AVS 66th International Symposium & Exhibition | |
Thin Films Division | Thursday Sessions |
Session TF-ThP |
Session: | Thin Films Poster Session |
Presenter: | Keisuke Nakamura, Kogakuin University, Japan |
Authors: | K. Nakamura, Kogakuin University, Japan K. Sasaki, Kogakuin University, Japan Y. Shibata, Kogakuin University, Japan K. Oe, Kogakuin University, Japan S. Aikawa, Kogakuin University, Japan |
Correspondent: | Click to Email |
Indium oxide (In2O3)-based thin-film transistor (TFT) have attractive much attention because high field-effect mobility (> 10 cm2/Vs) can be obtained even room temperature deposition. However, a high-temperature post-annealing is necessary for typical fabrication processes. This sacrifices the merit of In2O3-based TFTs that can be fabricated at low temperature. One reason for high-temperature treatment is that an In2O3 surface might be sensitive to ambient gases, thus, the electrical properties of the film is changed in various environmental conditions. In order to clarify such instability, we investigate the electrical properties of In2O3 TFT in ambient, vacuum and N2 environments.
The In2O3 TFT was fabricated on a Si substrate with a thermally-grown oxide layer (SiO2 thickness: 200 nm). Before deposition of In2O3 active channels, the substrate was ultrasonically cleaned in acetone and isopropyl alcohol, and was irradiated by an excimer lamp (wavelength: 172 nm) for 5 min to remove the organic residue. The In2O3 film was then deposited at room temperature by RF magnetron sputtering. The O2/(Ar + O2) ratio, RF power and total pressure during sputtering deposition were fixed at 25 %, 100 W and 0.24 Pa, respectively. The background pressure was below ~5 × 10−4 Pa. The thickness of the active channel formed through a stencil shadow mask was 20 nm by optimizing the deposition time. Source and drain electrodes (Cu: 100 nm) were then formed by an electron beam evaporation through a stencil shadow mask. The In2O3 TFT was characterized in a vacuum probe station with a semiconductor parameter analyzer (Agilent 4156A) at room temperature in the dark condition. The electrical measurement of the TFTs was performed in ambient at first, then the chamber was evacuated to ~4 × 10‒2 Pa for vacuum measurement. A N2 gas was subsequently introduced into the chamber to be N2 environmental condition.
The In2O3 TFT properties were drastically changed between ambient and vacuum conditions. This might be caused by desorption of excess oxygen in the film. To investigate a measurement environmental sensitivity in In2O3 TFT, a sequential I-V measurement was performed. The result showed that the transfer characteristics between 1st and 2nd measurement is obviously different. The degradation of the sensitivity after the 2nd measurement might be due to N2 molecule passivation. However, the sensitivity tended to slight recover with increasing the number of measurements. We will discuss the N2 passivation effect, and the relationship between the sensitivity and number of measurements.