欢迎登录材料期刊网

材料期刊网

高级检索

介绍了一种新型的在钢铁基体上制备氮化钽薄膜的方法 --网状阴极法.其设备简单、价格低廉.实验中发现,在各个参数配比合适的条件下,可制备出结构为fcc(面心立方)和hex(密排六方)的氮化钽薄膜.薄膜较致密且均匀,与基体的结合好 .同时分析了在最佳工艺参数条件下合成氮化钽膜的成分、组织、表面、断口形貌和结合力等.该方法为氮化钽薄膜作为结构材料使用提供了一种新的途径.

参考文献

[1] Moody N R;Strojny A;Medlin D L et al.Substrate composition e ffects on the interfacial fravture of tantalum nitride films[J].Journal of Materials Research,1999,14(06):2306-2313.
[2] Kang Y K;Lee C M;Lee .G Effects of processing variab le on the mechanical properties of Ta/TaN multi player coatings[J].Material Science and Engineering,2000,B75:17-23.
[3] Gerstenberg D;Calbick C J .Effect of nitrogenmethane and oxyg en on str-ucture and electrical properties of thin solid film[J].Journal of Applied Physics,1964,35:402-407.
[4] K. Radhakrishnan ; N. Geok ing .Reactive sputter deposition and characterization of tantalum nitride thin films[J].Materials Science & Engineering, A. Structural Materials: Properties, Misrostructure and Processing,1999(3):224-227.
[5] Stavrev M.;Wenzel C.;Drescher K.;Mattern N.;Fischer D. .CRYSTALLOGRAPHIC AND MORPHOLOGICAL CHARACTERIZATION OF REACTIVELY SPUTTERED TA, TA-N AND TA-N-O THIN FILMS[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,1997(1/2):79-88.
[6] Massalski T B .Binary Alloy Phase Diagrams[J].The Materials Informa tion Society Materials Park OH,1990,3:2703-2704.
[7] 张庆瑜;陈斌;王敏 等.TaN薄膜的结构、成分及性能[J].大连理工大学学报,1995,35(04):482-485.
[8] Volz K;Kiuchi M;Ensinger W .Tantalum nitride films formed by ion beam assisted deposition:analysis of the structure in dependence on the ion irradiat ion intensity[J].Surface and Coatings Technology,2001,128-129:298-302.
[9] 杨春生;章吉良;赵小林.溅射钽薄膜内应力[J].微细加工技术,1994(04):60-63.
[10] P. Andersen;M. Moske;K. Dyrbye;J. Bottiger .Stress formation and relaxation in amorphous Ta-Cr films[J].Thin Solid Films: An International Journal on the Science and Technology of Thin and Thick Films,1999(1/2):205-209.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%