scholarly journals High-temperature phase transitions in dense germanium

2021 ◽  
Vol 154 (17) ◽  
pp. 174702
Author(s):  
Liam C. Kelsall ◽  
Miriam Peña-Alvarez ◽  
Miguel Martinez-Canales ◽  
Jack Binns ◽  
Chris J. Pickard ◽  
...  
1989 ◽  
Vol 100 (1) ◽  
pp. 135-141 ◽  
Author(s):  
A. I. Baranov ◽  
V. P. Khiznichenko ◽  
L. A. Shuvalov

2001 ◽  
Vol 145 (1-4) ◽  
pp. 179-184 ◽  
Author(s):  
Calum R.I. Chisholm ◽  
Sossina M. Haile

2008 ◽  
Vol 81 (1) ◽  
pp. 29-41 ◽  
Author(s):  
M. M. Abdel-Kader ◽  
F. El-Kabbany ◽  
H. Naguib ◽  
W. M. Gamal

1999 ◽  
Vol 95 (3) ◽  
pp. 351-357 ◽  
Author(s):  
V. Kapustianik ◽  
Yu. Korchak ◽  
S. Sveleba ◽  
R. Tchukvinskyi ◽  
I. Girnyk

2015 ◽  
Vol 48 (2) ◽  
pp. 318-333 ◽  
Author(s):  
B. Orayech ◽  
A. Faik ◽  
G. A. López ◽  
O. Fabelo ◽  
J. M. Igartua

Na0.5K0.5NbO3has been synthesized by the conventional solid-state reaction process. The crystal structures and phase transitions, at low and high temperature, determined from the Rietveld refinements of X-ray and neutron powder diffraction data are reported. The structure evolution of Na0.5K0.5NbO3in the temperature range from 2 to 875 K shows the presence of three phase transitions. The first one, at ∼135 K, is discontinuous from the rhombohedralR3c(No. 161) space group to the room-temperature orthorhombicAmm2 (No. 38) space group; the second is discontinuous from the orthorhombic to the tetragonalP4mmspace group (No. 99) at ∼465 K, and the third is continuous from the tetragonal to the cubic Pm\overline{3}m space group (No. 221) at ∼700 K. The obtained phase-transition sequence isR3c→Amm2 →P4mm→Pm\overline{3}m. No previous studies at low temperature have been carried out on the material with composition Na0.5K0.5NbO3. In the course of the determination of the three experimentally found phases, a novel method of refinement is presented. This is a step forward in the use of the symmetry-adapted modes as degrees of freedom in the refinement process: the parameterization of a direction in the internal space of the, in this case, sole irreducible representation, GM4−, responsible for the symmetry breaking from the parent cubic space group to the polar distorted low-symmetry phases. Eventually, this procedure enables the calculation of the spontaneous polarization.


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