The three independent single-crystal elastic-stiffness constants
C<
sub>
ijsub> of cubic γ′-Fe<
sub>4
sub>N (face-centred cubic (fcc)-type
iron substructure) have been calculated by first-principles methods using the density functional theory:
C<
sub>11
sub> = 307.2 GPa,
C<
sub>12
sub> = 134.1 GPa and
C<
sub>44
sub> = 46.0 GPa. The Zener elastic-anisotropy ratio,
A = 2
C<
sub>44
sub>/(
C<
sub>11
sub> −
C<
sub>12
sub>) = 0.53, is strikingly less than 1, implying
direct.com/sci
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direct.com/sci
dirimg/entities/232a.gif" alt="right-pointing angle bracket" border=0> as stiffest
directions, whereas all fcc metals show
A > 1. This elastic anisotropy is ascribed to the ordered
distribution of N on the octahedral interstitial
sites. X-ray
diffraction lattice-strain measurements for a set of
different
h k l reflections recorded from γ′-Fe<
sub>4
sub>N<
sub>1−
ysub> layers on top of α-Fe confirmed the “abnormal” elastic anisotropy of γ′-Fe<
sub>4
sub>N<
sub>1−
ysub>. Stress evaluation, yiel
ding a compressive stress of about −670 MPa parallel to the surface, was performed on the basis of effective X-ray elastic constants determined from the calculated single-crystal elastic constants
C<
sub>
ijsub> and allowing a grain interaction interme
diate between the Reuss and the Voigt
models.