However, HfO2 dielectric film has a critical disadvantage of high charge trap density between the gate electrode and gate dielectric, as well as the gate dielectric and channel layer [7]. Recently, rare earth (RE) oxide films have been extensively investigated due to their probable thermal, physical, and Veliparib solubility dmso electrical performances [6]. To date, the application of RE oxide materials as gate dielectrics in a-IGZO TFTs has not been reported. Among the RE oxide films, an erbium oxide (Er2O3) film can be considered as a gate oxide because of its large dielectric constant (approximately 14), wide bandgap energy (>5 eV), and high transparency in the visible range

[8, 9]. The main problem when using RE films is moisture absorption, which degrades their permittivity due to the formation of low-permittivity hydroxides [10]. The moisture absorption of RE oxide films RGFP966 nmr may be attributed to the oxygen vacancies in the films [11]. To solve this problem, the addition of Ti or TiO x (κ = 50 to approximately 110) into the RE dielectric films can result in improved physical and electrical properties [12]. In this study, we Angiogenesis inhibitor compared the structural and electrical properties of Er2O3 and Er2TiO5 gate dielectrics on the a-IGZO TFT devices. Methods The Er2O3 and Er2TiO5 a-IGZO TFT devices were fabricated on the insulated SiO2/Si substrate. A 50-nm TaN

film was deposited on the SiO2 as a bottom gate through a reactive sputtering system. Next, an approximately 45-nm Er2O3 was deposited by sputtering from an Er target,

while an Er2TiO5 thin film (approximately 45 nm) was deposited through cosputtering using both Er and Ti targets at room temperature. Then, postdeposition annealing was performed using furnace in O2 ambient for Rho 10 min at 400°C. The a-IGZO channel material (approximately 20 nm) was deposited at room temperature by sputtering from a ceramic IGZO target (In2O3/Ga2O3/ZnO = 1:1:1). Top Al (50 nm) source/drain electrodes were formed by a thermal evaporation system. The channel width/length of examined device was 1,000/200 μm. The film structure and composition of the dielectric films were analyzed using X-ray diffraction (XRD) and X-ray photoelectron spectroscopy (XPS), respectively. The surface morphology of the films was investigated by atomic force microscopy (AFM). The capacitance-voltage (C-V) curves of the Al/Er2O3/TaN and Al/Er2TiO5/TaN devices were measured using a HP4284 LCR meter. The electrical characteristics of the a-IGZO TFT device were performed at room temperature using a semiconductor parameter Hewlett-Packard (HP) 4156C (Palo Alto, CA, USA). The threshold voltage (V TH) was determined by linearly fitting the square root of the drain current versus the gate voltage curve. Field-effect mobility (μ FE) is derived from the maximum transconductance. Results and discussion Figure  1 displays the XRD patterns of the Er2O3 and Er2TiO5 thin films deposited on the TaN/SiO2/Si substrate.