Figure 2
From: Bistability of Hydrogen in ZnO: Origin of Doping Limit and Persistent Photoconductivity

Electronic structures and optical properties of H-DX−.
Calculated (a) total and (b) partial densities of states for H-DX− in ZnO are shown. The total density of states for perfect (pure) ZnO is also shown (gray filled area) in (a). (c) A schematic diagram for the electronic structures of HO+ and H-DX−. The charge densities of (d) α and (e) α* states are shown with the isosurface value of 3.50 × 10−5 Å−3. (f) The imaginary dielectric function [ε2(ω)] calculated for H-DX− is shown. The dielectric function is calculated by using the Kubo formula based on the electric-dipole-approximation25 and averaged over the x-, y- and z-polarization vectors. Here, we used a 72 atom supercell.