首页> 外文期刊>ACS applied materials & interfaces >Band Alignment of the CdS/Cu2Zn(Sn1-xGex)Se-4 Heterointerface and Electronic Properties at the Cu2Zn(Sn1-xGex)Se-4 Surface: x=0, 0.2, and 0.4
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Band Alignment of the CdS/Cu2Zn(Sn1-xGex)Se-4 Heterointerface and Electronic Properties at the Cu2Zn(Sn1-xGex)Se-4 Surface: x=0, 0.2, and 0.4

机译:CdS / Cu2Zn(SN1-XGEx)SE-4的带对准CU-4(SN1-XGEX)SE-4表面上的外燃接近和电子性质:x = 0,0.2和0.4

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摘要

The surface electronic properties of the light absorber and band alignment at the p/n heterointerface are key issues for high-performance heterojunction solar cells. We investigated the band alignment of the heterointerface between cadmium sulfide (CdS) and Ge-incorporated Cu2ZnSnSe4 (CZTGSe), with Ge/(Ge + Sn) ratios (x) between 0 and 0.4, by X-ray photoelectron, ultraviolet, and inversed photoemission spectroscopies (XPS, UPS, and IPES, respectively). In particular, we used interface-induced band bending in order to determine the conduction band offset (CBO) and valence-band offset (VBO), which were calculated from the core-level shifts of each element in both the CdS overlayer and the CZTGSe bottom layer. Moreover, the surface electronic properties of CZTGSe were also investigated by laser-irradiated XPS. The CBO at the CdS/CZTGSe heterointerface decreased linearly, from +0.36 to +0.20 eV, as x was increased from 0 to 0.4; in contrast, the VBO at the CdS/CZTGSe heterointerface was independent of Ge content. Both UPS and IPES revealed that the Fermi level at the CZTGSe surface is located near the center of the band gap. The hole concentration at the CZTGSe surface was on the order of 10(11) cm(-3), which is much smaller than that of the bulk (similar to 10(16) cm(-3)). We discuss the differences in hole deficiencies near the surface and in the bulk on the basis of laser-irradiated XPS and conclude that hole deficiencies are due to defects distributed near the surface with densities that are lower than in the bulk, and the Fermi level is not pinned at the CZTGSe surface.
机译:光吸收器的表面电子特性和P / N异成面的带对准是高性能异质结太阳能电池的关键问题。我们研究了硫化镉(Cds)和Ge掺入的Cu2zNSNSE4(CZTGSE)之间的异肠面积的带对准,Ge /(Ge + sn)比率(x)在0和0.4之间,通过X射线光电电体,紫外线和反转PhotoEmission Spectroscips(XPS,UPS和IPE)分别为。特别地,我们使用了接口感应带弯曲以确定导电带偏移(CBO)和价带偏移(VBO),该偏移(VBO)是由CDS覆盖器和CZTSE中的每个元素的核心级移位计算的底层。此外,还通过激光辐照XPS研究了CZTGSE的表面电子性质。 CDS / CZTGSE异常接近的CBO线性下降,从+ 0.36到+ 0.20eV下降,因为x增加到0.4;相反,CDS / CZTGSE异常面的VBO与GE内容无关。 UPS和IPES都显示CZTGSE表面的费米水平位于带隙的中心附近。 CZTGSE表面的空穴浓度约为10(11)厘米(-3),其远小于体积(类似于10(16 )cm(-3))。我们在激光照射XPS的基础上讨论表面附近和体积差异的差异,并得出结论,孔缺陷是由于在表面附近分布的缺陷,密度低于散装,并且费米水平没有在CZTGSE表面上固定。

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  • 来源
    《ACS applied materials & interfaces》 |2019年第4期|共12页
  • 作者单位

    Natl Inst Adv Ind Sci &

    Technol Res Ctr Photovolta RCPV Cent 2 1-1-1 Umezono Tsukuba Ibaraki 3058568 Japan;

    Kagoshima Univ Grad Sch Sci &

    Engn 1-21-40 Korimoto Kagoshima 8900065 Japan;

    Kagoshima Univ Grad Sch Sci &

    Engn 1-21-40 Korimoto Kagoshima 8900065 Japan;

    Kagoshima Univ Grad Sch Sci &

    Engn 1-21-40 Korimoto Kagoshima 8900065 Japan;

    Kagoshima Univ Grad Sch Sci &

    Engn 1-21-40 Korimoto Kagoshima 8900065 Japan;

    Kagoshima Univ Grad Sch Sci &

    Engn 1-21-40 Korimoto Kagoshima 8900065 Japan;

    Natl Inst Adv Ind Sci &

    Technol Res Ctr Photovolta RCPV Cent 2 1-1-1 Umezono Tsukuba Ibaraki 3058568 Japan;

    Natl Inst Adv Ind Sci &

    Technol Res Ctr Photovolta RCPV Cent 2 1-1-1 Umezono Tsukuba Ibaraki 3058568 Japan;

    Natl Inst Adv Ind Sci &

    Technol Res Ctr Photovolta RCPV Cent 2 1-1-1 Umezono Tsukuba Ibaraki 3058568 Japan;

    Natl Inst Adv Ind Sci &

    Technol Res Ctr Photovolta RCPV Cent 2 1-1-1 Umezono Tsukuba Ibaraki 3058568 Japan;

    Natl Inst Adv Ind Sci &

    Technol Dept Energy &

    Environm E&

    E Cent 1 1-1-1 Umezono Tsukuba Ibaraki 3058568 Japan;

    Kagoshima Univ Grad Sch Sci &

    Engn 1-21-40 Korimoto Kagoshima 8900065 Japan;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 化学工业;
  • 关键词

    band alignment; CZTGS; IPES; UPS; XPS; kesterite; solar cell;

    机译:带对准;CZTGS;IPES;UPS;XPS;ketterite;太阳能电池;

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