外加磁场对纳米镍膜电磁屏蔽性能的影响
The Effect of External Magnetic Field on the Electromagnetic Shielding Performance of Nanometer Nickel Film
DOI: 10.12677/MP.2013.31007, PDF, HTML,  被引量 下载: 3,287  浏览: 10,037  国家科技经费支持
作者: 徐军军, 张海燕*, 曾国勋, 杨振大:广东工业大学材料与能源学院,广州
关键词: 磁控溅射金属镍薄膜屏蔽效能矫顽力Magnetron Sputtering; Nickel Films; Shielding Effectiveness; Coercive Force
摘要: 用磁控溅射在柔性衬底上制备金属镍纳米薄膜,研究了磁场对薄膜样品的形貌的影响,分析了在有无磁场条件下制备的薄膜样品的X衍射,饱和磁化强度和矫顽力以及在电磁波频段为3.95~5.85 GHz内的电磁屏蔽效果。结果表明,在磁场条件下的制备的薄膜样品要比无磁场条件下制备的薄膜的结晶性好;有外加磁场下制备的薄膜矫顽力为112.89 Oe,无外加磁场条件下制备的薄膜的矫顽力为14.82 Oe,外加磁场下制备的薄膜矫顽力要比无外加磁场条件下制备的薄膜的矫顽力增加7.6倍。磁场下生长的薄膜样品的屏蔽效果明显优于无磁场下薄膜的屏蔽效果,屏蔽效能平均值提高了30%。
Abstract: Nickel nanometer thin films were deposited by magnetron sputtering on flexible substrates, the impact of morphology of the film sample of magnetic field, under magnetic and no magnetic of film were investigated by X-ray diffraction. A comparison of their saturation magnetization and coercive force as well as in the electromagnetic spec-trum for 3.95 - 5.85 GHz electromagnetic shielding effect. The result show that, the film of crystallinity was deposited under magnetic field is better than this no magnetic, the coercivity of the film was prepared under magnetic field is 112.89 Oe, while be prepared under no magnetic field is 14.82 Oe; the film be prepared under an external magnetic field is as 7.6 times no magnetic. The shielding effect of film sample under magnetic field is obviously better than that of no magnetic field, the average increase of shielding effectiveness is 30%.
文章引用:徐军军, 张海燕, 曾国勋, 杨振大. 外加磁场对纳米镍膜电磁屏蔽性能的影响[J]. 现代物理, 2013, 3(1): 38-42. http://dx.doi.org/10.12677/MP.2013.31007

参考文献

[1] 赵福辰. 电磁屏蔽材料的发展现状[J]. 材料开发与虚用, 2001, 11(5): 29-33.
[2] Z. Zou, J. Ye, K. Sayama, et al. Direct splitting of water under visible light irradiation with an oxide semiconductor photocatalyst. Nature, 2001, 414(6864): 625-627.
[3] 邵寒梅, 官建国, 王一龙等. 电磁波屏蔽复合材料的研究进展[J]. 屏蔽技术与屏蔽材料, 2008, 10(1): 65-70.
[4] 常德龙, 邱帖轶, 王群有等. 木材磁控溅射镀膜金属试验[J].东北林业大学学报, 2007, 35(12): 34-36.
[5] X. Zhang, W. Liu. Controllable synthesis of nickel den-dritic crystals induced by magnetic field. Materials Research Bulletin, 2008, 43(8-9): 2100.
[6] J. Ye, Q. W. Chen and Y. Q. Zheng. Mag-netic properties of nickel film formed under magnetic fields. Journal of Physics D: Applied Physics, 2008, 41(20): 205011.
[7] H. Y. Wang, S. Mitani, M. Motokawa, et al. Effect of high mag- netic fields on the morphology of soft magnetic α’-FeN films. Journal of Applied Physics, 2003, 93(11): 9145-9150.
[8] H. Matsushima, T. Nohira, Y. Ito, et al. Magnetic field effects on the crystal orientation and surface morphol-ogy of electrodepos- ited iron films. Journal of Solid State Electro-chemistry, 2004, 8(3): 195-200.
[9] H.Matsushima, T. Nohira, Y. Ito, et al. Effects of magnetic fields on iron electrodeposition. Surface and Coatings Technology, 2004, 179(2-3): 245.
[10] J. Wang, K. Zhang, Z. M. Peng, et al. Magnetic properties improvement in Fe3O4 nanoparti-cles grown under magnetic fields. Journal of Crystal Growth, 2004, 266(4): 500.
[11] L. X. Sun, Q. W. Chen. Core-shell cylindrical mag-netic domains in nickel wires prepared under magnetic fields. The Journal of Physical Chemistry C, 2009, 113(7): 2710.
[12] L. X. Zhang, J. Luo and Q. W. Chen. Magnetic properties of assembled ferrite nanostructures induced by magnetic fields. Journal of Physics: Condensed Matter, 2005, 17(33): 5095.
[13] M. Z. Wu, Y. Xiong, Y. S. Jia, et al. Magnetic field-assisted hydrothermal growth of chain-like nanostructure of magnetite. Chemical Physics Letters, 2005, 40l(4-6): 374-379.
[14] M. S. Chen, Z. X. Shen, X. Y. Liu, et al. Raman and magnetization studies of barium ferrite powder prepared by wa-ter-in-oil microemulsion. Journal of Materials Research, 2000, 15(2): 483.