Insight into segregation sites for oxygen impurities at grain boundaries in silicon

Author(s):  
Yutaka Ohno ◽  
Jie Ren ◽  
Shingo Tanaka ◽  
Masanori Kohyama ◽  
Koji Inoue ◽  
...  
2017 ◽  
Vol 130 ◽  
pp. 268-281 ◽  
Author(s):  
S. Chandra ◽  
N. Naveen Kumar ◽  
M.K. Samal ◽  
V.M. Chavan ◽  
S. Raghunathan

iScience ◽  
2019 ◽  
Vol 16 ◽  
pp. 390-398 ◽  
Author(s):  
Lirong Wang ◽  
Jinyan Cai ◽  
Yangcenzi Xie ◽  
Jiasheng Guo ◽  
Lingxiao Xu ◽  
...  

2019 ◽  
Author(s):  
Hayden Nunley ◽  
Mikiko Nagashima ◽  
Kamirah Martin ◽  
Alcides Lorenzo Gonzalez ◽  
Sachihiro C. Suzuki ◽  
...  

ABSTRACTThe outer epithelial layer of zebrafish retinae contains a crystalline array of cone photoreceptors, called the cone mosaic. As this mosaic grows by mitotic addition of new photoreceptors at the rim of the hemispheric retina, topological defects, called “Y-Junctions”, form to maintain approximately constant cell spacing. The generation of topological defects due to growth on a curved surface is a distinct feature of the cone mosaic not seen in other well-studied biological patterns like the R8 photoreceptor array in the Drosophila compound eye. Since defects can provide insight into cell-cell interactions responsible for pattern formation, we characterize the arrangement of cones in individual Y-Junction cores as well as the spatial distribution of Y-junctions across entire retinae. We find that for individual Y-junctions, the distribution of cones near the core corresponds closely to structures observed in physical crystals. In addition, Y-Junctions are organized into lines, called grain boundaries, from the retinal center to the periphery. In physical crystals, regardless of the initial distribution of defects, grain boundaries can form via the mobility of individual particles. By imaging in live fish, we demonstrate that grain boundaries in the cone mosaic instead appear during initial mosaic formation, without requiring defect motion. Motivated by this observation, we show that a computational model of repulsive cell-cell interactions generates a mosaic with grain boundaries. In contrast to paradigmatic models of fate specification in mostly motionless cell packings, this study emphasizes the role of cell motion, guided by cell-cell interactions during differentiation, in forming biological crystals. Such a route to the formation of regular patterns may be especially valuable in situations, like growth on a curved surface, where long-ranged, elastic, effective interactions between defects can help to group them into grain boundaries.AUTHOR SUMMARYFrom hair cells in the mammalian inner ear to the bristles on a fly’s back, sensory cells often form precise arrays, ensuring that these cells are evenly spread out on the tissue’s surface. Here we consider the zebrafish cone mosaic, a crystal of cone photoreceptors in the outer retinal layer. Because the cone mosaic grows from the rim of the curved retinal surface, new rows of cones (i.e., defects) are inserted to maintain constant spacing between sensory cells. We study the spatial distribution of these defects to gain insight into how the cone pattern forms. By imaging retinae in live fish, we find that as differentiating cones are incorporated into the mosaic, defects form lines (grain boundaries) that separate mostly defect-free domains. Then, we show that a computational model based on repulsion between mobile cells during their incorporation into the mosaic generates similar grain boundaries. This study thus suggests that cell motion governed by repulsive cell-cell interactions can play an important role in establishing regular patterns in living systems.


Author(s):  
Blas P. Uberuaga ◽  
Pauline Simonnin ◽  
Kevin M. Rosso ◽  
Daniel K. Schreiber ◽  
Mark Asta

AbstractMass transport along grain boundaries in alloys depends not only on the atomic structure of the boundary, but also its chemical make-up. In this work, we use molecular dynamics to examine the effect of Cr alloying on interstitial and vacancy-mediated transport at a variety of grain boundaries in Ni. We find that, in general, Cr tends to reduce the rate of mass transport, an effect which is greatest for interstitials at pure tilt boundaries. However, there are special scenarios in which it can greatly enhance atomic mobility. Cr tends to migrate faster than Ni, though again this depends on the structure of the grain boundary. Further, grain boundary mobility, which is sometimes pronounced for pure Ni grain boundaries, is eliminated on the time scales of our simulations when Cr is present. We conclude that the enhanced transport and grain boundary mobility often seen in this system in experimental studies is the result of non-equilibrium effects and is not intrinsic to the alloyed grain boundary. These results provide new insight into the role of grain boundary alloying on transport that can help in the interpretation of experimental results and the development of predictive models of materials evolution.


RSC Advances ◽  
2017 ◽  
Vol 7 (14) ◽  
pp. 8589-8597 ◽  
Author(s):  
Binbin Bao ◽  
Jinglei Liu ◽  
Hong Xu ◽  
Bo Liu ◽  
Kai Zhang ◽  
...  

A MnCr2O4 spinel coating initially forms at grain boundaries under a H2–H2O gas mixture at high temperature.


2000 ◽  
Vol 48 (14) ◽  
pp. 3623-3632 ◽  
Author(s):  
D.I. Thomson ◽  
V. Heine ◽  
M.C. Payne ◽  
N. Marzari ◽  
M.W. Finnis

1996 ◽  
Vol 460 ◽  
Author(s):  
Shanthi Subramanian ◽  
David A. Muller ◽  
John Silcox ◽  
Stephen. L. Sass

ABSTRACTTo obtain insight into the effect of dopants on the bonding and cohesive energy of gram boundaries in Ll2 intermetallic compounds, the chemistry and electronic structure at grain boundaries in B-free and B-doped Ni-23 at % Si alloys were examined, with electron energy loss spectroscopy (EELS) providing information on the former and energy dispersive X-ray spectroscopy (EDX) on the latter. Ni-enrichment was seen at large angle boundaries, both in the absence and presence of B. EELS of the Ni L3 edge showed that the bonding at Ni-rich grain boundaries was similar in both undoped and doped alloys. Comparison of the Ni L3 edge recorded at the grain boundary and in the bulk suggests that reduced hybridization and weaker bonding occurs at Ni-rich grain boundaries in both doped and undoped alloys. These changes in bonding are interpreted in terms of changes in the cohesive energy of the boundaries.


1997 ◽  
Vol 3 (S2) ◽  
pp. 657-658
Author(s):  
N. D. Browning ◽  
J. P. Buban ◽  
C. Prouteau ◽  
G. Duscher ◽  
M. F. Chisholm ◽  
...  

The short coherence length in high-Tc superconductors (5-15Å) makes an atomic scale understanding of the electronic properties at defects and interfaces essential for device applications. This understanding is particularly relevant for grain boundaries in YBa2CU3O7-δ (YBCO), where although extensive studies have shown a clear exponential decrease in critical current with misorientation angle, the absolute value can vary by several orders of magnitude at any given misorientation angle.Figure 1 shows Z-contrast images of an [001] low-angle tilt boundary and a 30° [001] asymmetric tilt grain boundary. An interesting feature of both of these boundaries is that there appear to be sites where two atom columns are too close together. However, the problem of like-ion repulsion can be avoided if the columns are taken to be partially occupied. Insight into the effect of this partial occupancy can be obtained through the use of bond-valence sum analysis. Here, the formal valence of an atom is made up of contributions from all of its nearest neighbors, the magnitude of which are determined by the bond length.


Nano Research ◽  
2019 ◽  
Vol 12 (5) ◽  
pp. 1099-1104 ◽  
Author(s):  
Lulu Zhao ◽  
Lei Li ◽  
Huaping Sheng ◽  
He Zheng ◽  
Shuangfeng Jia ◽  
...  

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