Characterization of CuIn1-xGaxSe2 films prepared by spin-coating and co-reduction method
1
조회
0
다운로드
1
인용
0
참고문헌
키워드
초록
CuIn1-xGaxSe2 film has excellent photovoltaic performance due to its large optical absorption coefficient and direct-band gap. It was prepared by spin-coating and chemical co-reduction method which is a simple and easy way with low cost in this work. The surface morphology of the product film was observed using scanning electron microscope (SEM). The absorbance curvesare measured by visible spectrophotometer. The phases of the samples were characterized by X-ray diffraction (XRD). It wasfound by phase analysis that prolonging the reaction time and increasing the reaction temperature were beneficial to thesample crystallization. With the doping concentration increasing, the surface morphology of CuIn1-xGaxSe2 films changed witha tendency from spherical crystals to rods. The effect of doping concentration on the resistivity is not particularly obvious. Asthe doping concentration increases, the resistivity will increase slightly; When x=1, the resistivity changes greatly, which maybe due to the poor film continuity. Their estimated band gaps of CuIn1-xGaxSe2 films are 1.25 eV, 1.3 eV, 1.33 eV, 1.38 eV and1.4 eV respectively.
Abstract
CuIn1-xGaxSe2 film has excellent photovoltaic performance due to its large optical absorption coefficient and direct-band gap. It was prepared by spin-coating and chemical co-reduction method which is a simple and easy way with low cost in this work. The surface morphology of the product film was observed using scanning electron microscope (SEM). The absorbance curvesare measured by visible spectrophotometer. The phases of the samples were characterized by X-ray diffraction (XRD). It wasfound by phase analysis that prolonging the reaction time and increasing the reaction temperature were beneficial to thesample crystallization. With the doping concentration increasing, the surface morphology of CuIn1-xGaxSe2 films changed witha tendency from spherical crystals to rods. The effect of doping concentration on the resistivity is not particularly obvious. Asthe doping concentration increases, the resistivity will increase slightly; When x=1, the resistivity changes greatly, which maybe due to the poor film continuity. Their estimated band gaps of CuIn1-xGaxSe2 films are 1.25 eV, 1.3 eV, 1.33 eV, 1.38 eV and1.4 eV respectively.
참고문헌 (20)
- R. Bouferra, , Physica B, 565, pp.14~17 (2019)
- S. M. Chauhan, , Mat. Sci. Semicon. Proc, 74, pp.329~335 (2018)
- Young Ji Park, "Improved luminescence properties of Na2TiSiO5 phosphor by the Ge4+ doping in the crystal lattice", Journal of Ceramic Processing Research, 20(5), pp.460~463 (2019), 청정에너지연구소[DOI]
- Takumi Kato, "Dosimetric properties of Mg-doped Al2O3 transparent ceramics", Journal of Ceramic Processing Research, 20(5), pp.449~454 (2019), 청정에너지연구소[DOI]
- Hiroyuki Fukushima, "Scintillation and photoluminescence properties of Prdoped CaHfO3 crystals", Journal of Ceramic Processing Research, 20(3), pp.211~215 (2019), 청정에너지연구소[DOI]
- Tamal Tahsin Khan, "Enhanced thermoelectric properties of the SrTiO3 by Zr-doping with different doping level", Journal of Ceramic Processing Research, 19(4), pp.327~331 (2018), 청정에너지연구소[DOI]
- A. Aissata, , Energy Procedia, 18, pp.197~204 (2012)
- G. Yin, , Sol. Energy, 163, pp.443~452 (2018)
- Y. -S. Cheng, , Appl. Surf. Sci, 396, pp.631~636 (2017)
- C. -S. Chiou, , Sol. Energy, 146, pp.436~442 (2017)
- B. Noikaew, , Surf. Coat. Tech, 307, pp.547~553 (2016)
- Y. -F. Wu, , J. Lumin, 142, pp.81~85 (2013)
- M. Behr, , Thin Solid Films, 665, pp.36~45 (2018)
- S. Mandati, , Mater. Lett, 118, pp.158~160 (2014)
- H. T. Xue, , Mater. Lett, 164, pp.169~171 (2016)
- S. Sunkoju, , Thin Solid Films, 606, pp.113~119 (2016)
- A. Khanaki, , Mat. Sci. Semicon. Proc, 16, pp.1397~1404 (2013)
- A. B. Marai, , J. Alloy Compd, 658, pp.961~966 (2016)
- R. -W. You, , Mater. Res. Bull, 96, pp.183~187 (2017)
- K. G. Liu, , Results in Physics, 12, pp.766~770 (2019)
