Structural Dynamics in Nanostructured Systems Probed by Ultrafast Convergent Electron Beam Diffraction

2021 ◽  
Author(s):  
Nora Bach ◽  
1989 ◽  
Vol 163 ◽  
Author(s):  
Yoshihisa Fujisaki ◽  
Shigeo Goto

AbstractSurface structure of (NH4)2S treated GaAs. is investigated using PL (PhotoLuminescence), XPS (X-ray Photoelectron Spectroscopy) and RHEED (Reflection of High Energy Electron beam Diffraction). The data taken with these techniques show the strong dependence upon the crystal orientations coming from the stabilities of chemical bonds of Ga-S and As-S on GaAs crystals. The greater enhancement of PL intensity, the clearer RHEED patterns and the smaller amount of oxides on (111)A than (111)B implies the realization of a more stable structure composed mainly of the Ga-S chemical bond.


2008 ◽  
Author(s):  
T. A. Grishina ◽  
O. D. Potapkin ◽  
M. A. Zaporogez

1992 ◽  
Vol 8-9 (1-6) ◽  
pp. 555-563
Author(s):  
Y.G. NAKAGAWA ◽  
H. YOSHIZAWA ◽  
T. UMEMOTO ◽  
C. FUKUOKA ◽  
M.E. LAPIDES

Author(s):  
R. Vincent ◽  
J.W. Steeds

Electron-beam welds in the Ni-base superalloy, Inconel 718 are freauently found to contain an extensive system of micro-cracks radiating from the weld boundary into the heat-affected zone (HAZ) of the matrix. To study precipitation in cross-sections of weld samples* over a large area adjacent to the weld, extraction replicas were prepared from the electro-polished and etched surfaces. Some preliminary identification of the extracted particles has been made by EDX analysis and convergent-beam diffraction, combined with scanning microscopy and EDX analysis of the electro-polished or ion-eroded surfaces. The welds are 1 cm deep, and near the top surface, where most of the long U+2018cracks’ occur (Fig.1a), the weld is 1.5 mm wide. The FAZ, as defined by a suitable etchant (10% HC1-methanol), extends for a further 1mm on each side. The grain size (50-100μm) is unchanged across the matrix-FAZ boundary. EDX spectra from the large precipitates (2-10μm) in the matrix and HAZ (Fig.la) show a strong Mb peak coupled with a weak Ti peak; the other alloy elements are entirely absent. Additional evidence from convergent-beam diffraction patterns (Fig.3) and measurement of the lattice constant2 (ao = 4.42 + 0.015 Å), proves that the majority of the particles are carbides, (Nb,Ti)C, with a F-centred cubic structure. These precipitates are absent from the weld, and the backbone of the dendritic weld precipitation is formed by thin, branched platelets (Fig.4). These are also carbides, (Nb,Ti)C, which recrystal 1ize from the melt. However, the FDX snectra now show weak additional peaks from most of the alloy elements (Ni, Cr, Fe, Mo).


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