The aim of the study was to find whether the basic phenomena that occur dur
ing the glow discharge assisted nitriding of metal differ from those occurr
ing during gaseous nitriding. To define the specificity of a glow discharge
assistance a simple model system such as an iron cathode nitrided in d.c.
glow discharge in nitrogen at a low temperature was examined. The Fe4N laye
r of thickness 0.8 mum and 1.5 mum was produced in 5 h at 275 degreesC and
3 h at 350 degreesC, respectively. The results were compared with experimen
tal data of gaseous nitriding and computer aided simulations based on the L
ehrer (NH3-H-2)(1.5)(Fe-N) equilibrium diagram. The thickness of the Fe4N l
ayer produced in our experiment was greater than the thickness of the Fe4N
layer produced in the gaseous process observed experimentally and as the es
timated values from the model based on the equilibrium diagram, in spite of
the fact that the total number of N atoms in the gaseous process was 40 di
vided by 80 times greater than in the glow discharge assisted process. Base
d on the relation DeltaN = k root Dt we proposed that the difference betwee
n the gaseous nitriding process and the glow discharge assisted nitriding p
rocess results from the difference in the values of k, which in turn depend
on the N level at the diffusion front. The higher N level can be explained
in terms of a shallow ion implantation. (C) 2001 Elsevier Science B.V. All
rights reserved.