Electrical Properties of Pulsed Laser Deposited Y 2 O 3 Gate Oxide on 4H–SiC Hock Jin Quah, a Way Foong Lim, a Stuart C. Wimbush, b Zainovia Lockman, a and Kuan Yew Cheong a,z a Energy Efficient and Sustainable Semiconductor Research Group, School of Materials and Mineral Resources Engineering, Universiti Sains Malaysia, Engineering Campus, 14300 Nibong Tebal, Pulau Pinang, Malaysia b Department of Materials Science and Metallurgy, University of Cambridge, Cambridge CB2 3QZ, United Kingdom Yttrium oxide Y 2 O 3 has been successfully deposited on n-type 4H–SiC substrates using pulsed laser deposition. The effects of postdeposition annealing temperature 400, 500, and 600°Con the electrical properties of the Y 2 O 3 gate oxide have been studied in comparison with the as-deposited sample. The sample annealed at 600°C possessed the highest dielectric breakdown field of 6.5 MV cm -1 at 10 -6 A cm -2 , resulting from the lowest interface trap density and total interface trap density. The Fowler– Nordheim tunneling mechanism has been investigated on all samples and the highest value of barrier height extracted between the semiconductor and oxide conduction band edges was 2.67 eV. © 2010 The Electrochemical Society. DOI: 10.1149/1.3481926All rights reserved. Manuscript submitted July 8, 2010; revised manuscript received July 28, 2010. Published September 3, 2010. Tremendous research effort has been focused on the utilization of wide bandgap WBGsemiconductors as substrates for high power metal oxide semiconductor MOSbased devices due to their im- pressive properties. Among the WBG semiconductors, silicon car- bide SiCwith its high breakdown field E B , high electron drift velocity, and high thermal conductivity has been suggested as a suitable substrate for the aforementioned application. 1,2 The integra- tion of a high quality gate oxide is essential in SiC-based MOS devices to prevent the injection of charge from the SiC or the gate electrode, thus sustaining a high E B and a low gate leakage current. 3 The exceptional advantage of SiC when compared with other WBGs is its ability to produce a native oxide SiO 2 via thermal oxidation. 1,4 To date, thermally nitrided SiO 2 on SiC is regarded as the most promising gate oxide due to its exhibition of an extremely low leakage current. 5-7 However, its relatively low dielectric con- stant SiO 2 = 3.9when compared to that of SiC SiC = 9.7may constrain the maximum permissible electric field. 8,9 Therefore, the application of high-gate oxides such as Al 2 O 3 , 10 CeO 2 , 9 La 2 O 3 , 11 HfO 2 , 12 and Gd 2 O 3 13 on SiC substrates has been thoroughly inves- tigated to enable the exploitation of the SiC breakdown field. Yt- trium oxide Y 2 O 3 is a potential candidate as an alternative gate oxide for SiO 2 due to its relatively high-value = 14–18, large bandgap 5.5 eV, and high thermal stability of up to 2300°C. 14,15 However, there is no article on utilizing Y 2 O 3 as the gate oxide for SiC MOS-based devices. Thus, the effects of postdeposition anneal- ing on the MOS characteristics of a pulsed laser deposited Y 2 O 3 film on SiC have been systematically investigated in this work. Experimental n-Type, 8° off 0001oriented, 4H–SiC wafers with a 10 m thick epilayer doped with 1–410 16 cm -3 of nitrogen were used as the starting substrates. The SiC wafer was subjected to the RCA cleaning process, and the native oxide of SiO 2 was etched by HF:H 2 O 1:50solution. Y 2 O 3 films with a thickness of 20 nm were deposited on these substrates by off-axis pulsed laser deposi- tion KrF of = 248 nm, 10 Hz, 2 J cm -2 in an oxygen atmo- sphere 30 Pato maintain oxygen stoichiometry, in which the thick- ness was measured by in situ growth process. The substrates were held at 800°C during deposition and subsequently cooled at 30°C /min in 0.5 atm static oxygen. After the deposition, an ex situ postdeposition annealing treatment was performed at different tem- peratures 400, 500, and 600°Cin argon atmosphere for 15 min. The heating and cooling rates were 5°C /min. A typical field- emission-scanning electron microscopy FESEMmicrograph inset of Fig. 1reveals that the produced film is smooth and uniform, while energy-dispersive X-ray spectroscopy not shownperformed at six different locations showed that Y 2 O 3 is homogenously distrib- uted through the film with an atomic percentage of Y and O of 0.97 0.05 and 1.46 0.15 atom %, respectively. Thus, the re- sulting film achieved a stoichiometric of Y:O = 2:3. After cooling, a layer of Al was thermally evaporated on top of the oxide. An array of 2.5 10 -3 cm 2 Al gate electrodes was then defined using a pho- tolithography process. Electrical properties of the test structures were examined by high frequency 1 MHzcapacitance–voltage C-Vand current–voltage measurements using an LCR meter Agi- lent 4284Aand a semiconductor parameter analyzer Agilent 4156C, respectively. Results and Discussion Figure 1 presents the high frequency normalized C-V curves of the as-deposited and annealed Y 2 O 3 films at different temperatures, in which the gate bias is swept bidirectionally from -4 to +4 V. Negative flatband voltage shift V FB is observed in both the 400 and 500°C annealed samples, implying that positive traps are present in these samples. A larger negative V FB is exhibited by the sample z E-mail: cheong@eng.usm.my Figure 1. 1 MHz normalized C-V curves for the as-deposited and annealed Y 2 O 3 gate oxides on SiC same symbols used in this figure apply to the following figures. The inset shows a typical FESEM micrograph of Y 2 O 3 film annealed at 600°C. Electrochemical and Solid-State Letters, 13 11H396-H398 2010 1099-0062/2010/1311/H396/3/$28.00 © The Electrochemical Society H396 Downloaded 05 Sep 2010 to 202.170.51.222. Redistribution subject to ECS license or copyright; see http://www.ecsdl.org/terms_use.jsp