期刊文献+

Synthesis, structure, optical, and electric properties of Ce-doped CuInTe_2 compound 被引量:1

Synthesis, structure, optical, and electric properties of Ce-doped CuInTe_2 compound
下载PDF
导出
摘要 Ce-doped Cu In Te2(CICT) semiconducting compounds are successfully synthesized. The phase structures, optical,and electric properties are investigated using powder X-ray diffraction(XRD), field emission scanning electron microscopy(FESEM), X-ray photoelectron spectrometer(XPS), Raman spectrometer, ultraviolet and visible spectrophotometer(UVVis), and a standard four-probe method. Cu In1-xCex Te2 crystallizes into a tetragonal structure with predominant orientation along the [112] direction. The lattice parameters are a = 6.190(6) A–6.193(0) A and c = 12.406(5) A–12.409(5) A. Ce prefers to occupy the 4b crystal position. According to the analysis of XPS spectra, Ce shows the mixture of valences 4+and 3+. Raman spectra reveal that the photon vibrating model in the CICT follows A1 mode in a wavenumber range of123 cm^-1–128 cm^-1. UV-Vis spectra show that the band gap Eg values before and after 0.1 mole Ce doped into Cu In Te2 are 1.28 e V and 1.16 e V, respectively. It might be due to the mixture of valences for Ce. Ce doped into Cu In Te2 still shows the semiconductor characteristics. Ce-doped Cu In Te2(CICT) semiconducting compounds are successfully synthesized. The phase structures, optical,and electric properties are investigated using powder X-ray diffraction(XRD), field emission scanning electron microscopy(FESEM), X-ray photoelectron spectrometer(XPS), Raman spectrometer, ultraviolet and visible spectrophotometer(UVVis), and a standard four-probe method. Cu In1-xCex Te2 crystallizes into a tetragonal structure with predominant orientation along the [112] direction. The lattice parameters are a = 6.190(6) A–6.193(0) A and c = 12.406(5) A–12.409(5) A. Ce prefers to occupy the 4b crystal position. According to the analysis of XPS spectra, Ce shows the mixture of valences 4+and 3+. Raman spectra reveal that the photon vibrating model in the CICT follows A1 mode in a wavenumber range of123 cm^-1–128 cm^-1. UV-Vis spectra show that the band gap Eg values before and after 0.1 mole Ce doped into Cu In Te2 are 1.28 e V and 1.16 e V, respectively. It might be due to the mixture of valences for Ce. Ce doped into Cu In Te2 still shows the semiconductor characteristics.
作者 付丽 郭永权
出处 《Chinese Physics B》 SCIE EI CAS CSCD 2014年第12期469-475,共7页 中国物理B(英文版)
基金 Project supported by the National Natural Science Foundation of China(Grant No.11274110)
关键词 CuIn1-xCexTe2 CHALCOPYRITE Raman spectrum band gap SEMICONDUCTOR CuIn1-xCexTe2 chalcopyrite Raman spectrum band gap semiconductor
  • 相关文献

参考文献29

  • 1Yassitepe E, Shafarman W N and Shah S 1 2014 J. Solid State Chem. 213 198.
  • 2Wu S M, Xue Y Z, Zhou L M, Liu X and Xu D Y 2014 Alloys Compd. 600 96.
  • 3Hsu H R, Hsu S C and Liu Y S 2012 Solar Energy 86 48.
  • 4Park S W, Kim D I, Lee T S, Lee K U, Yoon Y, Cho Y H, Kim J H, Alan K M, Lee K J and Jeon CW 2014 Solar Energy Materials and Solar Cells 125 66.
  • 5Lakhe M and Chaure N B 2014 Solar Energy Materials and Solar Cells 123 122.
  • 6Chen D S, Yang J, Xu F, Zhou P H, Du H W, Shi J W, Yu Z S and Zhang Y H 2013 Chin. Phys. B 22 018801.
  • 7Li W, Zhao Y M, Liu X J, Ao J P and Sun Y 2011 Chin. Phys. B 20 068102.
  • 8Jackson P, Hariskos D, Lotter E, Paetel S, Wuerz R, Menner R, Wis- chmann W and Powalla M 2011 Progress in Photovoltaics: Research and Applications 19 894.
  • 9Bodnar' I V, Gurin V S, Solove I N P and Molochko A P 2007 Semi- conductors 41 939.
  • 10Kim S, Kang M, Kim S, Heo J H, Noh J H, Im S H, Seok S I and Kim S W 2013 ACSNano 7 4756.

同被引文献2

引证文献1

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部