1979
DOI: 10.1080/01418617908239275
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Lattice imaging of faulted dipoles in silicon

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Cited by 42 publications
(5 citation statements)
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“…HRTEM has so far contributed mainly to studies of extended defects in semiconductors. Various types of extended defects, i.e., dislocations (Anstis et al, 1981;Chiang et al, 1980;Sato et al, 1980;Spence and Kolar, 1979), stacking fault tetrahedra (Coene et al, 1985), interfaces between two different semiconducting crystals (Ichinose et al, 1987;Ikarashi et al, 1994;Ourmazd et al, 1993), and grain boundaries (Bourret and Desseaux, 1979;Krivanek et al, 1977) have been examined in detail. They are to some extent similar to those in other materials such as metallic alloys, but characteristic in many cases; they exhibit the bond topology that is governed by the general nature of covalent bonding and occasionally different from the parent diamond lattice.…”
Section: Introductionmentioning
confidence: 99%
“…HRTEM has so far contributed mainly to studies of extended defects in semiconductors. Various types of extended defects, i.e., dislocations (Anstis et al, 1981;Chiang et al, 1980;Sato et al, 1980;Spence and Kolar, 1979), stacking fault tetrahedra (Coene et al, 1985), interfaces between two different semiconducting crystals (Ichinose et al, 1987;Ikarashi et al, 1994;Ourmazd et al, 1993), and grain boundaries (Bourret and Desseaux, 1979;Krivanek et al, 1977) have been examined in detail. They are to some extent similar to those in other materials such as metallic alloys, but characteristic in many cases; they exhibit the bond topology that is governed by the general nature of covalent bonding and occasionally different from the parent diamond lattice.…”
Section: Introductionmentioning
confidence: 99%
“…High resolution electron microscopy (HREM), in addition to scanning tunneling microscopy and Z-contrast imaging in scanning transmission electron microscopy, is a valuable technique which enables structural information on defects in real space to be ascertained on the atomic scale. The atomic arrangements in the vicinity of structural defects within semiconductors have been determined from projected end-on images [5][6][7][8][9]. To date, there have been several detailed quantitative reports of atom positions and displacements around such defects using HREM [10][11][12][13].…”
mentioning
confidence: 99%
“…Notably, two distinct defect structures are observed in the pure fcc domain near the domain boundary: the pure fcc domain in region R1 (Figure 4b) exhibits three intrinsic SFs (white arrows) with multiple SFs (yellow arrows) lying on the (111) planes parallel to the domain boundary, while the pure fcc domain in region R2 (Figure 4c) exhibits other SFs intersecting the intrinsic SFs at 70.5°, forming a Z‐shaped faulted dipole. [ 37,38 ] However, the interiors of the hcp domains (bottom) shown in the R1 and R2 regions are free of defects. Higher‐magnification TEM images (Figure 4d,e), obtained from the boxed regions denoted as M and N in Figure 4b,c demonstrate more clearly that dislocation cores [ 39 ] (cyan arrows in Figure 4e) in the Z‐shaped faulted dipole are formed at the intersections of the three intrinsic SFs 1 on the (111) plane and the one extrinsic SF 2 on the (−1−11) plane.…”
Section: Resultsmentioning
confidence: 99%