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Material deposition and laser annealing of metal oxide thin films for electronics fabricated at low temperature

机译:低温制造的电子产品的金属氧化物薄膜的材料沉积和激光退火

摘要

With an aim to investigate methods to realise low thermal-budget fabrication of aluminium doped zinc oxide (AZO) and indium gallium zinc oxide (IGZO) thin films, a dual step fabrication process was studied in this research. Initially, an experimental programme was undertaken to deposit AZO and IGZO films by radio frequency (RF) magnetron sputtering with no external substrate heating and at a wide range of deposition parameters including oxygen to argon ratio, RF power, and sputtering pressure. Thereafter, the samples were subjected to post-depositing annealing in air at ambient temperature utilising the advantages of excimer laser annealing (ELA) with a pulsed krypton fluoride (KrF) excimer laser at different laser fluences and number of pulses. The electrical, structural, compositional, and optical properties of the fabricated samples were systematically investigated as a function of the fabrication (deposition and annealing) conditions. A range of thin film characterisation techniques was used including 4-point probe (4PP), Van der Pauw (VDP), Hall Effect, X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), Atomic-force microscopy (AFM), Energy-dispersive X-ray spectroscopy (EDX), and optical transmittance and reflectance spectroscopy. Sputter-deposition of AZO and IGZO at room temperature revealed that the electrical properties of the deposited films are profoundly controlled by the deposition conditions applied. Low sputtering pressure of 2 mTorr is desired to obtain the best quality materials. However, high RF power of 180 W (4 W/cm2) is required to produce AZO with enhanced crystallinity, high electron density, and thus low resistivity. While, moderate RF power of 50 W (1.1 W/cm2) is applied to produce amorphous IGZO films with moderate-to-high resistivity suitable for thin film transistors (TFTs). The oxygen to argon ratio is found to have the most significant impact on defining the electrical properties for both AZO and IGZO. The resistivity of IGZO films was dependant on their metallic composition which in turn is controlled by the deposition conditions. TFTs were fabricated on silicon substrates with 40 nm thick IGZO as the active layer deposited at room temperature and different growth conditions. TFT performance was largely affected by the active layer deposition conditions. TFTs with the optimised IGZO, deposited at 50 W and 2 mTorr of 2% oxygen to argon ratio, exhibited a field effect mobility of 0.67 cm2/Vs, an on/off current ratio of 5x105, a turn on voltage of -0.15 V, and a subthreshold swing S of 0.28 V/decade. Upon ELA, AZO showed a resistivity reduction which is shown to result from increasing both the free electron density and mobility. When the optimised as-deposited AZO, 180 nm thick deposited at 180 W and 2 mTorr of 0.2% oxygen to argon ratio, annealed with 5 pulses at 125 mJ/cm2, a 50% resistivity reduction to 5x10-4 Ω.cm was obtained. It was demonstrated that average grain size increase, oxygen related defects decrease, and aluminium activation in doped ZnO are the origin of the AZO resistivity reduction upon ELA. Rapid thermal annealing (RTA) was also examined on AZO; RTA in nitrogen at 300°C for 20s increased the AZO gain size and doping efficiency leading to similar resistivity reduction to that achieved by the optimised ELA. Both ELA and RTA enhanced the AZO visible transmission to > 85 %, while the near infrared transmission was degraded due to higher electron density after annealing. The electro-optical properties of the optimised AZO samples obtained by ELA and RTA, which are very close to those of standard tin doped indium oxide (ITO), demonstrate the viability of AZO as an attractive transparent conducting material for various electronic applications. The potential use of AZO for photovoltaics (PVs) as well as the AZO stability against damp heat exposure were also examined. PVs with optimised ELA and RTA treated AZO samples showed comparable power conversion efficiency (PCE) to that of PVs with high-quality commercial ITO. The damp heat stability of AZO samples was strongly dependant on the fabrication conditions. In regard to IGZO, ELA increased the free electron density and mobility leading to better conductivity, while the amorphous structure is maintained. ELA with single pulse at a low energy density of 30 mJ/cm2 resulted in an improved performance for IGZO TFTs on silicon substrates achieving a field effect mobility of 3.33 cm2/Vs, an on/off current ratio of 3x107, a turn on voltage of +0.35 V, and a subthreshold swing S of 0.27 V/decade. Moreover, ELA was successfully applied to IGZO TFTs on polymer flexible PEN leading to TFTs with enhanced performance. Hence, a combination of RF magnetron sputtering at room temperature and ELA, which are both efficiently applicable to thin films mass production, has been demonstrated to provide a low thermal budget fabrication route for functional materials including AZO, as the most promising substitute to ITO in a wide range of applications, and IGZO as the most attractive material for TFT applications. This combination is an alternative thin film fabrication route to using elevated substrate temperature or post-deposition thermal annealing typically applied in the dominant literature reports, to obtain thin films with suitable characteristics.
机译:为了研究实现低热预算制造掺铝氧化锌(AZO)和铟镓锌氧化物(IGZO)薄膜的方法,本研究研究了双步制造工艺。最初,进行了一个实验程序,通过射频(RF)磁控管溅射法沉积AZO和IGZO膜,而无需外部基板加热,并且在包括氧与氩比,RF功率和溅射压力在内的各种沉积参数下进行沉积。此后,利用准分子激光退火(ELA)和脉冲氟化氟化rypto(KrF)准分子激光在不同的激光注量和脉冲数下的优势,在室温下于空气中对样品进行沉积后退火。系统地研究了所制造样品的电学,结构,组成和光学性质,它们是制造条件(沉积和退火)的函数。使用了一系列薄膜表征技术,包括4点探针(4PP),范德堡(VDP),霍尔效应,X射线衍射(XRD),X射线光电子能谱(XPS),原子力显微镜( AFM),能量色散X射线光谱(EDX)以及光透射率和反射率光谱。室温下AZO和IGZO的溅射沉积表明,所沉积薄膜的电学性能受到所应用沉积条件的严格控制。需要2 mTorr的低溅射压力以获得最佳质量的材料。然而,需要180 W(4 W / cm2)的高RF功率来生产具有增强的结晶度,高电子密度和低电阻率的AZO。同时,施加50 W(1.1 W / cm2)的中等RF功率,以生产适用于薄膜晶体管(TFT)的具有中等至高电阻率的非晶IGZO膜。发现氧气与氩气的比例对定义AZO和IGZO的电学性能影响最大。 IGZO膜的电阻率取决于其金属成分,而金属成分又受沉积条件控制。在具有40 nm厚IGZO作为在室温和不同生长条件下沉积的有源层的硅基板上制造TFT。 TFT性能在很大程度上受到有源层沉积条件的影响。具有优化的IGZO的TFT以50 W的功率和2 mTorr的2%氧气与氩气沉积,场效应迁移率为0.67 cm2 / Vs,开/关电流比为5x105,开启电压为-0.15 V,亚阈值摆幅S为0.28 V /十倍。在ELA上,AZO的电阻率降低,这是由于增加了自由电子密度和迁移率所致。当在180 W和2 mTorr的氧气和氩气比率为2 mTorr的条件下沉积180 nm厚的优化沉积态AZO并以125 mJ / cm2的频率进行5次脉冲退火时,电阻率降低了50%,降至5x10-4Ω.cm。 。结果表明,平均晶粒尺寸增加,与氧有关的缺陷减少以及掺杂的ZnO中的铝活化是ELA上AZO电阻率降低的原因。还对AZO进行了快速热退火(RTA);氮气中的RTA在300°C下持续20s会增加AZO的增益大小和掺杂效率,从而导致电阻率的降低与优化的ELA相似。 ELA和RTA都将AZO可见光透射率提高到> 85%,而近红外透射率由于退火后较高的电子密度而降低。通过ELA和RTA获得的优化的AZO样品的电光性能非常接近标准的掺锡氧化铟(ITO),证明了AZO作为有吸引力的透明导电材料在各种电子应用中的可行性。还检查了AZO在光伏(PVs)中的潜在用途以及AZO对湿热暴露的稳定性。经过优化的ELA和RTA处理的AZO样品的PV的功率转换效率(PCE)与具有高质量商用ITO的PV相当。 AZO样品的湿热稳定性在很大程度上取决于制造条件。关于IGZO,ELA增加了自由电子密度和迁移率,从而导致了更好的导电性,同时保持了非晶结构。具有30 mJ / cm2的低能量密度的单脉冲ELA改善了硅基板上的IGZO TFT的性能,实现了3.33 cm2 / Vs的场效应迁移率,3x107的开/关电流比, +0.35 V,亚阈值摆幅S为0.27 V /十倍。此外,ELA已成功应用于聚合物柔性PEN上的IGZO TFT,从而提高了TFT的性能。因此,已经证明,室温下的射频磁控溅射和ELA均可有效地应用于薄膜的大规模生产,从而为包括AZO在内的功能材料提供了低热预算的制造途径。,在广泛的应用中是ITO的最有希望的替代品,而IGZO是TFT应用中最有吸引力的材料。这种组合是使用升高的基板温度或通常在主要文献报道中应用的沉积后热退火来获得具有合适特性的薄膜的另一种薄膜制造途径。

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    Elhamali SO;

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