High Entropy Spinel-structure Oxide for electrochemical application

2021 ◽  
pp. 133448
Author(s):  
Zheng Sun ◽  
Yongjie Zhao ◽  
Chen Sun ◽  
Qing Ni ◽  
Chengzhi Wang ◽  
...  
2020 ◽  
Vol 503 ◽  
pp. 166594 ◽  
Author(s):  
Aiqin Mao ◽  
Hong-Xiang Xie ◽  
Hou-Zheng Xiang ◽  
Zhan-Guo Zhang ◽  
Hui Zhang ◽  
...  

2018 ◽  
Vol 216 ◽  
pp. 32-36 ◽  
Author(s):  
Juliusz Dąbrowa ◽  
Mirosław Stygar ◽  
Andrzej Mikuła ◽  
Arkadiusz Knapik ◽  
Krzysztof Mroczka ◽  
...  

2020 ◽  
Vol 989 ◽  
pp. 341-346
Author(s):  
O.V. Zaitseva ◽  
Vladimir E. Zhivulin ◽  
D.E. Zhivulin

This paper presents the results of an experimental study of the possibility of high-entropy oxide phases creation using the of solid-phase synthesis method in the Al2O3–BaO–CuO–Fe2O3–Mn2O3–NiO–SrO–TiO2–ZnO and Al2O3–BaO–CuO–Fe2O3–NiO–SrO–TiO2–WO3–ZnO systems. As a result of the study, a microcrystalline octahedral multicomponent phase was found in the crystallized sample. Judging by the composition, this phase has a spinel structure and is characterized (judging by the components concentrations and its ratio) by rather high values of the mixing configurational entropy. It is shown that barium, strontium and tungsten are not included in this phase in appreciable amounts. The obtained results indicate the possibility of synthesizing high-entropic spinels using these Al2O3–CuO–Fe2O3–Mn2O3–NiO–TiO2–ZnO systems.


Author(s):  
Hui-Xia Guo ◽  
Wei-Ming Wang ◽  
Cheng-Yu He ◽  
Bao-Hua Liu ◽  
Dong-Mei Yu ◽  
...  

Author(s):  
C. A. Bateman ◽  
A.Z. Ringwelski ◽  
R.W. Broach

Gamma (γ) alumina is referred to as a defect spinel because it has a tetragonally distorted spinel structure (AB2O4) and an insufficient number of cations to fill all cation sites. In the spinel structure, the oxygen lattice is cubic close packed with A- and B-site cations in tetrahedral and octahedral coordination, respectively. The 2l⅓ Al atoms per unit cell of γ alumina can distribute themselves across 16 octahedral and 8 tetrahedral sites.The literature differs on where the 2⅔ cation vacancies per unit cell are located. Wilson and McConnell proposed that the vacancies in γ alumina, as first formed by calcining boehmite, are predominantly on the tetrahedral lattice but, with further heat treatment, move to occupy random positions on both octahedral and tetrahedral lattices. One study using NMR showed that the vacancies lay exclusively on the tetrahedral lattice, independent of the calcination temperature. A more-recent study using Rietveld refinement of powder neutron diffraction data suggested that both octahedral and tetrahedral lattices were partially occupied.


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