Austenite
Thin films: changed fcc to FCC to align with the rest of the page and general usage otherwise, missed a second one
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=== Thin films === |
=== Thin films === |
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Austenite is only stable above {{convert|910|C|abbr=on}} in bulk metal form. However, |
Austenite is only stable above {{convert|910|C|abbr=on}} in bulk metal form. However, FCC transition metals can be grown on a [[Cubic crystal system#Bravais lattices|face-centered cubic]] (FCC) or [[diamond cubic]].{{cite journal |vauthors=Hoff HA, Waytena GL, Glesener JW, Harris VG, Pappas DP |title=Critical thickness of single crystal fcc iron on diamond |journal=Surf Sci |date=Mar 1995 |volume=326 |issue=3 |pages=252–66 |doi=10.1016/0039-6028(94)00787-X |bibcode = 1995SurSc.326..252H |s2cid=93826286 }} The epitaxial growth of austenite on the diamond (100) face is feasible because of the close lattice match and the symmetry of the diamond (100) face is fcc. More than a monolayer of γ-iron can be grown because the critical thickness for the strained multilayer is greater than a monolayer. The determined critical thickness is in close agreement with theoretical prediction. |
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==Transformation and Curie point== |
==Transformation and Curie point== |
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