4.7 Article

Evidence and Influence of Copper Vacancies in p-Type CuGaO2 Mesoporous Films

Journal

ACS APPLIED ENERGY MATERIALS
Volume 2, Issue 1, Pages 19-28

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsaem.8b01558

Keywords

CuGaO2; delafossite; p-type metal oxide; hole transport; heterojunction solar cell

Funding

  1. EPSCoR [1809847]
  2. National Science Foundation, Division of Materials Research
  3. Department of Chemistry and Biochemistry at Auburn University
  4. Department of Physics at Auburn University
  5. Direct For Mathematical & Physical Scien
  6. Division Of Materials Research [1809847] Funding Source: National Science Foundation

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Delafossite CuGaO2 nanocrystals were hydrothermally synthesized and characterized spectroscopically and electrochemically as mesoporous thin films. The nanocrystals demonstrate a preferred orientation within the film structure, as shown by enhancement of the (001) peaks via two-dimensional powder X-ray diffraction. Annealing conditions of low and high temperature (i.e., 100-300 degrees C), with oxygen and/or argon atmospheres, were investigated, and the resulting effect on the thin film electrochemistry was measured. Cyclic voltammetry showed an increase in non-faradaic current with higher annealing temperatures and demonstrated a quasi-reversible redox feature (E-1/2 = 0.1 V vs Fc(+1/0)). This feature is assigned to a Cu-II/Cu-I redox couple associated with surface defects. X-ray photoelectron and energy dispersive spectroscopies provide evidence for Cu-II surface defects and copper vacancies. Electrochemical impedance spectroscopy revealed that CuGaO2 films were highly conductive with sigma similar to 10(-5) Omega cm(-1), consistent with a large density of hole carriers induced by copper vacancies. The significance of synthesis, film preparation, and annealing conditions on the presence of surface defects and large hole densities is discussed. The prevalence of such defects in delafossite CuGaO2 is expected to have a large impact on the use of this material as a hole transport layer in solar cell architectures.

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