10 research outputs found
Electronic structure and light-induced conductivity in a transparent refractory oxide
Combined first-principles and experimental investigations reveal the
underlying mechanism responsible for a drastic change of the conductivity (by
10 orders of magnitude) following hydrogen annealing and UV-irradiation in a
transparent oxide, 12CaO.7Al2O3, found by Hayashi et al. The charge transport
associated with photo-excitation of an electron from H, occurs by electron
hopping. We identify the atoms participating in the hops, determine the exact
paths for the carrier migration, estimate the temperature behavior of the
hopping transport and predict a way to enhance the conductivity by specific
doping.Comment: 4 pages including 4 figure
Electronic band structure and carrier effective mass in calcium aluminates
First-principles electronic band structure investigations of five compounds
of the CaO-Al2O3 family, 3CaO.Al2O3, 12CaO.7Al2O3, CaO.Al2O3, CaO.2Al2O3 and
CaO.6Al2O3, as well as CaO and alpha-, theta- and kappa-Al2O3 are performed. We
find that the conduction band in the complex oxides is formed from the oxygen
antibonding p-states and, although the band gap in Al2O3 is almost twice larger
than in CaO, the s-states of both cations. Such a hybrid nature of the
conduction band leads to isotropic electron effective masses which are nearly
the same for all compounds investigated. This insensitivity of the effective
mass to variations in the composition and structure suggests that upon a proper
degenerate doping, both amorphous and crystalline phases of the materials will
possess mobile extra electrons
Hopping versus bulk conductivity in transparent oxides: 12CaO∙7Al2O3
First-principles calculations of the mayenite-based oxide,
[Ca12Al14O32]{2+}(2e-), reveal the mechanism responsible for its high
conductivity. A detailed comparison of the electronic and optical properties of
this material with those of the recently discovered novel transparent
conducting oxide, H-doped UV-activated Ca12Al14O33, allowed us to conclude that
the enhanced conductivity in [Ca12Al14O32]{2+}(2e-) is achieved by elimination
of the Coulomb blocade of the charge carriers. This results in a transition
from variable range hopping behavior with a Coulomb gap in H-doped
UV-irradiated Ca12Al14O33 to bulk conductivity in [Ca12Al14O32]{2+}(2e-).
Further, the high degree of the delocalization of the conduction electrons
obtained in [Ca12Al14O32]{2+}(2e-) indicate that it cannot be classified as an
electride, originally suggested.Comment: submitte