First-principles electronic structure and relative stability of pyrite and marcasite: Implications for photovoltaic performance

被引:135
作者
Sun, Ruoshi [1 ]
Chan, M. K. Y. [1 ,2 ]
Ceder, G. [1 ]
机构
[1] MIT, Dept Mat Sci & Engn, Cambridge, MA 02139 USA
[2] Argonne Natl Lab, Ctr Nanoscale Mat, Argonne, IL 60439 USA
基金
美国国家科学基金会;
关键词
DENSITY-FUNCTIONAL THEORY; INITIO MOLECULAR-DYNAMICS; TOTAL-ENERGY CALCULATIONS; IRON PYRITE; THIN-FILMS; BAND-GAP; FES2; TRANSITION; EFFICIENCY; GROWTH;
D O I
10.1103/PhysRevB.83.235311
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Despite the many advantages (e.g., suitable band gap, exceptional optical absorptivity, earth abundance) of pyrite as a photovoltaic material, its low open-circuit voltage (OCV) has remained the biggest challenge preventing its use in practical devices. Two of the most widely accepted reasons for the cause of the low OCV are (i) Fermi level pinning due to intrinsic surface states that appear as gap states, and (ii) the presence of the metastable polymorph, marcasite. In this paper, we investigate these claims, via density-functional theory, by examining the electronic structure, bulk, surface, and interfacial energies of pyrite and marcasite. Regardless of whether the Hubbard U correction is applied, the intrinsic {100} surface states are found to be of d(z)(2) character, as expected from ligand field theory. However, they are not gap states but rather located at the conduction-band edge. Thus, ligand field splitting at the symmetry-broken surface cannot be the sole cause of the low OCV. We also investigate epitaxial growth of marcasite on pyrite. Based on the surface, interfacial, and strain energies of pyrite and marcasite, we find from our model that only one layer of epitaxial growth of marcasite is thermodynamically favorable. Within all methods used (LDA, GGA-PBE, GGA-PBE+U, GGA-AM05, GGA-AM05+U, HSE06, and Delta-sol), the marcasite band gap is not less than the pyrite band gap, and is even larger than the experimental marcasite gap. Moreover, gap states are not observed at the pyrite-marcasite interface. We conclude that intrinsic surface states or the presence of marcasite are unlikely to undermine the photovoltaic performance of pyrite.
引用
收藏
页数:12
相关论文
共 58 条
[1]   Computational Investigation of FeS2 Surfaces and Prediction of Effects of Sulfur Environment on Stabilities [J].
Alfonso, Dominic R. .
JOURNAL OF PHYSICAL CHEMISTRY C, 2010, 114 (19) :8971-8980
[2]   First-principles calculations of the electronic structure and spectra of strongly correlated systems: The LDA+U method [J].
Anisimov, VI ;
Aryasetiawan, F ;
Lichtenstein, AI .
JOURNAL OF PHYSICS-CONDENSED MATTER, 1997, 9 (04) :767-808
[3]  
[Anonymous], ELECTROCHIM ACTA
[4]   Functional designed to include surface effects in self-consistent density functional theory [J].
Armiento, R ;
Mattsson, AE .
PHYSICAL REVIEW B, 2005, 72 (08)
[5]   SULFUR DEFICIENCY IN IRON PYRITE (FES2-X) AND ITS CONSEQUENCES FOR BAND-STRUCTURE MODELS [J].
BIRKHOLZ, M ;
FIECHTER, S ;
HARTMANN, A ;
TRIBUTSCH, H .
PHYSICAL REVIEW B, 1991, 43 (14) :11926-11936
[6]   IMPROVED TETRAHEDRON METHOD FOR BRILLOUIN-ZONE INTEGRATIONS [J].
BLOCHL, PE ;
JEPSEN, O ;
ANDERSEN, OK .
PHYSICAL REVIEW B, 1994, 49 (23) :16223-16233
[7]  
BROCK KJ, 1978, AM MINERAL, V63, P210
[8]   SURFACE PREPARATION OF FES2 VIA ELECTROCHEMICAL ETCHING AND INTERFACE FORMATION WITH METALS [J].
BRONOLD, M ;
BUKER, K ;
KUBALA, S ;
PETTENKOFER, C ;
TRIBUTSCH, H .
PHYSICA STATUS SOLIDI A-APPLIED RESEARCH, 1993, 135 (01) :231-243
[9]   SURFACE-STATES ON CUBIC D-BAND SEMICONDUCTOR PYRITE (FES(2)) [J].
BRONOLD, M ;
TOMM, Y ;
JAEGERMANN, W .
SURFACE SCIENCE, 1994, 314 (03) :L931-L936
[10]   SURFACE PHOTOVOLTAGE MEASUREMENTS ON PYRITE(100) CLEAVAGE PLANES - EVIDENCE FOR ELECTRONIC BULK DEFECTS [J].
BRONOLD, M ;
PETTENKOFER, C ;
JAEGERMANN, W .
JOURNAL OF APPLIED PHYSICS, 1994, 76 (10) :5800-5808