Cubic to Tetragonal Phase Transition of SrTiO3 under Epitaxial Stress: An X-Ray Backscattering Study

2000 ◽  
Vol 181 (2) ◽  
pp. 387-404 ◽  
Author(s):  
Lixin Cao ◽  
E. Sozontov ◽  
J. Zegenhagen
2002 ◽  
Vol 164 (1) ◽  
pp. 51-59 ◽  
Author(s):  
Roushown Ali ◽  
Masatomo Yashima ◽  
Masahiko Tanaka ◽  
Hideki Yoshioka ◽  
Takeharu Mori ◽  
...  

2017 ◽  
Vol 53 (54) ◽  
pp. 7537-7540 ◽  
Author(s):  
Shijing Sun ◽  
Zeyu Deng ◽  
Yue Wu ◽  
Fengxia Wei ◽  
Furkan Halis Isikgor ◽  
...  

Single crystals of [(NH2)2CH]PbI3 undergo a cubic-to-tetragonal phase transition at low temperature and high pressure.


1988 ◽  
Vol 23 (10) ◽  
pp. 1409-1415 ◽  
Author(s):  
Y. Ueda ◽  
A. Mitushima ◽  
H. Toda ◽  
N. Kojima ◽  
M. Yoshikawa ◽  
...  

1969 ◽  
Vol 24 (10) ◽  
pp. 1518-1525
Author(s):  
C. Friebel ◽  
D. Reinen

Abstract The ESR-powder-spectra of the perovskite-mixed-crystals M2II (CuxZn1-xW)O6 [MII=Sr, Ba] and Sr2(CuxZn1-xTe)O6 , which have been investigated by means of conventional X-ray-techniques and ligand-field-spectroscopy 1,2, are described and the results extensively discussed. The conclusions can be summarized as follows: (a) At very low x-values isolated, dynamically Jahn-Teller-distorted CuO6-octahedra are present in the cubic matrices, which can be frozen into tetragonally elongated polyhedra at 4.2 °K; (b) At high x-values the CuO6-entities are statically JT-distorted with the long axes lined up along the c-axis of the macroscopically tetragonal phases; (c) The ESR-spectra around the cubic-tetragonal phase-transition are complex, containing signals of obviously magnetically coupled Cu2+-ions; (d) The g-values "follow" the ligand-field-parameters quantitatively. Comparative data of some other compounds are given.


1982 ◽  
Vol 25 (1) ◽  
pp. 364-371 ◽  
Author(s):  
Y. Fujii ◽  
J. B. Hastings ◽  
M. Kaplan ◽  
G. Shirane ◽  
Y. Inada ◽  
...  

1987 ◽  
Vol 99 ◽  
Author(s):  
G. Gonzalez ◽  
D. Rios-Jara ◽  
T. Akachi ◽  
R. Barrio ◽  
L. BañOs ◽  
...  

ABSTRACTSuperconducting compounds of Y1B2C3−xFexOy, with x=0.125, 0.0625, 0.125 and 0.300, were studied using X-ray powder diffractometry. Two sets of samples were prepared. Samples quenched from 950°C to liquid nitrogen temperature showed a tetragonal non-superconducting phase, whose lattice parameters depend on the Fe content and differ from those of the yttrium 1:2:3 tetragonal phase. Samples oxygenated at 450°C showed an orthorhombic to tetragonal phase transition for Fe contents higher than x=0.0625. The lattice parameters of this tetragonal phase were different from those of both tetragonal phases mentioned above. All these observations allow us to conclude that C(l) sites are occupied at least partially by Fe impurities.


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