欢迎访问沈阳真空杂志社 Email Alert    RSS服务

真空 ›› 2020, Vol. 57 ›› Issue (1): 26-30.doi: 10.13385/j.cnki.vacuum.2020.01.05

• • 上一篇    下一篇

射频功率占比对氮掺杂二氧化钛薄膜性能的影响

胡家培1,2, 张华1, 徐惠民1, 曹强1, 唐超3, 刘旭杰1, 李炎峰1   

  1. 1.安徽科技学院 机械工程学院,安徽 凤阳 233100;
    2.五河县职业技术学校,安徽 蚌埠 233300;
    3.神龙汽车有限公司,武汉 湖北 430000
  • 收稿日期:2019-04-25 出版日期:2020-01-25 发布日期:2020-03-17
  • 通讯作者: 张华,博士,教授。
  • 作者简介:胡家培(1989-),男,安徽省六安市人,硕士生。

Effect of RF Power Ratio on Properties of Nitrogen-Doped TiO2 Film

HU Jia-pei1,2, ZHANG Hua1, XU Hui-min1, CAO Qiang1, TANG Chao3, LIU Xu-jie1, LI Yan-feng1   

  1. 1.College of Mechanical Engineering, Anhui University of Science and Technology, Fengyang 233100, China;
    2.Wuhe County Vocational and Technical School, Bengbu 233300, China;
    3.Dongfeng Peugeot Citroen Automobile Company Ltd, Wuhan 430000, China
  • Received:2019-04-25 Online:2020-01-25 Published:2020-03-17

摘要: 本研究主要利用射频耦合直流磁控溅射技术,在室温下用TiO2陶瓷靶在玻璃基底上制备N掺杂到TiO2薄膜。同时也利用光学轮廓仪、X射线衍射、扫描电子显微镜、X射线光电子能谱和紫外可见光分光光度计研究了不同射频功率占比对薄膜的微观结构和光学性能的影响。实验结果表明:随着射频功率的增加,薄膜的沉积速率增加,薄膜的结晶性变优,晶粒尺寸变大,N掺入的比例增加,Ti的价态出现未完全氧化的Ti3+,薄膜的禁带宽度也相应地减小,N掺杂TiO2薄膜的吸收边扩展到可见光区域。

关键词: TiO2薄膜, 射频功率占比, 直流耦合

Abstract: This study mainly used RF coupled DC magnetron sputtering technology to prepare N-doped TiO2 thin films on glass substrates at room temperature with TiO2 ceramic targets. At the same time, the effects of different RF power ratios on the microstructure and optical properties of the films were investigated by optical profilometry, X-ray diffraction, scanning electron microscopy, X-ray photoelectron spectroscopy and UV-visible spectrophotometer. The experimental results show that, with the increase of RF power, the deposition rate of the film increases, the crystallinity of the film becomes better, the grain size becomes larger, the proportion of N doping increases, and the valence state of Ti shows incompletely oxidized Ti3+. The forbidden band width is also correspondingly reduced, and the absorption edge of the N-doped TiO2 film is extended to the visible light region.

Key words: TiO2 film, RF power ratio, DC coupling

中图分类号: 

  • TB34
[1] Grigorov K G, Oliveira I C, Maciel H S, et al.Cunha, Optical and morphological properties of N-doped TiO2 thin films[J]. Surf, Sci., 2011, 605(7-8): 775-782.
[2] Cabrera R Q, Vazquez C S, Darr J A, et al.Critical influence of surface nitrogen species on the activity of N-doped TiO2 thin-films during photodegradation of stearic acid under UV light irradiation[J]. Appl. Catal. B Environ. 2014, (160-161): 582-588.
[3] Zhang J, Fu W, Xi J H, et al.N-doped rutile TiO2 nano-rods show tunable photocatalytic selectivity[J]. J. Alloy. Compd, 2013, 575: 40-47.
[4] Baker M A, Fakhouri H, Grilli R, et al.F. Arefi-Khonsari, Effect of total gas pressure and O2/N2 flow rate on the nanostructure of N-doped TiO2 thin films deposited by reactive sputtering[J]. Thin Solid Films, 2014, 552: 10-17.
[5] Guillen C, Montero J, Herrero J.Influence of N-doping and air annealing on the structural and optical properties of TiO2 thin films deposited by reactive DC sputtering at room temperature[J]. J. Alloy. Compd, 2015, 647: 498-506.
[6] Liu H L, Yao T T, Ding W Y, et al.Study on the optical property and surface morphology of N doped TiO2 film deposited with different N2 flow rates by DCPMS[J]. J. Environ. Sci., 2013, 25: 54-58.
[7] Fujishima A, Honda K.Electrochemical photolysis of water at a semiconductor electrode[J]. Nature, 1992, 238(5358):37-38.
[8] Yamaki T, Sumita T, Yamamoto S.Formation of TiO2-xFx compounds in fluorine-implanted TiO2[J]. J. Mater. Sci, 2002,(21): 33-35.
[9] Umebayashi T, Yamaki T, Itoh H, et al.Band gap narrowing of titanium dioxide by sulfur doping[J]. Appl. Phys. Lett, 2002(81): 454-456.
[10] Lee S H, Yamasue E, Okumura H, et al.Effect of substrate roughness and working pressure on photocatalyst of N-doped TiOx films prepared by reactive sputtering with air[J]. Appl. Sur. Sci, 2015(324): 339-348.
[11] Asahi R, Morikawa T, Ohwaki T, et al.Visible-light photocatalysis in nitrogen-doped titanium oxides[J]. Science, 2001(293): 269-271.
[12] 梅乐夫, 梁开明. 氮掺杂TiO2薄膜光催化剂的制备[J]. 稀有金属材料与工程, 2009(38): 644-646.
[13] 丁万昱, 王华林, 巨英东, 等. O2流量对磁控溅射N掺杂TiO2薄膜成分及晶体结构的影响[J]. 物理学报, 2011, 60(2): 728-735.
[14] Migita T, Kamei R, Tanaka T, et al.Effect of dc bias on the compositional ratio of WNx thin films prepared by rf-dc coupled magnetron sputtering[J]. Appl. Surf. Sci. 2012, (169-170): 362-365.
[15] Ding W Y, Xu J, Lu W Q, et al.The effect of N2 flow rate on discharge characteristics of microwave electron cyclotron resonance plasma[J]. Phys. Plasmas, 2009(16): 053502-053506.
[16] Liu B S, Wen L P, Zhao X J.The structure and photocatalytic studies of N doped TiO2 films prepared by radio frequency reactive magnetron sputtering[J]. Sol. Energy Mat. Sol. C, 2008(92):1-10.
[17] Wolff M, Schultze J W, Strehblow H H.Low-energy implantation and sputtering of TiO2 by nitrogen and argon and the electrochemical reoxidation[J]. Surf. Interf. Anal, 1991(17): 726-736.
[18] Saha N C, Tompkins H G.Titanium nitride oxidation chemistry:an xeray photoelectron spectroscopy study[J]. J. Appl. Phys, 1992(72): 3072-3079.
[19] Irie H, Watanabe Y, Hashimoto K.Nitrogen-concentration dependence on photocatalytic activity of TiO2-xNx powders[J]. J. Phys. Chem. B, 2003(107): 5483-5486.
[20] Ryoji A, Takeshi M, Hiroshi I.Nitrogen-doped titanium dioxide as visible-light-sensitive photocatalyst:designs, developments, and prospects[J]. Chem. Rev., 2014(114):9824-9852.
[21] Hagfeld A, Gratzel M.Light-induced redox reactions in nanocrystalline systems[J]. Chem. Rev, 1995(95): 49-68.
[22] 徐凌, 唐超群, 戴磊, 等, N掺杂锐钛矿TiO2电子结构的第一性原理研究[J]. 物理学报, 2007, 56(2): 1048-1053.
[23] 彭丽萍, 徐凌, 尹建武. N掺杂锐钛矿TiO2光学性能的第一性原理研究[J]. 物理学报, 2007, 56(3): 1585-1589.
[1] 仲召进 , 曹 欣 , 高 强 , 韩 娜 , 崔介东 , 石丽芬 , 姚婷婷 , 马立云, 彭 寿. 射频溅射功率对室温沉积 AZO 薄膜性能的影响[J]. 真空, 2019, 56(1): 45-48.
[2] 张子欣, 刘忠伟, 杨丽珍, 陈强. 等离子体辅助原子层沉积技术包覆硅基氮化物荧光粉的结果性能研究[J]. 真空, 2019, 56(4): 19-23.
[3] 樊启鹏, 胡玉莲, 刘博文, 田旭, 江德荣, 刘忠伟. 等离子体增强原子层沉积技术制备碳化钴薄膜*[J]. 真空, 2019, 56(5): 56-60.
Viewed
Full text


Abstract

Cited

  Shared   
  Discussed   
[1] 李得天, 成永军, 张虎忠, 孙雯君, 王永军, 孙 健, 李 刚, 裴晓强. 碳纳米管场发射阴极制备及其应用研究[J]. 真空, 2018, 55(5): 1 -9 .
[2] 周彬彬, 张 建, 何剑锋, 董长昆. 基于 CVD 直接生长法的碳纳米管场发射阴极[J]. 真空, 2018, 55(5): 10 -14 .
[3] 李志胜. 空间环境下超大型红外定标用辐射屏蔽门的研制[J]. 真空, 2018, 55(5): 66 -70 .
[4] 郑 列, 李 宏. 200kV/2mA 连续可调直流高压发生器的设计[J]. 真空, 2018, 55(6): 10 -13 .
[5] 柴晓彤, 汪 亮, 王永庆, 刘明昆, 刘星洲, 干蜀毅. 基于 STM32F103 单片机的单泵运行参数数据采集系统[J]. 真空, 2018, 55(5): 15 -18 .
[6] 孙立志, 闫荣鑫, 李天野, 贾瑞金, 李 征, 孙立臣, 王 勇, 王 健, 张 强. 放样氙气在大型收集室内分布规律研究[J]. 真空, 2018, 55(5): 38 -41 .
[7] 黄 思 , 王学谦 , 莫宇石 , 张展发 , 应 冰 . 液环压缩机性能相似定律的实验研究[J]. 真空, 2018, 55(5): 42 -45 .
[8] 纪 明, 孙 亮, 杨敏勃. 一种用于对月球样品自动密封锁紧的设计[J]. 真空, 2018, 55(6): 24 -27 .
[9] 李民久, 熊 涛, 姜亚南, 贺岩斌, 陈庆川. 基于双管正激式变换器的金属表面去毛刺 20kV 高压脉冲电源[J]. 真空, 2018, 55(5): 19 -24 .
[10] 刘燕文, 孟宪展, 田 宏, 李 芬, 石文奇, 朱 虹, 谷 兵, 王小霞 . 空间行波管极高真空的获得与测量[J]. 真空, 2018, 55(5): 25 -28 .