DC sputter deposition of amorphous indiumgalliumzincoxide (a-IGZO) lms with H 2 O introduction Takafumi Aoi a , Nobuto Oka a , Yasushi Sato a , Ryo Hayashi b , Hideya Kumomi b , Yuzo Shigesato a, a Graduate School of Science and Engineering, Aoyama Gakuin University, 5-10-1, Fuchinobe, Sagamihara, Kanagawa 229-8558, Japan b Canon Inc., 3-30-2 Shimomaruko, Ohta-ku, Tokyo 146-8501, Japan abstract article info Available online 13 October 2009 Keywords: Amorphous indium gallium zinc oxide Transparent amorphous semiconductor oxide H 2 O dc magnetron sputtering Thin lm transistor Amorphous indiumgalliumzincoxide (a-IGZO) lms were deposited by dc magnetron sputtering with H 2 O introduction and how the H 2 O partial pressure (P H 2 O ) during the deposition affects the electrical properties of the lms was investigated in detail. Resistivity of the a-IGZO lms increased dramatically to over 2×10 5 Ωcm with increasing P H 2 O to 2.7×10 -2 Pa while the hydrogen concentration in the lms increased to 2.0 × 10 21 cm -3 . TFTs using a-IGZO channels deposited under P H 2 O at 1.68.6 × 10 -2 Pa exhibited a eld-effect mobility of 1.43.0 cm 2 /Vs, subthreshold swing of 1.01.6 V/decade and onoff current ratio of 3.9 × 10 7 1.0 × 10 8 . © 2009 Elsevier B.V. All rights reserved. 1. Introduction Transparent amorphous oxide semiconductors (TAOSs) have attracted much attention as high performance channel materials for thin lm transistors (TFTs) [14]. TAOSs can be fabricated on plastic substrates at low temperature by physical vapor deposition methods such as the conventional dc sputtering method. In particular, the carrier density of amorphous indium gallium zinc oxide (a-IGZO) can be precisely controlled at very low levels, which is stable under various conditions. Thus, a-IGZO has been the strongest candidate for the semiconductor layer in TFTs. Yabuta, et al. have demonstrated high-performance TFTs using a-IGZO lms deposited by rf sputtering on exible plastic substrates [5]. It is well known that 10 -3 10 -4 Pa of H 2 O vapor exists in the sputter chambers normally used in the industry and the precise control of P H 2 O should be important in optimizing the electrical properties and surface morphologies of transparent conducting oxide (TCO) or TAOS lms. We have previously reported that the electrical properties of ZnO-based TCO lms deposited by sputtering were strongly affected by the H 2 O partial pressure (P H 2 O ) of the residual gas in the vacuum chamber [6]. On the other hands, there have been attempts to use industrially applicable H 2 O as a reactive gas to improve the electrical properties or etching rate of Sn-doped In 2 O 3 (ITO) lms [79]. Therefore, it must be important to investigate the effects of H 2 O introduction into the deposition processes to yield a-IGZO lms with the electrical properties appropriate for TFT applications. In this study we investigated the effects of P H 2 O on the electrical properties of a-IGZO lms and on the TFT's device characteristics. 2. Experimental details 2.1. Deposition of the a-IGZO lms by dc sputtering with H 2 O introduction 200-nm-thick a-IGZO lms were deposited on fused silica glass and alkali-free glass (Corning #1737) substrates by dc magnetron sputtering using a polycrystalline InGaZnO 4 ceramic sputtering target (Toshima MFG Co., Ltd.). The sputtering gas was a mixture of Ar and H 2 O vapor, whose total pressure was maintained at 0.5 Pa. These depositions were carried out under various P H 2 O from 8.0 × 10 -4 to 6.0×10 -2 Pa. As illustrated in Fig. 1, the P H 2 O during sputter deposition of a-IGZO lms was precisely controlled using a precision needle valve and quadrupole mass spectrometer (QMS), where P H 2 O can be monitored quantitatively. The distance between the substrate and target was 60 mm, and the sputtering power was kept at 50 W. 2.2. Fabricating TFTs using a-IGZO lms Bottom gate, bottom contact-type TFT devices were fabricated on alkali-free glass (Corning #1737) substrates. As shown in Fig. 2, the TFT is composed of a gate electrode of Mo lm (thickness: 100 nm), a gate insulator of SiO 2 lm (thickness: 200 nm), a channel layer of a-IGZO lm (thickness: 30 nm), source and drain electrodes of an ITO lm (thickness: 30 nm) and a channel protection layer of SiO 2 lm (thickness: 200 nm). The channel width and length were 180 μm and 30 μm, respectively. The a-IGZO channel layer was deposited by dc magnetron sputtering with H 2 O introduction, where the P H 2 O was Thin Solid Films 518 (2010) 30043007 Corresponding author. Tel.: +81 42 759 6223; fax: +81 42 759 6493. E-mail address: yuzo@chem.aoyama.ac.jp (Y. Shigesato). 0040-6090/$ see front matter © 2009 Elsevier B.V. All rights reserved. doi:10.1016/j.tsf.2009.09.176 Contents lists available at ScienceDirect Thin Solid Films journal homepage: www.elsevier.com/locate/tsf