TY - GEN
T1 - Structural, electronic, and optical properties of the In2O 3(ZnO)n system
AU - Yan, Yanfa
AU - Walsh, Aron
AU - Da Silva, Juarez L.F.
AU - Wei, Su Huai
AU - Al-Jassim, Mowafak
PY - 2009
Y1 - 2009
N2 - We studied the structural, electronic, and optical properties of the In2O3(ZnO)n system by a combination of high-resolution electron microscopy, image simulation, and density-functional theory calculation. We found that the In2O3(ZnO) n system has a polytypoid structure that consists of wurtzite InZnnOn+1 slabs separated by single In-O octahedral layers. These octahedral layers are inversion domain boundaries and satisfy the electronic octet rule. The InZnnOn+1 slabs contain another type of boundary that inverts the polarities again. This boundary prefers a zigzag modulated structure and also obeys the electronic octet rule. We also found that the red-shift in optical transitions for the In2O 3(ZnO)n system as compared to individual In 2O3 and ZnO systems is because the symmetry-forbidden band-edge transitions in In2O3 are overcome by the formation of superlattices, with ZnO contributions to the top of the valence band. We further found that increasing n results in an enhanced valence-band maximum in the ZnO region, while the conduction-band minimum becomes more localized on the InO2 layers, which introduces confinement to electron carriers. Such enhanced localization explains why Zn-rich compounds (higher n) exhibit lower conductivity.
AB - We studied the structural, electronic, and optical properties of the In2O3(ZnO)n system by a combination of high-resolution electron microscopy, image simulation, and density-functional theory calculation. We found that the In2O3(ZnO) n system has a polytypoid structure that consists of wurtzite InZnnOn+1 slabs separated by single In-O octahedral layers. These octahedral layers are inversion domain boundaries and satisfy the electronic octet rule. The InZnnOn+1 slabs contain another type of boundary that inverts the polarities again. This boundary prefers a zigzag modulated structure and also obeys the electronic octet rule. We also found that the red-shift in optical transitions for the In2O 3(ZnO)n system as compared to individual In 2O3 and ZnO systems is because the symmetry-forbidden band-edge transitions in In2O3 are overcome by the formation of superlattices, with ZnO contributions to the top of the valence band. We further found that increasing n results in an enhanced valence-band maximum in the ZnO region, while the conduction-band minimum becomes more localized on the InO2 layers, which introduces confinement to electron carriers. Such enhanced localization explains why Zn-rich compounds (higher n) exhibit lower conductivity.
UR - http://www.scopus.com/inward/record.url?scp=77951569333&partnerID=8YFLogxK
U2 - 10.1109/PVSC.2009.5411702
DO - 10.1109/PVSC.2009.5411702
M3 - Conference contribution
AN - SCOPUS:77951569333
SN - 9781424429509
T3 - Conference Record of the IEEE Photovoltaic Specialists Conference
SP - 172
EP - 174
BT - 2009 34th IEEE Photovoltaic Specialists Conference, PVSC 2009
T2 - 2009 34th IEEE Photovoltaic Specialists Conference, PVSC 2009
Y2 - 7 June 2009 through 12 June 2009
ER -