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Effect of Nitrogen Flow in Hydrogen/Nitrogen Plasma Annealing on Aluminum-Doped Zinc Oxide/Tin-Doped Indium Oxide Bilayer Films Applied in Low Emissivity Glass

机译:氮气/氮血浆退火对低发射玻璃铝掺杂锌氧化锌/锡掺杂氧化物双层膜的影响

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摘要

Low emissivity glass (low-e glass), which is often used in energy-saving buildings, has high thermal resistance and visible light transmission. Heavily doped wide band gap semiconductors like aluminum-doped zinc oxide (AZO) and tin-doped indium oxide (ITO) have these properties, especially after certain treatment. In our experiments, in-line sputtered AZO and ITO bilayer (AZO/ITO) films on glass substrates were prepared first. The deposition of AZO/ITO films was following by annealing in hydrogen/nitrogen (H2/N2) plasma with different N2 flows. The structure and optical and electrical properties of AZO/ITO films were surveyed. Experiment results indicated that N2 flow in H2/N2 plasma annealing of AZO/ITO films slightly modified the structure and electrical properties of AZO/ITO films. The X-ray diffraction peak corresponding to zinc oxide (002) crystal plane slightly shifted to a higher angle and its full width at half maximum decreased as the N2 flow increased. The electrical resistivity and the emissivity reduced for the plasma annealed AZO/ITO films when the N2 flow was raised. The optimum H2/N2 gas flow was 100/100 for plasma annealed AZO/ITO films in this work for low emissivity application. The emissivity and average visible transmittance for H2/N2 = 100/100 plasma annealed AZO/ITO were 0.07 and 80%, respectively, lying in the range of commercially used low emissivity glass.
机译:通常用于节能建筑的低发射玻璃(低E玻璃)具有高耐热性和可见光透光。掺杂掺杂的宽带间隙半导体,如铝掺杂的氧化锌(偶氮)和掺杂锡掺杂的氧化物(ITO)具有这些性质,尤其是在某些处理之后。在我们的实验中,首先制备玻璃基板上的在线溅射的偶氮和ITO双层(AZO / ITO)膜。通过用不同的N 2流动在氢气/氮气(H2 / N 2)等离子体中通过退火来沉积AZO / ITO膜。调查了AZO / ITO薄膜的结构和光学和电气性能。实验结果表明,偶氮/ ITO薄膜的H2 / N2等离子体退火中的N2流动略微修改了AZO / ITO薄膜的结构和电性能。随着N2流量的增加,对应于氧化锌(002)晶面的X射线衍射峰值略微移位到较高角度,并且其全宽度降低。当升高时,电阻率和发射率降低了等离子体退火的AZO / ITO膜。最佳H2 / N 2气流为血浆退火的AZO / ITO薄膜100/100,用于低发射率应用。 H2 / N2 = 100/100等离子体退火的辐射/ ITO的发射率和平均可见光率分别为0.07和80%,位于商业上使用的低发射玻璃范围内。

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