Characterization of Amorphous Oxide Nano-Thick Layers on 316L Stainless Steel by Electron Channeling Contrast Imaging and Electron Backscatter Diffraction

2016 ◽  
Vol 22 (5) ◽  
pp. 997-1006 ◽  
Author(s):  
Mahrokh Dorri ◽  
Stéphane Turgeon ◽  
Nicolas Brodusch ◽  
Maxime Cloutier ◽  
Pascale Chevallier ◽  
...  

AbstractCharacterization of the topmost surface of biomaterials is crucial to understanding their properties and interactions with the local environment. In this study, the oxide layer microstructure of plasma-modified 316L stainless steel (SS316L) samples was analyzed by a combination of electron backscatter diffraction and electron channeling contrast imaging using low-energy incident electrons. Both techniques allowed clear identification of a nano-thick amorphous oxide layer, on top of the polycrystalline substrate, for the plasma-modified samples. A methodology was developed using Monte Carlo simulations combined with the experimental results to estimate thickness of the amorphous layer for different surface conditions. X-ray photoelectron spectroscopy depth profiles were used to validate these estimations.

2005 ◽  
Vol 892 ◽  
Author(s):  
Carol Trager-Cowan ◽  
Francis Sweeney ◽  
A J Wilkinson ◽  
P W Trimby ◽  
A. P. Day ◽  
...  

2014 ◽  
Vol 783-786 ◽  
pp. 750-754
Author(s):  
Iván Gutierrez-Urrutia ◽  
Dierk Raabe

We have investigated the formation of dislocation substructures in high-Mn steels by electron channeling contrast imaging in the SEM. The coupling of electron channeling contrast imaging (ECCI) with electron backscatter diffraction (EBSD) provides an efficient and fast approach to characterize dislocation substructures under controlled diffraction conditions with enhanced contrast. The dislocation substructure of high-Mn steels at intermediate strain levels is characterized by cells and cell blocks with strong crystallographic orientation dependence. We observe a significant effect of strain path on dislocation patterning. Microband formation is enabled under shearing conditions. We explain this effect on terms of Schmid’s law.


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