laue microdiffraction
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2021 ◽  
Vol 60 (SB) ◽  
pp. SBBC02
Author(s):  
M. Murugesan ◽  
Y. Susumago ◽  
K. Sumitani ◽  
Y. Imai ◽  
S. Kimura ◽  
...  

Nano Select ◽  
2020 ◽  
Author(s):  
Florian Lauraux ◽  
Sarah Yehya ◽  
Stéphane Labat ◽  
Jean‐Sébastien Micha ◽  
Odile Robach ◽  
...  

2020 ◽  
Vol 116 (24) ◽  
pp. 243101
Author(s):  
Z. Ren ◽  
T. W. Cornelius ◽  
C. Leclere ◽  
A. Davydok ◽  
J.-S. Micha ◽  
...  

Minerals ◽  
2020 ◽  
Vol 10 (3) ◽  
pp. 204
Author(s):  
Camelia Veronica Stan ◽  
Earl Francis O’Bannon ◽  
Pavel Mukhin ◽  
Nobumichi Tamura ◽  
Larissa Dobrzhinetskaya

Moissanite, SiC, is an uncommon accessory mineral that forms under low oxygen fugacity. Here, we analyze natural SiC from a Miocene tuff-sandstone using synchrotron Laue microdiffraction and Raman spectroscopy, in order to better understand the SiC phases and formation physics. The studied crystals of SiC consist of 4H- and 6H-SiC domains, formed from either, continuous growth or, in one case, intergrown, together with native Si. The native Si is polycrystalline, with a large crystal size relative to the analytical beam dimensions (>1–2 μm). We find that the intergrown region shows low distortion or dislocation density in SiC, but these features are comparatively high in Si. The distortion/deformation observed in Si may have been caused by a mismatch in the coefficients of thermal expansion of the two materials. Raman spectroscopic measurements are discussed in combination with our Laue microdiffraction results. Our results suggest that these SiC grains likely grew from an igneous melt.


Author(s):  
L. Deillon ◽  
S. Verheyden ◽  
D. Ferreira Sanchez ◽  
S. Van Petegem ◽  
H. Van Swygenhoven ◽  
...  

2019 ◽  
Vol 168 ◽  
pp. 210-221 ◽  
Author(s):  
Johan Hektor ◽  
Jean-Sébastien Micha ◽  
Stephen A. Hall ◽  
Srinivasan Iyengar ◽  
Matti Ristinmaa

2019 ◽  
Vol 3 (1) ◽  
pp. 6 ◽  
Author(s):  
Yubin Zhang ◽  
Rozaliya Barabash

Synchrotron 3D X-ray Laue microdiffraction, available at beamline 34-ID-E at Advanced Photon Source in Argonne National Laboratory, is a powerful tool for 3D non-destructive mapping of local orientations and strains at sub-micron scale in the bulk. With this technique, it is possible to study local residual stresses developed during manufacturing or while in service due to interactions between, for example, different phases and/or grains with different orientations in materials containing multiple or single phase(s). Such information is essential for understanding mechanical properties and designing advanced materials, but is largely non-existent in the current generation of materials models. In the present paper, the principle and experimental set-up of the 3D microdiffraction are introduced, followed by a description of a method for quantification of the local plastic deformation based on high-angular-resolution orientation maps. The quantification of local residual stresses in two model materials, ductile cast iron (two phases) and partially recrystallized pure nickel (single phase), using 3D microdiffraction will then be presented. The results show that 3D microdiffraction is important for understanding the origin of local residual stresses and to relate them to the microstructural evolution. Finally, the limitations of the 3D microdiffraction on the current generation synchrotron source and new possibilities after the synchrotron upgrade are discussed.


2018 ◽  
Vol 2 (11) ◽  
pp. 1161-1167
Author(s):  
Jordan G. Hamilton ◽  
Joel W. Reid ◽  
Renfei Feng ◽  
Derek Peak

2018 ◽  
Vol 74 (a1) ◽  
pp. a173-a173
Author(s):  
Camelia Stan ◽  
Earl O'Bannon ◽  
Larissa Dobrzhinetskaya ◽  
Nobumichi Tamura

Solid Earth ◽  
2018 ◽  
Vol 9 (2) ◽  
pp. 505-529
Author(s):  
Anne-Marie Boullier ◽  
Odile Robach ◽  
Benoît Ildefonse ◽  
Fabrice Barou ◽  
David Mainprice ◽  
...  

Abstract. During the last decade pulverized rocks have been described on outcrops along large active faults and attributed to damage related to a propagating seismic rupture front. Questions remain concerning the maximal lateral distance from the fault plane and maximal depth for dynamic damage to be imprinted in rocks. In order to document these questions, a representative core sample of granodiorite located 51.3 m from the Nojima fault (Japan) that was drilled after the Hyogo-ken Nanbu (Kobe) earthquake is studied by using electron backscattered diffraction (EBSD) and high-resolution X-ray Laue microdiffraction. Although located outside of the Nojima damage fault zone and macroscopically undeformed, the sample shows pervasive microfractures and local fragmentation. These features are attributed to the first stage of seismic activity along the Nojima fault characterized by laumontite as the main sealing mineral. EBSD mapping was used in order to characterize the crystallographic orientation and deformation microstructures in the sample, and X-ray microdiffraction was used to measure elastic strain and residual stresses on each point of the mapped quartz grain. Both methods give consistent results on the crystallographic orientation and show small and short wavelength misorientations associated with laumontite-sealed microfractures and alignments of tiny fluid inclusions. Deformation microstructures in quartz are symptomatic of the semi-brittle faulting regime, in which low-temperature brittle plastic deformation and stress-driven dissolution-deposition processes occur conjointly. This deformation occurred at a 3.7–11.1 km depth interval as indicated by the laumontite stability domain. Residual stresses are calculated from deviatoric elastic strain tensor measured using X-ray Laue microdiffraction using the Hooke's law. The modal value of the von Mises stress distribution is at 100 MPa and the mean at 141 MPa. Such stress values are comparable to the peak strength of a deformed granodiorite from the damage zone of the Nojima fault. This indicates that, although apparently and macroscopically undeformed, the sample is actually damaged. The homogeneously distributed microfracturing of quartz is the microscopically visible imprint of this damage and suggests that high stresses were stored in the whole sample and not only concentrated on some crystal defects. It is proposed that the high residual stresses are the sum of the stress fields associated with individual dislocations and dislocation microstructures. These stresses are interpreted to be originated from the dynamic damage related to the propagation of rupture fronts or seismic waves at a depth where confining pressure prevented pulverization. Actually, M6 to M7 earthquakes occurred during the Paleocene on the Nojima fault and are good candidates for inducing this dynamic damage. The high residual stresses and the deformation microstructures would have contributed to the widening of the damaged fault zone with additional large earthquakes occurring on the Nojima fault.


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