scanning probe microscopic characterization of surface-modified n-TiO2 single-crystal electrodes. Langmuir, 1998, 14(12): 3405–3410

DOI

15
Wierzbiński E, Szklarczyk M. Photoelectrochemical and in situ atomic force microscopy studies of films derived from o-methoxyaniline solution on gallium arsenide (100) photoelectrode. Thin Solid Films, 2003, 424(2): 191–200

DOI

16
Toma F M, Cooper J K, Kunzelmann V, McDowell M T, Yu J, Larson D M, Borys N J, Abelyan C, Beeman J W, Yu K M, Yang J, Chen L, Shaner M R, Spurgeon J, Houle F A, Persson K A, Sharp I D. Mechanistic insights into chemical and photochemical transformations of bismuth vanadate photoanodes. Nature Communications, 2016, 7: 12012

DOI PMID

17
Economou N J, Mubeen S, Buratto S K, McFarland E W. Investigation of arrays of photosynthetically active heterostructures using conductive probe atomic force microscopy. Nano Letters, 2014, 14(6): 3328–3334

DOI PMID

18
Nakamura R, Nakato Y. Primary intermediates of oxygen photoevolution reaction on TiO2 (Rutile) particles, revealed by in situ FTIR absorption and photoluminescence measurements. Journal of the American Chemical Society, 2004, 126(4): 1290–1298

DOI PMID

19
Zandi O, Hamann T W. Determination of photoelectrochemical water oxidation intermediates on haematite electrode surfaces using operando infrared spectroscopy. Nature Chemistry, 2016, 8(8): 778–783

DOI PMID

20
McKelvey K, Nadappuram B P, Actis P, Takahashi Y, Korchev Y E, Matsue T, Robinson C, Unwin P R. Fabrication, characterization, and functionalization of dual carbon electrodes as probes for scanning electrochemical microscopy (SECM). Analytical Chemistry, 2013, 85(15): 7519–7526

DOI PMID

21
Zampardi G, Klink S, Kuznetsov V, Erichsen T, Maljusch A, La Mantia F, Schuhmann W, Ventosa E. Combined AFM/SECM investigation of the solid electrolyte interphase in Li-ion batteries. Chemelectrochem, 2015, 2(10): 1607–1611

DOI

22
Takahashi Y, Shevchuk A I, Novak P, Murakami Y, Shiku H, Korchev Y E, Matsue T. Simultaneous noncontact topography and electrochemical imaging by SECM/SICM featuring ion current feedback regulation. Journal of the American Chemical Society, 2010, 132(29): 10118–10126

DOI PMID

23
Baranski A, Diakowski P. Application of AC impedance techniques to scanning electrochemical microscopy. Journal of Solid State Electrochemistry, 2004, 8(10): 683–692

DOI

24
Mirkin M, Fan F, Bard A. Scanning electrochemical microscopy part 13. Evaluation of the tip shapes of nanometer size microelectrodes. Journal of Electroanalytical Chemistry, 1992, 328(1-2): 47–62

DOI

25
Bard A, Fan F, Kwak J, Lev O. Scanning electrochemical microscopy: introduction and principles. Analytical Chemistry, 1989, 61(3): 132–138

26
Engstrom R, Pharr C. Scanning electrochemical microscopy. Analytical Chemistry, 1989, 61(19): 1099A–1104A

DOI

27
Polcari D, Dauphin-Ducharme P, Mauzeroll J. Scanning electrochemical microscopy: a comprehensive review of experimental parameters from 1989 to 2015. Chemical Reviews, 2016, 116(22): 13234–13278

DOI PMID

28
Rodriguez-López J, Alpuche-Aviles M A, Bard A J. Selective insulation with poly(tetrafluoroethylene) of substrate electrodes for electrochemical background reduction in scanning electrochemical microscopy. Analytical Chemistry, 2008, 80(5): 1813–1818

DOI PMID

29
Rodríguez-López J.Surface interrogation mode of scanning electrochemical microscopy (SI-SECM): an approach to the study of adsorption and (electro)catalysis at electrodes. Electroanalytical Chemistry: A Series of Advances, 2012, 24: 287–341

30
Zhang B, Xu X, Zhang X, Huang D, Li S, Zhang Y, Zhan F, Deng M, He Y, Chen W, Shen Y, Wang M. Investigation of dye regeneration kinetics in sensitized solar cells by scanning electrochemical microscopy. ChemPhysChem, 2014, 15(6): 1182–1189

DOI PMID

31
Weng Y, Hsiao K. Composition optimization of ZnO-based photocatalyst arrays by scanning electrochemical microscopy and the characterization of efficient photocatalysts. International Journal of Hydrogen Energy, 2015, 40(8): 3238–3248

DOI

32
Li F, Ciani I, Bertoncello P, Unwin P R, Zhao J J, Bradbury C R, Fermin D J. Scanning electrochemical microscopy of redox-mediated hydrogen evolution catalyzed by two-dimensional assemblies of palladium nanoparticles. Journal of Physical Chemistry C, 2008, 112(26): 9686–9694

DOI

33
Zhang B, Yuan H, Zhang X, Huang D, Li S, Wang M, Shen Y. Investigation of regeneration kinetics in quantum-dots-sensitized solar cells with scanning electrochemical microscopy. ACS Applied Materials & Interfaces, 2014, 6(23): 20913–20918

DOI PMID

34
Alemu G, Zhang B, Li J, Xu X, Cui J, Shen Y, Wang M. Investigation of dye-regeneration kinetics at dye-sensitized p-type CuCrO2 film/electrolytes interface with scanning electrochemical microscopy. Nano, 2014, 9(5): 1440008

35
Martin C, Bozic-Weber B, Constable E, Glatzel T, Housecroft C, Wright I. Development of scanning electrochemical microscopy (SECM) techniques for the optimization of dye sensitized solar cells. Electrochimica Acta, 2014, 119: 86–91

DOI

36
Schmidt I, Plettenberg I, Kimmich D, Ellis H, Witt J, Dosche C, Wittstock G. Spatially resolved analysis of screen printed photoanodes of dye-sensitized solar cells by scanning electrochemical microscopy. Electrochimica Acta, 2016, 222: 735–746

DOI

37
Shen Y, Träuble M, Wittstock G. Detection of hydrogen peroxide produced during electrochemical oxygen reduction using scanning electrochemical microscopy. Analytical Chemistry, 2008, 80(3): 750–759

DOI PMID

38
Li H, Du M, Mleczko M J, Koh A L, Nishi Y, Pop E, Bard A J, Zheng X. Kinetic study of hydrogen evolution reaction over strained MoS2 with sulfur vacancies using scanning electrochemical microscopy. Journal of the American Chemical Society, 2016, 138(15): 5123–5129

DOI PMID

39
Jung C, Sánchez-Sánchez C M, Lin C L, Rodríguez-López J, Bard A J. Electrocatalytic activity of Pd-Co bimetallic mixtures for formic acid oxidation studied by scanning electrochemical microscopy. Analytical Chemistry, 2009, 81(16): 7003–7008

DOI PMID

40
Sánchez-Sánchez C M, Rodríguez-López J, Bard A J. Scanning electrochemical microscopy. 60. Quantitative calibration of the SECM substrate generation/tip collection mode and its use for the study of the oxygen reduction mechanism. Analytical Chemistry, 2008, 80(9): 3254–3260

DOI PMID

41
Ventosa E, Schuhmann W. Scanning electrochemical microscopy of Li-ion batteries. Physical Chemistry Chemical Physics, 2015, 17(43): 28441–28450

DOI PMID

42
Xu F, Beak B, Jung C. In situ electrochemical studies for Li+ ions dissociation from the LiCoO2 electrode by the substrate-generation/tip-collection mode in SECM. Journal of Solid State Electrochemistry, 2012, 16(1): 305–311

DOI

43
Bülter H, Peters F, Schwenzel J, Wittstock G. Spatiotemporal changes of the solid electrolyte interphase in lithium-ion batteries detected by scanning electrochemical microscopy. Angewandte Chemie, 2014, 53(39): 10531–10535

DOI PMID

44
Sumboja A, Tefashe U, Wittstock G, Lee P S. Investigation of charge transfer kinetics of polyaniline supercapacitor electrodes by scanning electrochemical microscopy. Advanced Materials Interfaces, 2015, 2(1): 1400154

DOI

45
Zhang Q, Ye Z, Zhu Z, Liu X, Zhang J, Cao F. Separation and kinetic study of iron corrosion in acidic solution via a modified tip generation/substrate collection mode by SECM. Corrosion Science, 2018, 139: 403–409

DOI

46
Lee J, Ye H, Pan S, Bard A J. Screening of photocatalysts by scanning electrochemical microscopy. Analytical Chemistry, 2008, 80(19): 7445–7450

DOI PMID

47
Sreekanth N, Phani K L. Selective reduction of CO2 to formate through bicarbonate reduction on metal electrodes: new insights gained from SG/TC mode of SECM. Chemical Communications (Cambridge, England), 2014, 50(76): 11143–11146

DOI PMID

48
Rodríguez-López J, Bard A J. Scanning electrochemical microscopy: surface interrogation of adsorbed hydrogen and the open circuit catalytic decomposition of formic acid at platinum. Journal of the American Chemical Society, 2010, 132(14): 5121–5129

DOI PMID

49
Fernández J L, White J M, Sun Y, Tang W, Henkelman G, Bard A J. Characterization and theory of electrocatalysts based on scanning electrochemical microscopy screening methods. Langmuir, 2006, 22(25): 10426–10431

DOI PMID

50
Jantz D, Leonard K. Characterizing electrocatalysts with scanning electrochemical microscopy. Industrial & Engineering Chemistry Research, 2018, 57(22): 7431–7440

DOI

51
Li Y, Ning X, Ma Q, Qin D, Lu X. Recent advances in electrochemistry by scanning electrochemical microscopy. Trends in Analytical Chemistry, 2016, 80: 242–254

DOI

52
Rincón M E, Trujillo M E, Ávalos J, Casillas N. Photoelectrochemical processes at interfaces of nanostructured TiO2/carbon black composites studied by scanning photoelectrochemical microscopy. Journal of Solid State Electrochemistry, 2007, 11(9): 1287–1294

DOI

53
Bozic B, Figgemeier E. Scanning electrochemical microscopy under illumination: an elegant tool to directly determine the mobility of charge carriers within dye-sensitized nanostructured semiconductors. Chemical Communications (Cambridge, England), 2006, 21(21): 2268–2270

DOI PMID

54
Tefashe U M, Loewenstein T, Miura H, Schlettwein D, Wittstock G. Scanning electrochemical microscope studies of dye regeneration in indoline (D149)-sensitized ZnO photoelectrochemical cells. Journal of Electroanalytical Chemistry, 2010, 650(1): 24–30

DOI

55
Tefashe U M, Rudolph M, Miura H, Schlettwein D, Wittstock G. Photovoltaic characteristics and dye regeneration kinetics in D149-sensitized ZnO with varied dye loading and film thickness. Physical Chemistry Chemical Physics, 2012, 14(20): 7533–7542

DOI PMID

56
Tefashe U M, Nonomura K, Vlachopoulos N, Hagfeldt A, Wittstock G. Effect of cationon dye regeneration kinetics of N719-sensitized TiO2 films in acetonitrile-based and ionic-liquid-based electrolytes investigated by scanning electrochemical microscopy. Journal of Physical Chemistry C, 2012, 116(6): 4316–4323

DOI

57
Shen Y, Nonomura K, Schlettwein D, Zhao C, Wittstock G. Photoelectrochemical kinetics of eosin y-sensitized zinc oxide films investigated by scanning electrochemical microscopy. Chemistry (Weinheim an der Bergstrasse, Germany), 2006, 12(22): 5832–5839

DOI PMID

58
Shen Y, Tefashe U M, Nonomura K, Loewenstein T, Schlettwein D, Wittstock G. Photoelectrochemical kinetics of Eosin Y-sensitized zinc oxide films investigated by scanning electrochemical microscopy under illumination with different LED. Electrochimica Acta, 2009, 55(2): 458–464

DOI

59
Xu X, Zhang B, Cui J, Xiong D, Shen Y, Chen W, Sun L, Cheng Y, Wang M. Efficient p-type dye-sensitized solar cells based on disulfide/thiolate electrolytes. Nanoscale, 2013, 5(17): 7963–7969

DOI PMID

60
Kojima A, Teshima K, Shirai Y, Miyasaka T. Organometal halide perovskites as visible-light sensitizers for photovoltaic cells. Journal of the American Chemical Society, 2009, 131(17): 6050–6051

DOI PMID

61
Hsu H, Ji L, Du M, Zhao J, Yu E, Bard A. Optimization of PbI2/MAPbI3 perovskite composites by scanning electrochemical microscopy. Journal of Physical Chemistry C, 2016, 120(35): 19890–19895

DOI

62
Alemu G, Li J, Cui J, Xu X, Zhang B, Cao K, Shen Y, Cheng Y, Wang M. Investigation on regeneration kinetics at perovskite/oxide interface with scanning electrochemical microscopy. Journal of Materials Chemistry A, Materials for Energy and Sustainability, 2015, 3(17): 9216–9222

DOI

63
Jang J, Lee J, Ye H, Fan F, Bard A. Rapid screening of effective dopants for Fe2O3 photocatalysts with scanning electrochemical microscopy and investigation of their photoelectrochemical properties. Journal of Physical Chemistry C, 2009, 113(16): 6719–6724

DOI

64
Currao A. Photoelectrochemical water splitting. Chimia, 2007, 61(12): 815–819

DOI

65
Acar C, Dincer I, Zamfirescu C. A review on selected heterogeneous photocatalysts for hydrogen production. International Journal of Energy Research, 2014, 38(15): 1903–1920

DOI

66
Acar C, Dincer I. A review and evaluation of photoelectrode coating materials and methods for photoelectrochemical hydrogen production. International Journal of Hydrogen Energy, 2016, 41(19): 7950–7959

DOI

67
Shi Q, Murcia-López S, Tang P, Flox C, Morante J, Bian Z, Wang H, Andreu T. Role of tungsten doping on the surface states in BiVO4 photoanodes for water oxidation: tuning the electron trapping process. ACS Catalysis, 2018, 8(4): 3331–3342

DOI

68
Yang Y, Niu S, Han D, Liu T, Wang G, Li Y. Progress in developing metal oxide nanomaterials for photoelectrochemical water splitting. Advanced Energy Materials, 2017, 7(19): 1700555

DOI

69
Zhang X, Zhang B, Zuo Z, Wang M, Shen Y. N/Si co-doped oriented single crystalline rutile TiO2 nanorods for photoelectrochemical water splitting. Journal of Materials Chemistry A, Materials for Energy and Sustainability, 2015, 3(18): 10020–10025

DOI

70
Zhang X, Yang H, Zhang B, Shen Y, Wang M. BiOI-TiO2 nanocomposites for photoelectrochemical water splitting. Advanced Materials Interfaces, 2016, 3(1): 1500273

DOI

71
Harrison S, Hayne M. Photoelectrolysis using type-II semiconductor heterojunctions. Scientific Reports, 2017, 7(1): 11638

DOI PMID

72
Wang H, Zhang L, Chen Z, Hu J, Li S, Wang Z, Liu J, Wang X. Semiconductor heterojunction photocatalysts: design, construction, and photocatalytic performances. Chemical Society Reviews, 2014, 43(15): 5234–5244

DOI PMID

73
Yang J, Wang D, Han H, Li C. Roles of cocatalysts in photocatalysis and photoelectrocatalysis. Accounts of Chemical Research, 2013, 46(8): 1900–1909

DOI PMID

74
Zhang X, Zhang B, Liu S, Kang H, Kong W, Zhang S, Shen Y, Yang B. RGO modified Ni doped FeOOH for enhanced electrochemical and photoelectrochemical water oxidation. Applied Surface Science, 2018, 436: 974–980

DOI

75
Zhang X, Zhang B, Luo Y, Lv X, Shen Y. Phosphate modified N/Si co-doped rutile TiO2 nanorods for photoelectrochemical water oxidation. Applied Surface Science, 2017, 391: 288–294

DOI

76
Zhang X, Zhang B, Huang D, Yuan H, Wang M, Shen Y. TiO2 nanotubes modified with electrochemically reduced graphene oxide for photoelectrochemical water splitting. Carbon, 2014, 80: 591–598

DOI

77
Shi W, Zhang X, Brillet J, Huang D, Li M, Wang M, Shen Y. Significant enhancement of the photoelectrochemical activity of WO3 nanoflakes by carbon quantum dots decoration. Carbon, 2016, 105: 387–393

DOI

78
Shi W, Zhang X, Li S, Zhang B, Wang M, Shen Y. Carbon coated Cu2O nanowires for photoelectrochemical water splitting with enhanced activity. Applied Surface Science, 2015, 358: 404–411

DOI

79
Zhang X, Zhang B, Cao K, Brillet J, Chen J, Wang M, Shen Y. A perovskite solar cell-TiO2@BiVO4 photoelectrochemical system for direct solar water splitting. Journal of Materials Chemistry A, Materials for Energy and Sustainability, 2015, 3(43): 21630–21636

DOI

80
Chen Y S, Manser J S, Kamat P V. All solution-processed lead halide perovskite-BiVO4 tandem assembly for photolytic solar fuels production. Journal of the American Chemical Society, 2015, 137(2): 974–981

DOI PMID

81
Brillet J, Yum J, Cornuz M, Hisatomi T, Solarska R, Augustynski J, Grätzel M, Sivula K. Highly efficient water splitting by a dual-absorber tandem cell. Nature Photonics, 2012, 6(12): 824–828

DOI

82
Park H, Kweon K, Ye H, Paek E, Hwang G, Bard A. Factors in the metal doping of BiVO4 for improved photoelectrocatalytic activity as studied by scanning electrochemical microscopy and first-principles density-functional calculation. Journal of Physical Chemistry C, 2011, 115(36): 17870–17879

DOI

83
Leonard K, Nam K, Lee H, Kang S, Park H, Bard A. ZnWO4/WO3 composite for improving photoelectrochemical water oxidation. Journal of Physical Chemistry C, 2013, 117(31): 15901–15910

DOI

84
Ye H, Park H, Bard A. Screening of electrocatalysts for photoelectrochemical water oxidation on W-doped BiVO4 photocatalysts by scanning electrochemic al microscopy. Journal of Physical Chemistry C, 2011, 115(25): 12464–12470

DOI

85
Ye H, Lee J, Jang J, Bard A. Rapid screening of BiVO4-based photocatalysts by scanning electrochemical microscopy (SECM) and studies of their photoelectrochemical properties. Journal of Physical Chemistry C, 2010, 114(31): 13322–13328

DOI

86
Lu X, Hu Y, He H. Electron transfer kinetics at interfaces using secm (scanning electrochemical microscopy). In: Sur U K, ed. Recent Trend in Electrochemical Science and Technology. Rijeka: In Tech, 2012, 127–156

87
Ahn H S, Bard A J. Surface interrogation scanning electrochemical microscopy of Ni1−xFexOOH (0<x< 0.27) oxygen evolving catalyst: kinetics of the “fast” iron sites. Journal of the American Chemical Society, 2016, 138(1): 313–318

DOI PMID

88
Zhang B, Zhang X, Xiao X, Shen Y. Photoelectrochemical water splitting system--a study of interfacial charge transfer with scanning electrochemical microscopy. ACS Applied Materials & Interfaces, 2016, 8(3): 1606–1614

DOI PMID

89
Rastgar S, Wittstock G. Characterization of photoactivity of nanostructured BiVO4 at polarized liquid-liquid interfaces by scanning electrochemical microscopy. Journal of Physical Chemistry C, 2017, 121(46): 25941–25948

DOI

90
Ahn H S, Bard A J. Surface interrogation of CoPi water oxidation catalyst by scanning electrochemical microscopy. Journal of the American Chemical Society, 2015, 137(2): 612–615

DOI PMID

91
Zigah D, Rodríguez-López J, Bard A J. Quantification of photoelectrogenerated hydroxyl radical on TiO2 by surface interrogation scanning electrochemical microscopy. Physical Chemistry Chemical Physics, 2012, 14(37): 12764–12772

DOI PMID

92
Park H, Leonard K, Bard A. Surface interrogation scanning electrochemical microscopy (SI-SECM) of photoelectrochemistry at a W/Mo-BiVO4 semiconductor electrode: quantification of hydroxyl radicals during water oxidation. Journal of Physical Chemistry C, 2013, 117(23): 12093–12102

DOI

93
Cho S, Park H, Lee H, Nam K, Bard A. Metal doping of BiVO4 by composite electrodeposition with improved photoelectrochemical water oxidation. Journal of Physical Chemistry C, 2013, 117(44): 23048–23056

DOI

94
Krumov M R, Simpson B H, Counihan M J, Rodríguez-López J.In situ quantification of surface intermediates and correlation to discharge products on hematite photoanodes using a combined scanning electrochemical microscopy approach. Analytical Chemistry, 2018, 90(5): 3050–3057

DOI PMID

95
Kim J Y, Ahn H S, Bard A J. Surface interrogation scanning electrochemical microscopy for a photoelectrochemical reaction: water oxidation on a hematite surface. Analytical Chemistry, 2018, 90(5): 3045–3049

DOI PMID

Outlines

/