Magnetic and structural properties of ion nitrided stainless steel

被引:33
作者
Basso, R. L. O. [1 ,2 ]
Pimentel, V. L. [3 ]
Weber, S. [4 ]
Marcos, G. [5 ,6 ]
Czerwiec, T. [5 ,6 ]
Baumvol, I. J. R. [1 ,7 ]
Figueroa, C. A. [1 ]
机构
[1] Univ Caxias do Sul, Ctr Ciencias Exatas & Tecnol, BR-95070560 Caxias Do Sul, RS, Brazil
[2] Inst Fis Gleb Wataghin, BR-13083970 Campinas, SP, Brazil
[3] Lab Nacl Luz Sincrotron, BR-13084971 Campinas, SP, Brazil
[4] Ecole Mines, Phys Mat Lab, CNRS, UMR 7556, F-54042 Nancy, France
[5] CNRS, UMR 7570, Lab Sci & Genie Surfaces, F-75700 Paris, France
[6] Ecole Mines, Inst Natl Polytech Lorraine, F-54042 Nancy, France
[7] Univ Fed Rio Grande do Sul, Inst Fis, BR-91509970 Porto Alegre, RS, Brazil
关键词
LOW-ENERGY; ELECTRONIC-STRUCTURE; EXPANDED AUSTENITE; METAL-ALLOYS; IMPLANTATION; FE; TEMPERATURES; MOSSBAUER;
D O I
10.1063/1.3153945
中图分类号
O59 [应用物理学];
学科分类号
摘要
The magnetic properties and crystalline structure of expanded austenite obtained by ion beam nitriding of AISI 316 steel are investigated. Magnetic force microscopy reveals that the nitrogen expanded austenite has two different layers, an outermost ferromagnetic layer and a paramagnetic layer beneath it. Superimposing the nitrogen concentration profile determined by secondary neutral mass spectrometry and the magnetic force microscopy image, one can see that the paramagnetic-ferromagnetic transition takes place at the inflection point of the nitrogen concentration profile at about 14 +/- 2 N at. %. Conventional and glancing angle x-ray diffraction suggests that nitrogen could occupy first tetrahedral interstitial positions (nitrogen-poor paramagnetic phase) and then, after saturation of Cr traps, octahedral interstitial positions (nitrogen-rich ferromagnetic phase). The ferromagnetic-paramagnetic transition is seen to be governed by Cr (traps)-N interactions. (C) 2009 American Institute of Physics. [DOI: 10.1063/1.3153945]
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页数:5
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