scholarly journals Direct Measurement of the Surface Energy of Bimetallic Nanoparticles: Evidence of Vegard’s Rulelike Dependence

2018 ◽  
Vol 120 (2) ◽  
Author(s):  
Adrian Chmielewski ◽  
Jaysen Nelayah ◽  
Hakim Amara ◽  
Jérôme Creuze ◽  
Damien Alloyeau ◽  
...  
Nano Letters ◽  
2017 ◽  
Vol 17 (6) ◽  
pp. 3815-3821 ◽  
Author(s):  
Christian D. van Engers ◽  
Nico E. A. Cousens ◽  
Vitaliy Babenko ◽  
Jude Britton ◽  
Bruno Zappone ◽  
...  

Nanoscale ◽  
2019 ◽  
Vol 11 (3) ◽  
pp. 1386-1395 ◽  
Author(s):  
Zheng Zhao ◽  
Haoxiang Xu ◽  
Yi Gao ◽  
Daojian Cheng

To achieve universal description of the reshaping process of core–shell bimetallic nanoparticles, we combined the tight-binding Ising Hamiltonian model with molecular dynamic simulations to propose a general theoretical model at the atomic scale while considering the temperature, bond energy, atomic size, and surface energy effects.


2020 ◽  
Vol 22 (15) ◽  
pp. 7787-7793
Author(s):  
Kayoung Yun ◽  
Ho-Seok Nam ◽  
Seungchul Kim

The competition between mixing energy and surface energy determines atomic mixing pattern of bimetallic nanoparticles.


Author(s):  
Michael W. Bench ◽  
Paul G. Kotula ◽  
C. Barry Carter

The growth of semiconductors, superconductors, metals, and other insulators has been investigated using alumina substrates in a variety of orientations. The surface state of the alumina (for example surface reconstruction and step nature) can be expected to affect the growth nature and quality of the epilayers. As such, the surface nature has been studied using a number of techniques including low energy electron diffraction (LEED), reflection electron microscopy (REM), transmission electron microscopy (TEM), molecular dynamics computer simulations, and also by theoretical surface energy calculations. In the (0001) orientation, the bulk alumina lattice can be thought of as a layered structure with A1-A1-O stacking. This gives three possible terminations of the bulk alumina lattice, with theoretical surface energy calculations suggesting that termination should occur between the Al layers. Thus, the lattice often has been described as being made up of layers of (Al-O-Al) unit stacking sequences. There is a 180° rotation in the surface symmetry of successive layers and a total of six layers are required to form the alumina unit cell.


Author(s):  
P. J. Goodhew

Cavity nucleation and growth at grain and phase boundaries is of concern because it can lead to failure during creep and can lead to embrittlement as a result of radiation damage. Two major types of cavity are usually distinguished: The term bubble is applied to a cavity which contains gas at a pressure which is at least sufficient to support the surface tension (2g/r for a spherical bubble of radius r and surface energy g). The term void is generally applied to any cavity which contains less gas than this, but is not necessarily empty of gas. A void would therefore tend to shrink in the absence of any imposed driving force for growth, whereas a bubble would be stable or would tend to grow. It is widely considered that cavity nucleation always requires the presence of one or more gas atoms. However since it is extremely difficult to prepare experimental materials with a gas impurity concentration lower than their eventual cavity concentration there is little to be gained by debating this point.


1970 ◽  
Vol 13 (1) ◽  
pp. 65-73 ◽  
Author(s):  
Mary Mira

Listening, a significant dimension of the behavior of hearing-impaired children, may be measured directly by recording childrens' responses to obtain audio narrations programmed via a conjugate reinforcement system. Twelve hearing-impaired, school-aged children responded in varying ways to the opportunity to listen. Direct and continuous measurement of listening has relevance for evaluation of remediation methods and for discovery of variables potentially related to listening.


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