TY - JOUR
T1 - Doping limitation due to self-compensation by native defects in In-doped rocksalt Cdx Zn1-x O
AU - Ho, Chun Yuen
AU - Li, Chia Hsiang
AU - Liu, Chao Ping
AU - Huang, Zhi-Quan
AU - Chuang, Feng-Chuan
AU - Yu, Kin Man
PY - 2022/2/9
Y1 - 2022/2/9
N2 - Cadmium oxide (CdO)-ZnO alloys (Cdx Zn1-xO) exhibit a transformation from the wurtzite to the rocksalt (RS) phase at a CdO composition of ∼70% with a drastic change in the band gap and electrical properties. RS-Cdx Zn1-xO alloys (x > 0.7) are particularly interesting for transparent conductor applications due to their wide band gap and high electron mobility. In this work, we synthesized RS-Cdx Zn1-xO alloys doped with different concentrations of In dopants and evaluated their electrical and optical properties. Experimental results are analyzed in terms of the amphoteric native defect model and compared directly to defect formation energies obtained by hybrid density functional theory (DFT) calculations. A saturation in electron concentration of ∼7 × 1020 cm-3 accompanied by a rapid drop in electron mobility is observed for the RS-Cdx Zn1-xO films with 0.7 ≤ x < 1 when the In dopant concentration [In] is larger than 3%. Hybrid DFT calculations confirm that the formation energy of metal vacancy acceptor defects is significantly lower in RS-Cdx Zn1-xO than in CdO, and hence limits the free carrier concentration. Mobility calculations reveal that due to the strong compensation by native defects, RS-Cdx Zn1-xO alloys exhibit a compensation ratio of >0.7 for films with x < 0.8. As a consequence of the compensation by native defects, in heavily doped RS-Cdx Zn1-xO carrier-induced band filling effect is limited. Furthermore, the much lower mobility of the RS-Cdx Zn1-xO alloys also results in a higher resistivity and reduced transmittance in the near infra-red region (λ > 1100 nm), making the material not suitable as transparent conductors for full spectrum photovoltaics.
AB - Cadmium oxide (CdO)-ZnO alloys (Cdx Zn1-xO) exhibit a transformation from the wurtzite to the rocksalt (RS) phase at a CdO composition of ∼70% with a drastic change in the band gap and electrical properties. RS-Cdx Zn1-xO alloys (x > 0.7) are particularly interesting for transparent conductor applications due to their wide band gap and high electron mobility. In this work, we synthesized RS-Cdx Zn1-xO alloys doped with different concentrations of In dopants and evaluated their electrical and optical properties. Experimental results are analyzed in terms of the amphoteric native defect model and compared directly to defect formation energies obtained by hybrid density functional theory (DFT) calculations. A saturation in electron concentration of ∼7 × 1020 cm-3 accompanied by a rapid drop in electron mobility is observed for the RS-Cdx Zn1-xO films with 0.7 ≤ x < 1 when the In dopant concentration [In] is larger than 3%. Hybrid DFT calculations confirm that the formation energy of metal vacancy acceptor defects is significantly lower in RS-Cdx Zn1-xO than in CdO, and hence limits the free carrier concentration. Mobility calculations reveal that due to the strong compensation by native defects, RS-Cdx Zn1-xO alloys exhibit a compensation ratio of >0.7 for films with x < 0.8. As a consequence of the compensation by native defects, in heavily doped RS-Cdx Zn1-xO carrier-induced band filling effect is limited. Furthermore, the much lower mobility of the RS-Cdx Zn1-xO alloys also results in a higher resistivity and reduced transmittance in the near infra-red region (λ > 1100 nm), making the material not suitable as transparent conductors for full spectrum photovoltaics.
KW - CdO
KW - CdZnO
KW - defects
KW - transparent conducting oxides
UR - http://www.scopus.com/inward/record.url?scp=85120658311&partnerID=8YFLogxK
UR - https://www.scopus.com/record/pubmetrics.uri?eid=2-s2.0-85120658311&origin=recordpage
U2 - 10.1088/1361-648X/ac3585
DO - 10.1088/1361-648X/ac3585
M3 - RGC 21 - Publication in refereed journal
SN - 0953-8984
VL - 34
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 6
M1 - 065702
ER -