Abstract

CuZnO (CZO) films have attracted increasing amounts of attention due to their promising potential applications in semiconductor devices. ZnO shows n-type conductivity, and attempts have been made to dope several elements in ZnO to improve the electrical properties. This study investigated the electrical property transitions of CZO films and determined the copper concentration at which the conductivity of CZO films will change from n-type to p-type. In this study, CZO films were fabricated by ultrasonic spray pyrolysis with copper acetate, zinc acetate, and ammonium acetate precursor solution. The concentrations of Cu ions in the CZO films were controlled by the concentration ratios of copper acetate to zinc acetate in the precursor solutions. In addition, these samples were analyzed by Hall effect measurements, X-ray diffraction, transmittance measurements, and photoluminescence measurements. The results show that the conductivity of the CZO film changes from n-type to p-type when the copper ion concentration in the film is 5%.

Highlights

  • Zinc oxide (ZnO) is a popular material because of its large band gap (3.4 eV) and large exciton binding energy (60 meV) [1,2]

  • It is important to know the properties of CuZnO thin films; this study investigated CZO thin films doped with different concentrations of Cu ranging from 0% to 6%

  • As the Cu content of the CZO thin films increases from 1% to 6%, the film band gap increases from 3.02 eV to 3.22 eV

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Summary

Introduction

Zinc oxide (ZnO) is a popular material because of its large band gap (3.4 eV) and large exciton binding energy (60 meV) [1,2] Due to their superior properties such as high crystalline quality, large aspect ratio, and quantum confinement effects [3,4], ZnO nanostructures have attracted great research interest. Different techniques such as molecular beam epitaxy, sputtering, sol-gel processing, vapor deposition, and electrochemical deposition have been employed to fabricate ZnO nanowires and nanorods, which have been widely used in laser devices, gas sensors, ultraviolet–visible light emission devices, and many other applications [5,6,7,8]. These samples were analyzed by Hall effect measurements, X-ray diffraction, transmittance measurements, and photoluminescence measurements

Morphological and Structural Properties
Transmission and Absorption
Raman Analysis
Photoluminescence
Experimental Section
Conclusions
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