Electronic structure and defect properties of B6O from hybrid functional and many-body perturbation theory calculations: A possible ambipolar transparent conductor

B6O is a member of icosahedral boron-rich solids known for their physical hardness and stability under irradiation bombardment, but it has also recently emerged as a promising high mobility p-type transparent conducting oxide. Using a combination of hybrid functional and many-body perturbation theory calculations, we report on the electronic structure and defect properties of this material. Our calculations identify B6O has a direct band gap in excess of 3.0 eV and possesses largely isotropic and low effective masses for both holes and electrons. Of the native defects, we identify no intrinsic origin to the reported p-type conductivity and confirm that p-type doping is not prevented by intrinsic defects such as oxygen vacancies, which we find act exclusively as neutral defects rather than hole-killing donors. We also investigate a number of common impurities and plausible dopants, finding that isolated acceptor candidates tend to yield deep states within the band gap or act instead as donors, and cannot account for p-type conductivity. Our calculations identify the only shallow acceptor candidate to be a complex consisting of interstitial H bonded to C substituting on the O site (CH)O. We therefore attribute the origins of p-type conductivity to these complexes formed during growth or more likely via isolated CO which later binds with H within the crystal. Lastly, we identify Si as a plausible n-type dopant, as it favorably acts as a shallow donor and does not suffer from self-compensation as may the C-related defects. Thus, in addition to the observed p-type conductivity, B6O exhibits promise of n-type dopability if the stoichiometry and both native and extrinsic sources of compensation can be sufficiently controlled. © 2014 American Physical Society.

[1]  David J. Singh,et al.  BoltzTraP. A code for calculating band-structure dependent quantities , 2006, Comput. Phys. Commun..

[2]  L. Daemen,et al.  Boron suboxide: As hard as cubic boron nitride , 2002 .

[3]  M. Shimode,et al.  Fabrication of bipolar CuInO2 with delafossite structure , 2003 .

[4]  Anubhav Jain,et al.  Python Materials Genomics (pymatgen): A robust, open-source python library for materials analysis , 2012 .

[5]  P. Briddon,et al.  Behavior of hydrogen ions, atoms, and molecules in a-boron studied using density functional calculations , 2011, 1103.3374.

[6]  Giulia Galli,et al.  β-Rhombohedral boron: at the crossroads of the chemistry of boron and the physics of frustration. , 2013, Chemical reviews.

[7]  Jörg Neugebauer,et al.  Role of hydrogen in doping of GaN , 1996 .

[8]  H. Hosono,et al.  SrCu2O2: A p-type conductive oxide with wide band gap , 1998 .

[9]  K. E. Morgan,et al.  Some crystallography, chemistry, physics, and thermodynamics of B12O2, B12P2, B12As2, and related alpha-boron type crystals , 2014 .

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

[11]  J. Woicik,et al.  Origin of the Bipolar Doping Behavior of SnO from X-ray Spectroscopy and Density Functional Theory , 2013 .

[12]  Andrew G. Glen,et al.  APPL , 2001 .

[13]  A. Zakutayev,et al.  Origin of p-type conduction in single-crystal CuAlO2 , 2009 .

[14]  Blöchl,et al.  Projector augmented-wave method. , 1994, Physical review. B, Condensed matter.

[15]  Unusual properties of icosahedral boron-rich solids , 2006 .

[16]  Emin,et al.  Defect clustering and self-healing of electron-irradiated boron-rich solids. , 1995, Physical review. B, Condensed matter.

[17]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[18]  Lee,et al.  Crystal structure, formation enthalpy, and energy bands of B6O. , 1991, Physical review. B, Condensed matter.

[19]  C. Walle,et al.  First-principles calculations for defects and impurities: Applications to III-nitrides , 2004 .

[20]  H. Masumoto,et al.  Thermoelectric Properties of Hot-pressed Boron Suboxide (B6O) , 2002 .

[21]  K. Ellmer Past achievements and future challenges in the development of optically transparent electrodes , 2012, Nature Photonics.

[22]  G. Kresse,et al.  Efficiency of ab-initio total energy calculations for metals and semiconductors using a plane-wave basis set , 1996 .

[23]  G. Scuseria,et al.  Hybrid functionals based on a screened Coulomb potential , 2003 .

[24]  J. Robertson,et al.  Limits to doping in oxides , 2011 .

[25]  Kristin A. Persson,et al.  Commentary: The Materials Project: A materials genome approach to accelerating materials innovation , 2013 .

[26]  Jörg Neugebauer,et al.  Electrostatic interactions between charged defects in supercells , 2011 .

[27]  A. Janotti,et al.  Ambipolar doping in SnO , 2013 .

[28]  K. N. Dollman,et al.  - 1 , 1743 .

[29]  A. Zunger,et al.  Band or Polaron: The Hole Conduction Mechanism in the p-Type Spinel Rh2ZnO4 , 2012 .

[30]  A. J. Bosman,et al.  Small-polaron versus band conduction in some transition-metal oxides , 1970 .

[31]  Stefan Goedecker,et al.  ABINIT: First-principles approach to material and nanosystem properties , 2009, Comput. Phys. Commun..

[32]  H. Hosono,et al.  Bipolarity in electrical conduction of transparent oxide semiconductor CuInO2 with delafossite structure , 2001 .

[33]  Kalyan Kumar Chattopadhyay,et al.  Recent developments in the emerging field of crystalline p-type transparent conducting oxide thin films , 2005 .

[34]  Hideo Hosono,et al.  Ambipolar Oxide Thin‐Film Transistor , 2011, Advanced materials.

[35]  O. Kurakevych,et al.  Experimental study and critical review of structural, thermodynamic and mechanical properties of superhard refractory boron suboxide B6O , 2011, 1107.4895.

[36]  A. Pasquarello,et al.  Defect levels through hybrid density functionals: Insights and applications , 2011 .

[37]  Takao Kotani,et al.  Quasiparticle self-consistent GW theory. , 2006, Physical review letters.

[38]  D. Ginley,et al.  Handbook of transparent conductors , 2011 .

[39]  N. Kirillova,et al.  Properties of Boron Suboxide B13O2 , 2002 .

[40]  Graeme W Watson,et al.  Modeling the polaronic nature of p-type defects in Cu2O: the failure of GGA and GGA + U. , 2009, The Journal of chemical physics.

[41]  Alex Zunger,et al.  Practical doping principles , 2003 .

[42]  D. Lewis,et al.  Non-stoichiometry of boron suboxide (B6O) , 1976 .

[43]  D. Scanlon,et al.  On the possibility of p-type SnO2 , 2012 .

[44]  A. Janotti,et al.  Hydrogenated cation vacancies in semiconducting oxides , 2011, Journal of physics. Condensed matter : an Institute of Physics journal.

[45]  A. Janotti,et al.  Shallow versus deep nature of Mg acceptors in nitride semiconductors. , 2012, Physical review letters.

[46]  C. Freysoldt,et al.  Fully ab initio finite-size corrections for charged-defect supercell calculations. , 2009, Physical review letters.

[47]  P. Buseck,et al.  Icosahedral packing of B12 icosahedra in boron suboxide (B6O) , 1998, Nature.

[48]  Hideo Hosono,et al.  P-type electrical conduction in transparent thin films of CuAlO2 , 1997, Nature.

[49]  O. Biest,et al.  High temperature properties of B6O-materials , 2011 .

[50]  Guojia Fang,et al.  p‐type transparent conducting oxides , 2006 .

[51]  David S. Ginley,et al.  Transparent Conducting Oxides , 2000 .