Wüest M. 51 Wykes M. 82 Yamaguchi M. 17 Ybarra G. 129 Yubero F ...
Wüest M. 51 Wykes M. 82 Yamaguchi M. 17 Ybarra G. 129 Yubero F ...
Wüest M. 51 Wykes M. 82 Yamaguchi M. 17 Ybarra G. 129 Yubero F ...
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JUNE 28 WEDNESDAY AFTERNOON<br />
JS1-WeA-P.1 γ N -SHIFTING AS A FUNCTION OF N 2 CONTENT IN AISI 304 NI-<br />
TRIDING. R. Valencia-Alvarado a , A. de la Piedad-Beneitez , J. de la Rosa-Vázquez , R. López-<br />
Callejas , S. R. Barocio , O. G. Godoy-Cabrera , A. Mercado-Cabrera , R. Peña-Eguiluz and A.<br />
E. Muñoz-Castro. Instituto Nacional de Investigaciones Nucleares, Plasma Physics Laboratory, A<br />
P. 18-1027, 11801 México, D.F. Instituto Tecnológico de Toluca, AP 890, Toluca, México. Instituto<br />
Politécnico Nacional, ESIME, 07738, México, D.F. a E-mail: rva@nuclear.inin.mx<br />
We present in this work some experimental results obtained from nitriding AISI 304 stainless steel at<br />
different temperatures by means of RF/DC generated 10 15 -10 16 m -3 density plasmas in the 1-4 eV<br />
temperature range. The samples were biased up to –500 V. Substrate temperatures proof to be an<br />
influential factor in the diffusion of the impinging ions into the material under treatment. In turn,<br />
this temperature during the expanded γ N shift, is a function of the amount of nitrogen introduced to<br />
the sample given by the bias, the depth of the nitrided layer and the plasma characteristics. Thus, we<br />
have chosen the substrate temperature as a global control variable in order to analyze the evolution<br />
of the nitrogen enrichment process through its influence on the X ray diffraction imaging of the γ N<br />
shift in the samples. The optimization of the temperature is explored along with its limits in terms of<br />
the Cr precipitation threshold.<br />
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