Atomic-scale simulations of multiple ion–solid interactions and structural evolution in silicon carbide

2002 ◽  
Vol 17 (2) ◽  
pp. 259-262 ◽  
Author(s):  
F. Gao ◽  
W. J. Weber

Molecular dynamics (MD) were employed in atomic-level simulations of fundamental damage production processes due to multiple ion–solid collision events in cubic SiC. Isolated collision cascades produce single interstitials, vacancies, antisite defects, and small defect clusters. As the number of cascades (or equivalent dose) increases, the concentration of defects increases, and the collision cascades begin to overlap. The coalescence of defects and clusters with increasing dose is an important mechanism leading to amorphization in SiC and is consistent with the homogeneous amorphization process observed experimentally in SiC. The driving force for the crystalline– amorphous (c–a) transition is the accumulation of both interstitials and antisite defects. High-resolution transmission electron microscopy (HRTEM) images of the defect accumulation process and loss of long-range order in the MD simulation cell are consistent with experimental HRTEM images and disorder measurements. Thus, the MD simulations provide atomic-level insights into the interpretation of experimentally observed features associated with multiple ion–solid collision events in SiC.

2005 ◽  
Vol 475-479 ◽  
pp. 1345-1350
Author(s):  
William J. Weber ◽  
Fei Gao ◽  
Ram Devanathan ◽  
Weilin Jiang ◽  
Y. Zhang

Atomic-level simulations are used to determine defect production, cascade-overlap effects, and defect migration energies in SiC. Energetic C and Si collision cascades primarily produce single interstitials, mono-vacancies, antisite defects, and small defect clusters, while amorphous clusters are produced within 25% of Au cascades. Cascade overlap results in defect stimulated cluster growth that drives the amorphization process. The good agreement of disordering behavior and changes in volume and elastic modulus obtained computationally and experimentally provides atomic-level interpretation of experimentally observed features. Simulations indicate that close-pair recombination activation energies range from 0.24 to 0.38 eV, and long-range migration energies for interstitials and vacancies are determined.


1994 ◽  
Vol 332 ◽  
Author(s):  
T. F. Kelly ◽  
P. P. Camus ◽  
D. J. Larson ◽  
L. M. Holzman

ABSTRACTMuch of the current activity and excitement in materials science involves processing and understanding materials at the atomic scale. Accordingly, it is necessary for materials scientists to control and characterize materials at the atomic level. There are only a few microscopies that are capable of providing information about the structure of materials at the atomic level: the atom probe field ion microscope, the high resolution transmission electron microscope, and the scanning tunneling microscope. The three-dimensional atom probe (3DAP) determines the 3D location and elemental identity of each atom in a sample. It is the only technique that provides 3D information at the atomic scale.The origin and underlying concepts behind the 3DAP are described. Several examples of actual images from existing 3DAPs are shown with emphasis on nanometer-scale analysis. Current limitations of the technique and expected future developments in this form of microscopy are described. It is our opinion that 3D atomic-scale imaging will be an indispensable tool in materials science in the coming decades.


Author(s):  
Robert C. Rau ◽  
Robert L. Ladd ◽  
John Moteff

Transmission electron microscopy has been used to study the microstructure of vanadium irradiated at reactor ambient temperature (∼ 70°C) to a fast (E > 1 MeV) neutron fluence of 5 x 1019 n/cm2. Observations were made of the as-irradiated material, and after one-hour vacuum annealing at various temperatures ranging from 330°C to 1175°C.In the as-irradiated condition, shown in Fig. 1, a very high density of small defect clusters was present. These clusters appeared as black dots averaging approximately 25-50 Å in diameter, and were estimated to be present in quantities of 1016 to 1017 per cm3. Post-irradiation annealing caused the clusters to increase in average size and decrease in number, as shown in Figs. 2 and 3, until after the highest temperature anneal, 1175°C, the cluster density was legs than 1014 per cm3 and the average cluster size was approximately 500Å. After annealing at temperatures of 510°C or above, many of the clusters were seen to be resolvable as dislocation loops. Tilting experiments indicated that these loops were probably interstitial in nature.


Coatings ◽  
2019 ◽  
Vol 9 (12) ◽  
pp. 785
Author(s):  
Deniz Karataş ◽  
Dilek Senol Arslan ◽  
Ilgin Kursun Unver ◽  
Orhan Ozdemir

The amenability of gold nanoparticles (AuNPs) coating on natural and modified (hexadecyl trimethyl ammonium bromide, CTAB) sepiolite surfaces was studied both experimentally and theoretically. The zeta potential experiments and Fourier transform infrared spectrophotometer (FTIR), environmental scanning electron microscope (ESEM), and transmission electron microscopy (TEM) analyses were carried out with the sepiolite samples in the presence of AuNPs. In addition, the adsorption of three gold-nanoparticles on the sepiolite surface (100) in the absence and presence of CTAB was investigated by molecular dynamics (MD) simulations. The AuNPs showed no significant change in the zeta potential of natural sepiolite surfaces due to negative charges of both the sepiolite and AuNPs at natural pH. The surface charge of modified sepiolite decreased with the increase in AuNPs concentration indicating the significance AuNPs adsorption. FTIR, ESEM, and TEM analyses indicated the coating of AuNPs onto the modified sepiolite surface were higher than that of the natural sepiolite surface. The MD simulation results showed that AuNPs can easily adsorb onto the basal surface of the sepiolite due to its hydrophilicity in the presence and absence of CTAB as indicated in the experimental studies. In short, the modification of sepiolite with CTAB made the charge positive, and in turn considerably increased the AuNPs coating on sepiolite surfaces due to electrostatic attraction.


2012 ◽  
Vol 602-604 ◽  
pp. 747-750
Author(s):  
Miao Zhang ◽  
Ping Yang

Epoxy resin is widely used in many electronic packages, the ability to predict properties of cross linked epoxy resin before experiments will facilitate the process of materials design. Molecular dynamics (MD) is a powerful method that can simulate the materials at atomic scale and it can be used to predict the performance and properties of a wide range of materials. In this work, the properties of the cross-linked epoxy resin compound at high temperature were studies by MD simulations. The relations of the glass transition temperature (Tg) and properties of the cross-linked epoxy resin were investigated. The results show that Tg can be estimated by the plot of non-bond energy at different temperatures, and consist with the experimental data.


2019 ◽  
Vol 49 (1) ◽  
Author(s):  
Na Yeon Kim

AbstractStructural evolution of copper oxide nanoparticles is examined, especially with respect to Ostwald ripening under electron beam irradiation. Dissolution of the smaller particles into the larger one was clearly observed at the atomic scale using advanced transmission electron microscope.


2000 ◽  
Vol 650 ◽  
Author(s):  
Fei Gao ◽  
William J. Weber

ABSTRACTMolecular dynamics (MD) simulations have been employed to study cascade overlap and defect accumulation processes during amorphization in 3C-SiC. A large number of 10 keV displacement cascades were randomly generated in a model crystal to achieve the amorphous state, and the corresponding dose is consistent with experimental observations. The results show that most defects are single interstitials and mono-vacancies at low dose, whereas the amorphous or disordered clusters, which consist of interstitials and antisite defects, appear at intermediate dose levels. These local disordered regions play an important role in the amorphization of SiC. At higher doses, a significant proportion of antisite defects is created during continued cascade overlap. The increase in interstitials and antisite defects with increasing dose suggests that the primary driving force for the crystalline-to-amorphous transition under these ion irradiation conditions in SiC is due to the accumulation of both Frenkel pairs and antisite defects.


Author(s):  
C. R. Hills ◽  
G. J. Thomas ◽  
J. K. Maurin

Solution treated and quenched Si-Ge (30 at. %) alloy doped with phosphorus to a level of 1.54 × 1020 atoms/cm3 has been shown to increase in resistivity following aging at elevated temperatures. This effect is indicative of a loss of phosphorus from substitutional sites in the Si-Ge lattice and consequent precipitation of the excess phosphorus into electrically inactive centers. The structural changes occurring as a result of aging have been studied using transmission electron microscopy.Examination of the solution heat-treated material (1 hr. at 1000°C, then quenched) prior to aging revealed the presence of small defect clusters ranging in size from 20-80 Å, as well as larger defects approximately 200 Å in diameter exhibiting large strain field contrast.


Author(s):  
Rodney A. Herring

Diffracted beam interferometry, DBI, (previously referred to as Convergent Beam Electron Diffraction + Electron Biprism Interferometry, CBED+EBI) which uses an electron biprism to deflect diffracted beams (convergent or parallel) can produce an interferogram between any two beams within the information envelope of the microscope such that the beam's amplitude and phase can be measured and studied. As well, the electron source need not be highly coherent. So far, DBI has been applied only to transmission electron diffraction, although there is no reason why it shouldn't be applicable to all electron diffraction methods including reflection high (low) energy electron diffraction, RH(L)EED and, possibly, back-scattered electron diffraction, BSED, in the SEM for the study of surfaces. DBI has already shown that substantial phase information, such as strain at interfaces and dislocations, compositional gradients and small defect clusters which are on the size scale of the unit cell, are retrievable from its holograms.


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