Apr 23, 2024
11:15am - 11:30am
Room 448, Level 4, Summit
Chase Brooks1,Mark van Schilfgaarde2,Dimitar Pashov3,Jocienne Nelson2,Kirstin Alberi2,Daniel Dessau1,Stephan Lany2
University of Colorado Boulder1,National Renewable Energy Laboratory2,King's College London3
Chase Brooks1,Mark van Schilfgaarde2,Dimitar Pashov3,Jocienne Nelson2,Kirstin Alberi2,Daniel Dessau1,Stephan Lany2
University of Colorado Boulder1,National Renewable Energy Laboratory2,King's College London3
Cd<sub>3</sub>As<sub>2</sub> is a three-dimensional Dirac semimetal with sustained scientific interest. Intrinsic point defects, however, induce excess electron carriers that elevate the Fermi level <i>E</i><sub>F</sub> away from the Dirac point and limit accessibility to its topological features. By combining density functional theory (DFT) calculations of defect formation energies and quasiparticle self-consistent GW (QSGW) electronic structure calculations, we demonstrate an innate concentration dependence of defect formation energies, and we find that Cd interstitials are the primary source of this self-doping. We extrapolate formation energies to arbitrary electron concentrations, and we utilize a thermodynamic defect equilibria model to study how extrinsic electron accepting dopants (e.g. Si, Ge, Sn) and particular growth conditions can tune <i>E</i><sub>F</sub> closer to the Dirac point. Separately, Zn<sub>3</sub>As<sub>2</sub> is a trivial semiconductor with a direct band gap of 1.0 eV that typically forms with intrinsic <i>p</i>-type doping, so the (Cd,Zn)<sub>3</sub>As<sub>2</sub> alloy system is expected to undergo both a topological phase transition and a net doping crossover. Using Monte Carlo simulations, we determined representative alloy structures, which can serve as the basis for predicting electronic structure and defect properties of the alloy.