Nature of the band gap of halide perovskites ABX 3 (A = CH 3 NH 3 , Cs; B = Sn, Pb; X = Cl, Br, I): First-principles calculations

The electronic structures of cubic structure of ABX3(A=CH3NH3, Cs; B=Sn, Pb; X=Cl, Br, I) are analyzed by density functional theory using the Perdew–Burke–Ernzerhof exchange–correlation functional and using the Heyd–Scuseria–Ernzerhof hybrid functional. The valence band maximum (VBM) is found to be made up by an antibonding hybridization of B s and X p states, whereas bands made up by the π antibonding of B p and X p states dominates the conduction band minimum (CBM). The changes of VBM, CBM, and band gap with ion B and X are then systematically summarized. The natural band offsets of ABX3 are partly given. We also found for all the ABX3 perovskite materials in this study, the bandgap increases with an increasing lattice parameter. This phenomenon has good consistency with the experimental results.

[1]  Kiyoyuki Terakura,et al.  Charge-transport in tin-iodide perovskite CH3NH3SnI3: origin of high conductivity. , 2011, Dalton transactions.

[2]  R. Vaglio,et al.  Combined experimental and theoretical investigation of optical, structural and electronic properties of CH3NH3SnX3 thin films (X=Cl,Br) , 2008 .

[3]  Kresse,et al.  Efficient iterative schemes for ab initio total-energy calculations using a plane-wave basis set. , 1996, Physical review. B, Condensed matter.

[4]  Iftikhar Ahmad,et al.  First principle study of the structural and optoelectronic properties of cubic perovskites CsPbM3 (M¼Cl, Br, I) , 2011 .

[5]  Burke,et al.  Generalized Gradient Approximation Made Simple. , 1996, Physical review letters.

[6]  Yanhong Luo,et al.  Enhanced Performance in Perovskite Organic Lead Iodide Heterojunction Solar Cells with Metal-Insulator-Semiconductor Back Contact , 2013 .

[7]  H. Snaith Perovskites: The Emergence of a New Era for Low-Cost, High-Efficiency Solar Cells , 2013 .

[8]  Gustavo E. Scuseria,et al.  Erratum: “Hybrid functionals based on a screened Coulomb potential” [J. Chem. Phys. 118, 8207 (2003)] , 2006 .

[9]  Yoshihiro Furukawa,et al.  Phase Transition and Electric Conductivity of ASnCl3 (A = Cs and CH3NH3). , 1998 .

[10]  Mohammad Khaja Nazeeruddin,et al.  Organohalide lead perovskites for photovoltaic applications , 2014 .

[11]  M. Zhu,et al.  Prediction of lattice constant in cubic perovskites , 2006 .

[12]  M. Ghebouli,et al.  First-principles calculations on structural, elastic, electronic, optical and thermal properties of CsPbCl3 perovskite , 2011 .

[13]  J. Noh,et al.  Chemical management for colorful, efficient, and stable inorganic-organic hybrid nanostructured solar cells. , 2013, Nano letters.

[14]  Lukas Schmidt-Mende,et al.  Research Update: Physical and electrical characteristics of lead halide perovskites for solar cell applications , 2014 .

[15]  D. Trots,et al.  High-temperature structural evolution of caesium and rubidium triiodoplumbates , 2008 .

[16]  K. Asai,et al.  Electronic structures of lead iodide based low-dimensional crystals , 2003 .

[17]  Mercouri G Kanatzidis,et al.  Anomalous band gap behavior in mixed Sn and Pb perovskites enables broadening of absorption spectrum in solar cells. , 2014, Journal of the American Chemical Society.

[18]  Y. Kanemitsu,et al.  Photoelectronic Responses in Solution-Processed Perovskite CH$_{\bf 3}$ NH$_{\bf 3}$PbI $_{\bf 3}$ Solar Cells Studied by Photoluminescence and Photoabsorption Spectroscopy , 2015, IEEE Journal of Photovoltaics.

[19]  Gustavo E Scuseria,et al.  Assessment and validation of a screened Coulomb hybrid density functional. , 2004, The Journal of chemical physics.

[20]  Martin Schreyer,et al.  Synthesis and crystal chemistry of the hybrid perovskite (CH3NH3) PbI3 for solid-state sensitised solar cell applications , 2013 .

[21]  X. Gong,et al.  First-principles study on the electronic and optical properties of cubic ABX3 halide perovskites , 2013, 1309.0070.

[22]  M. Schreiber,et al.  Electronic structure, photoemission spectra, and vacuum-ultraviolet optical spectra of CsPb Cl 3 and CsPb Br 3 , 1981 .

[23]  T. Matsui,et al.  Structural phase transitions of the polymorphs of CsSnI3 by means of rietveld analysis of the X-ray diffraction. , 1991 .

[24]  M. Kanatzidis,et al.  Controllable perovskite crystallization at a gas-solid interface for hole conductor-free solar cells with steady power conversion efficiency over 10%. , 2014, Journal of the American Chemical Society.

[25]  Se-Young Jeong,et al.  Twin structure by 133Cs NMR in ferroelastic CsPbCl3 crystal , 1999 .

[26]  Paolo Umari,et al.  Relativistic GW calculations on CH3NH3PbI3 and CH3NH3SnI3 Perovskites for Solar Cell Applications , 2014, Scientific Reports.

[27]  T. Matsui,et al.  Structural phase transition and electrical conductivity of the perovskite CH3NH3Sn1−xPbxBr3 and CsSnBr3 , 1990 .

[28]  Gerbrand Ceder,et al.  Identification and design principles of low hole effective mass p-type transparent conducting oxides , 2013, Nature Communications.

[29]  N. Kitazawa,et al.  Optical properties of CH3NH3PbX3 (X = halogen) and their mixed-halide crystals , 2002 .

[30]  M. Kanatzidis,et al.  All-solid-state dye-sensitized solar cells with high efficiency , 2012, Nature.

[31]  Aron Walsh,et al.  Structural and electronic properties of hybrid perovskites for high-efficiency thin-film photovoltaics from first-principles , 2013, 1309.4215.