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In This Article

  • Summary
  • Abstract
  • Introduction
  • Protocol
  • Representative Results
  • Discussion
  • Acknowledgements
  • Materials
  • References
  • Reprints and Permissions

Summary

We present a method for the determination of the energy relations of semiconductor/liquid junctions, which are the basis for the successful operation of such renewable solar energy converting systems.

Abstract

Operando Ambient Pressure X-ray photoelectron spectroscopy (operando AP-XPS) investigation of semiconductor/liquid junctions provides quantitative understanding of the energy bands in these photoelectrochemical solar cells. Liquid junction photoelectrochemical cells allow a uniform contact between the light-absorbing semiconductor and its contacting electrolyte phase. Standard Ultra High Vacuum (UHV) based X-ray photoelectron spectroscopy (XPS) has been used to analyze the electronic energy band relations in solid-state photovoltaics. We demonstrate how operando AP-XPS may be used to determine these relationships for semiconductor/liquid systems. The use of "tender" X-ray synchrotron radiation produces photoelectrons with enough energy to escape through a thin electrolyte overlayer; these photoelectrons provide information regarding the chemical and electronic nature of the top ~10 nm of the electrode as well as of the electrolyte. The data can be analyzed to determine the energy relationship between the electronic energy bands in the semiconductor electrode and the redox levels in the solution. These relationships are critical to the operation of the photoelectrochemical cell and for understanding such processes as photoelectrode corrosion or passivation. Through the approach described herein, the major conditions for semiconductor-electrolyte contacts including accumulation, depletion, and Fermi-level pinning are observed, and the so-called flat-band energy can be determined.

Introduction

Semiconductor/liquid junctions have long been investigated due to their simplicity of construction and economical possibility of fuel generation 1-4, with some such systems obtaining efficiencies over 17%.5 These systems operate based on the formation of a rectifying junction at the interface between the semiconductor electrode and the electrolyte. The energetics of semiconductor/liquid junctions are similar to those of a semiconductor/metal, Schottky, junction 3 where an electrolyte assumes the role of the metal. The semiconductor Fermi level, EF, is the electrochemical potential of the electron in the semiconductor and is ....

Protocol

1. Preparation of Semiconductor for Analysis

  1. Clean a p+, (100)-oriented boron doped Czochralski-grown Si wafer with a resistivity of ρ < 0.005 Ωcm. First soak for 2 min in a 3:1 (by volume) "piranha" solution of concentrated H2SO4 (98%) to 30% H2O2(aq).
  2. Etch for 10 s in a 10% (by volume) solution of HF(aq).
  3. Immediately after step 1.2, etch in a 5:1:1 (by volume) solution of H2O, 36% hydrochlo.......

Representative Results

Representative results are shown in Figures 6, 7, and 8. Figure 6 shows the collected O 1s and Ti 2p core level spectra for a TiO2 electrolyte in 1.0 M KOH solution, stacked with respect to the applied potential. Figure 7 shows the plotted core level water O 1s and Ti 2p peak positions, as collected from Figure 6 as well as from data in which a TiO2/Ni/electrolyte sample was investigated in the same electrolyte. Figure 8 shows a brief summary of our conclusions from .......

Discussion

The most critical steps in the technique for data collection are the application of voltage and the collection of the XPS data. The semiconductor preparation is necessarily crucial but can be generalized to any system where the semiconductor/liquid junction is stable enough to be investigated. However, for the choice of electrolyte, a number of experimental parameters must be considered. First, there must be sufficient interaction (hydrophilic or hydrophobic) between the solid electrode and the electrolyte in order to fo.......

Acknowledgements

This work was supported through the Office of Science of the U.S. Department of Energy (DOE) under award No. DE SC0004993 to the Joint Center for Artificial Photosynthesis, a DOE Energy Innovation Hub. The Advanced Light Source is supported by the Director, Office of Science, Office of Basic Energy Sciences, of the U.S. Department of Energy under Contract No. DE AC02 05CH11231. The authors thank Dr. Philip Ross for contributions to the conceptual development of the operando AP-XPS endstation and experimental design.

....

Materials

NameCompanyCatalog NumberComments
p+-Si(100)Addison3P-111Resistivity < 0.005 Ω - cm
H2SO4Sigma Aldrich339741 99.999%
H2O2Sigma Aldrich21676330%
HFSigma Aldrich33926199.99%
millipore H2OEMDMilliporeMilli-Q® Advantage A1018.2 MΩ
HClSigma Aldrich320331ACS Reagent, 37%
Tetrakis(dimethylamido)titanium(IV) (TDMAT)Sigma Aldrich469858 99.999%
N2PraxairNI 6.0 RS>99.9999%
Ni targetAJA International7440-02-0>99.99%
In/GaSigma Aldrich495425>99.99%
Hysol 9460Ellsworth Adhesives83128Dual cartridge
KOHSigma Aldrich306568Semiconductor grade, 99.99%
Liquid NitrogenPraxairNI 5.0
Gold foilSigma Aldrich32649699.99%
HNO3Sigma Aldrich438073ACS Reagent, 70%
1-sided copper tapeadafruit1128For electrode construction
glass microscope slidesVWR48300-025For electrode construction
Ag/AgCl reference electrodeeDaqET072-1
Platinum foilSigma Aldrich349348 99.99%
SP-300 Biologic PotentiostatBiologicSP-300
Scienta r4000 HiPP-2 Detector APPESScientaHiPP-2

References

  1. Walter, M. G., et al. Solar Water Splitting Cells. Chem. Rev. 110 (11), 6446-6473 (2010).
  2. Bard, A. J. Design of semiconductor photoelectrochemical systems for solar energy conversion. J. Phys. Chem. 86....

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