Crystalline Structure and Physical Properties of High-Entropy Film Alloys

2019 ◽  
Vol 11 (2) ◽  
pp. 02026-1-02026-6
Author(s):  
Yu. S. Bereznyak ◽  
◽  
M. Opielak ◽  
L. V. Odnodvorets ◽  
D. V. Poduremne ◽  
...  
2021 ◽  
Author(s):  
Christian Wagner ◽  
Alberto Ferrari ◽  
Jürgen Schreuer ◽  
Jean-Philippe Couzinié ◽  
Yuji Ikeda ◽  
...  

2022 ◽  
Vol 893 ◽  
pp. 162108
Author(s):  
Taesung Park ◽  
Hamid Reza Javadinejad ◽  
Young-Kuk Kim ◽  
Hye Jung Chang ◽  
Haneul Choi ◽  
...  

MRS Advances ◽  
2020 ◽  
Vol 5 (64) ◽  
pp. 3419-3436 ◽  
Author(s):  
P. B. Meisenheimer ◽  
J. T. Heron

AbstractHistorically, the enthalpy is the criterion for oxide materials discovery and design. In this regime, highly controlled thin film epitaxy can be leveraged to manifest bulk and interfacial phases that are non-existent in bulk equilibrium phase diagrams. With the recent discovery of entropy-stabilized oxides, entropy and disorder engineering has been realized as an orthogonal approach. This has led to the nucleation and rapid growth of research on high-entropy oxides – multicomponent oxides where the configurational entropy is large but its contribution to its stabilization need not be significant or is currently unknown. From current research, it is clear that entropy enhances the chemical solubility of species and can realize new stereochemical configurations which has led to the rapid discovery of new phases and compositions. The research has expanded beyond studies to understand the role of entropy in stabilization and realization of new crystal structures to now include physical properties and the roles of local and global disorder. Here, key observations made regarding the dielectric and magnetic properties are reviewed. These materials have recently been observed to display concerted symmetry breaking, metal-insulator transitions, and magnetism, paving the way for engineering of these and potentially other functional phenomena. Excitingly, the disorder in these oxides allows for new interplay between spin, orbital, charge, and lattice degrees of freedom to design the physical behavior. We also provide a perspective on the state of the field and prospects for entropic oxide materials in applications considering their unique characteristics.


2020 ◽  
Vol 507 ◽  
pp. 145131
Author(s):  
Xiaoyao Sun ◽  
Xingwang Cheng ◽  
Hongnian Cai ◽  
Shuai Ma ◽  
Ziqi Xu ◽  
...  

It is now some ten years since it was first realised that, in common with natural and artificial cellulose fibres, animal fibres with a protein basis are in many cases sufficiently crystalline to yield a pronounced interference figure when examined with monochromatic X-rays. Such “ X-ray fibre diagrams ” were reported in 1921 by HERZOG and JANCKE* for muscle, nerve, sinew, and hair, and in 1924 similar photographs from human hair were obtained by one of the present writers. From an X-ray examination of wool it was concluded by THREADGOLD that “ there is no evidence for assuming the wool fibres and yarns examined to have a crystalline structure,” but in 1927 EWLES and SPEAKMAN had already obtained wool interference figures precisely similar to those previously obtained from hair. The two last-named authors endeavoured to interpret their results in the light of certain physical properties, but it has since become clear that the problem of hair structure is sufficiently complex to necessitate an X-ray study of a wide range of materials under as great a variety of conditions as possible. The present communication is an account of the preliminary results of such an investigation. Over a hundred X-ray photographs have been taken, using copper K-radiation filtered of the MATHS FORMULA line by nickel foil about 1/100 mm. thick. The “ slit” was a rectangular aperture, 4 cm. x 0.5mm., the scattered rays from which were screened off in the usual manner by a secondary slit.


Specimens of polychloroprene before and after light treatment have been examined by X -ray methods. There is no change in the crystalline structure, although there are differences in the physical properties ascribed to cross-linking of the long-chain molecules. The unit cell is possibly ortho­rhombic: a = 8·90 A , b = 4·70 A, c = 12·21 A, and contains four chloroprene (C 4 H 5 Cl) units.


2020 ◽  
Vol 820 ◽  
pp. 153228 ◽  
Author(s):  
S.A. Uporov ◽  
R.E. Ryltsev ◽  
V.A. Bykov ◽  
S. Kh Estemirova ◽  
D.A. Zamyatin

1996 ◽  
Vol 53 (7) ◽  
pp. 389-397 ◽  
Author(s):  
Takao NOMURA ◽  
Takeyoshi NISHIO ◽  
Kimio IMAIZUMI ◽  
Yoshikazu UEDA ◽  
Hiroshi OYAMADA

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