Defect-induced nonpolar-to-polar transition at the surface of CuInSe2

被引:21
作者
Jaffe, JE [1 ]
Zunger, A
机构
[1] Pacific NW Natl Lab, William R Wiley Environm Mol Sci Lab, Richland, WA 99352 USA
[2] Natl Renewable Energy Lab, Golden, CO 80401 USA
关键词
semiconductors;
D O I
10.1016/S0022-3697(03)00148-3
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
In contrast to zinc-blende semiconductors, where the nonpolar (110) surface has the lowest energy, our first-principles calculations on the chalcopyrite semiconductor CuInSe2 reveal that facets terminated by the (112)-cation and (112)-Se polar surfaces are lower in energy than the unfaceted (110) plane, despite the resulting increased surface area. This explains the hitherto puzzling existence of polar microfacets on nominally nonpolar (I 10) chalcopyrite surfaces. The extraordinary stability of these polar facets originates from the effective neutralization of surface charge by low-energy ordered Cu-In antisite or Cu vacancy surface defects, while the relaxed but defect-free (112) surface is metallic and much higher in energy. We explain the low carrier density of the observed faceted surface in terms of autocompensation between opposite-polarity facets. (C) 2003 Elsevier Ltd. All rights reserved.
引用
收藏
页码:1547 / 1552
页数:6
相关论文
共 27 条
[1]   1ST-PRINCIPLES ENERGY DENSITY AND ITS APPLICATIONS TO SELECTED POLAR SURFACES [J].
CHETTY, N ;
MARTIN, RM .
PHYSICAL REVIEW B, 1992, 45 (11) :6074-6088
[2]   DETERMINATION OF INTEGRALS AT SURFACES USING THE BULK CRYSTAL SYMMETRY [J].
CHETTY, N ;
MARTIN, RM .
PHYSICAL REVIEW B, 1991, 44 (11) :5568-5571
[3]   Texture manipulation of CuInSe2 thin films [J].
Contreras, MA ;
Egaas, B ;
King, D ;
Swartzlander, A ;
Dullweber, T .
THIN SOLID FILMS, 2000, 361 :167-171
[4]   HIGH-EFFICIENCY CUINXGA1-XSE2 SOLAR-CELLS MADE FROM (INX,GA1-X)2SE3 PRECURSOR FILMS [J].
GABOR, AM ;
TUTTLE, JR ;
ALBIN, DS ;
CONTRERAS, MA ;
NOUFI, R ;
HERMANN, AM .
APPLIED PHYSICS LETTERS, 1994, 65 (02) :198-200
[5]   Defect-induced nonpolar-to-polar transition at the surface of chalcopyrite semiconductors [J].
Jaffe, JE ;
Zunger, A .
PHYSICAL REVIEW B, 2001, 64 (24)
[6]   ELECTRONIC-STRUCTURE OF THE TERNARY CHALCOPYRITE SEMICONDUCTORS CUA1S2, CUGAS2, CUINS2, CUA1SE2, CUGASE2, AND CUINSE2 [J].
JAFFE, JE ;
ZUNGER, A .
PHYSICAL REVIEW B, 1983, 28 (10) :5822-5847
[7]   DETERMINANTS OF SURFACE ATOMIC GEOMETRY - THE CUCL(110) TEST CASE [J].
KAHN, A ;
AHSAN, S ;
CHEN, W ;
DUMAS, M ;
DUKE, CB ;
PATON, A .
PHYSICAL REVIEW LETTERS, 1992, 68 (21) :3200-3203
[8]   Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set [J].
Kresse, G ;
Furthmuller, J .
PHYSICAL REVIEW B, 1996, 54 (16) :11169-11186
[9]   ABINITIO MOLECULAR-DYNAMICS FOR LIQUID-METALS [J].
KRESSE, G ;
HAFNER, J .
PHYSICAL REVIEW B, 1993, 47 (01) :558-561
[10]   Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set [J].
Kresse, G ;
Furthmuller, J .
COMPUTATIONAL MATERIALS SCIENCE, 1996, 6 (01) :15-50