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Optical and hydrophobic properties of co-sputtered chromium and titanium oxynitride films

机译:共溅射铬和氮氧化钛薄膜的光学和疏水特性

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摘要

The chromium and titanium oxynitride films on glass substrate were deposited by using reactive RF magnetron sputtering in the present work. The structural and optical properties of the chromium and titanium oxynitride films as a function of power variations are investigated. The chromium oxynitride films are crystalline even at low power of Cr target (≥60W) but the titanium oxynitride films are amorphous at low target power of Ti target (≤90W) as observed from glancing incidence X-ray diffraction (GIXRD) patterns. The residual stress and strain of the chromium oxynitride films are calculated by sin~2 φ method, as the average crystallite size decreases with the increase in sputtering power of the Cr target, higher stress and strain values are observed. The chromium oxynitride films changes from hydrophilic to hydrophobic with the increase of contact angle value from 86.4° to 94.1°, but the deposited titanium oxynitride films are hydrophilic as observed from contact angle measurements. The changes in surface energy were calculated using contact angle measurements to substantiate the hydrophobic properties of the films. UV-vis and NIR spectrophotometer were used to obtain the transmission and absorption spectra, and the later was used for determining band gap values of the films, respectively. The refractive index of chromium and titanium oxynitride films increases with film packing density due to formation of crystalline chromium and titanium oxynitride films with the gradual rise in deposition rate as a result of increase in target powers.
机译:在本工作中,使用反应性射频磁控溅射在玻璃基板上沉积了铬和氧氮化钛膜。研究了铬和氮氧化钛薄膜的结构和光学性能随功率变化的变化。从掠入式X射线衍射(GIXRD)扫描图可以看出,即使在Cr靶的低功率(≥60W)下,氮氧化铬膜仍是结晶的,而在Ti靶的低靶功率(≤90W)下,氧氮化钛的膜是非晶的。氧氮化铬膜的残余应力和应变是通过sin〜2φ法计算的,随着平均晶粒尺寸随着Cr靶溅射功率的增加而减小,观察到较高的应力和应变值。随着接触角值从86.4°增大到94.1°,氧氮化铬膜从亲水性变为疏水性,但是从接触角测量中观察到,沉积的氧氮化钛膜是亲水性的。使用接触角测量来计算表面能的变化,以证实膜的疏水性。使用紫外可见分光光度计和近红外分光光度计获得透射光谱和吸收光谱,然后使用后者分别确定薄膜的带隙值。铬和氧氮化钛膜的折射率随膜堆积密度的增加而增加,这是由于形成结晶铬和氧氮化钛膜而导致的,随着靶功率的增加,沉积速率逐渐提高。

著录项

  • 来源
    《Applied Surface Science》 |2011年第21期|p.8755-8761|共7页
  • 作者单位

    Centre of Nanotechnology, Indian Institute of Technology Roorkee, Roorkee 247667, India,Nano Science Laboratory, Institute Instrumentation Centre, Indian Institute of Technology Roorkee, Roorkee 247667, India;

    Nano Science Laboratory, Institute Instrumentation Centre, Indian Institute of Technology Roorkee, Roorkee 247667, India;

    Centre of Nanotechnology, Indian Institute of Technology Roorkee, Roorkee 247667, India,Department of Metallurgical and Materials Engineering, Indian Institute of Technology Roorkee, Roorkee 247667, India;

    Centre of Nanotechnology, Indian Institute of Technology Roorkee, Roorkee 247667, India,Nano Science Laboratory, Institute Instrumentation Centre, Indian Institute of Technology Roorkee, Roorkee 247667, India;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

    chromium oxynitride; titanium oxynitride; co-sputtering; stress; strain; contact angle; optical properties;

    机译:氧氮化铬;氧氮化钛;共溅射;应力;应变;接触角;光学性能;
  • 入库时间 2022-08-18 03:07:07

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