TY - JOUR
T1 - Effect of ambient air flow on resistivity uniformity of transparent Ga-doped ZnO film deposited by atmospheric pressure plasma jet
AU - Juang, Jia Yang
AU - Lin, Hsin Tien
AU - Liang, Chun Tang
AU - Li, Pei Rong
AU - Chen, Wen Kai
AU - Chen, Yu Yi
AU - Pan, Kuo Long
N1 - Funding Information:
This work is supported by National Taiwan University ( NTU-10R70855 ) and ( 107L891006 ), and the Ministry of Science and Technology (MOST) of Taiwan ( 104-2221-E-002-024-MY2 ), ( 104-2221-E-002-022-MY2 ) and ( 106-2221-E-002-123-MY3 ). We thank Hsiao-Ping Hsu for technical support of XPS, and Dr. Jui-Mei Hsu (ITRI) for technical support of plasma jet. We thank Prof. I-Chun Cheng, Prof. Jian-Zhang Chen, and Prof. Li Xu for helpful discussions.
Funding Information:
This work is supported by National Taiwan University (NTU-10R70855) and (107L891006), and the Ministry of Science and Technology (MOST) of Taiwan (104-2221-E-002-024-MY2), (104-2221-E-002-022-MY2) and (106-2221-E-002-123-MY3). We thank Hsiao-Ping Hsu for technical support of XPS, and Dr. Jui-Mei Hsu (ITRI) for technical support of plasma jet. We thank Prof. I-Chun Cheng, Prof. Jian-Zhang Chen, and Prof. Li Xu for helpful discussions.
Publisher Copyright:
© 2018 Elsevier B.V.
PY - 2018/10/25
Y1 - 2018/10/25
N2 - Transparent gallium-doped zinc oxide films were deposited on large area (117 mm × 185 mm) glass substrates by atmospheric pressure plasma jet method, using two different enclosure conditions—with and without side opening boundary. The opening allows gas exchange between the growth ambient and outside atmosphere. The spatial resistivity distribution was apparently influenced by the air flow field. The case with side opening has higher overall non-uniformity, and the film near the opening has the highest resistivity, caused by considerable reduction in carrier concentration (−32%) and mobility (−15%). Computer fluid dynamics simulations show that air was drawn in, through the side opening, from outside atmosphere, resulting in a much higher oxygen mass fraction (+50%) near the opening. As such, the film near the opening was deposited in O-rich conditions. The degradation of electrical conductivity in O-rich conditions cannot be explained by oxygen vacancies. We suggest that it is due to the formation of dopant-defect complex GaZn−VZn (the lowest formation energy) and reduction of hydrogen impurity (reduced hydrogen partial pressure) in O-rich conditions. Therefore, the tool enclosure, gas flow field, and scanning trajectory must be carefully designed to achieve minimum resistivity non-uniformity on large-area substrates.
AB - Transparent gallium-doped zinc oxide films were deposited on large area (117 mm × 185 mm) glass substrates by atmospheric pressure plasma jet method, using two different enclosure conditions—with and without side opening boundary. The opening allows gas exchange between the growth ambient and outside atmosphere. The spatial resistivity distribution was apparently influenced by the air flow field. The case with side opening has higher overall non-uniformity, and the film near the opening has the highest resistivity, caused by considerable reduction in carrier concentration (−32%) and mobility (−15%). Computer fluid dynamics simulations show that air was drawn in, through the side opening, from outside atmosphere, resulting in a much higher oxygen mass fraction (+50%) near the opening. As such, the film near the opening was deposited in O-rich conditions. The degradation of electrical conductivity in O-rich conditions cannot be explained by oxygen vacancies. We suggest that it is due to the formation of dopant-defect complex GaZn−VZn (the lowest formation energy) and reduction of hydrogen impurity (reduced hydrogen partial pressure) in O-rich conditions. Therefore, the tool enclosure, gas flow field, and scanning trajectory must be carefully designed to achieve minimum resistivity non-uniformity on large-area substrates.
UR - http://www.scopus.com/inward/record.url?scp=85049538323&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85049538323&partnerID=8YFLogxK
U2 - 10.1016/j.jallcom.2018.07.030
DO - 10.1016/j.jallcom.2018.07.030
M3 - Article
AN - SCOPUS:85049538323
SN - 0925-8388
VL - 766
SP - 868
EP - 875
JO - Journal of Alloys and Compounds
JF - Journal of Alloys and Compounds
ER -