Lattice dynamics and the phase transition from the cubic phase to the tetragonal phase in the LaMnO3 crystal within the polarizable-ion model

2007 ◽  
Vol 49 (9) ◽  
pp. 1749-1758 ◽  
Author(s):  
V. I. Zinenko ◽  
M. S. Pavlovskiĭ
2008 ◽  
Vol 23 (S1) ◽  
pp. S70-S74 ◽  
Author(s):  
L. M. Acuña ◽  
R. O. Fuentes ◽  
D. G. Lamas ◽  
I. O. Fábregas ◽  
N. E. Walsöe de Reca ◽  
...  

Crystal structure of compositionally homogeneous, nanocrystalline ZrO2–CeO2 solutions was investigated by X-ray powder diffraction as a function of temperature for compositions between 50 and 65 mol % CeO2. ZrO2-50 and 60 mol % CeO2 solid solutions, which exhibit the t′-form of the tetragonal phase at room temperature, transform into the cubic phase in two steps: t′-to-t″ followed by t″-to-cubic. But the ZrO2-65 mol % CeO2, which exhibits the t″-form, transforms directly to the cubic phase. The results suggest that t′-to-t″ transition is of first order, but t″-to-cubic seems to be of second order.


1981 ◽  
Vol 42 (C6) ◽  
pp. C6-749-C6-751 ◽  
Author(s):  
M. D. Fontana ◽  
G. E. Kugel ◽  
C. Carabatos

1977 ◽  
Vol 32 (4) ◽  
pp. 413-415 ◽  
Author(s):  
P. W. Richter ◽  
J. B. Clark

The effect of pressure on the tetragonal/cubic phase transition in K3FeF6 was studied to 35 kbar. A new phase which also occurs in K3TiF6, exists over a small temperature region at low pressures. A strong possibility exists that the K3FeF6 tetragonal phase is isostructural with the corresponding phase found for the K3XF6 (X = Ln, Y) compounds.


2017 ◽  
Vol 5 (22) ◽  
pp. 5451-5457 ◽  
Author(s):  
Zhilei Sui ◽  
Shuhe Hu ◽  
Hao Chen ◽  
Chan Gao ◽  
Hao Su ◽  
...  

Laser irradiation transforms Sb2O3 from the tetragonal phase into an HD-amorphous phase under high pressure and back to cubic phase from LD-amorphous phase at ambient conditions.


1995 ◽  
Vol 52 (13) ◽  
pp. 9111-9114 ◽  
Author(s):  
A. P. Mirgorodsky ◽  
M. B. Smirnov ◽  
P. E. Quintard ◽  
T. Merle-Méjean

2014 ◽  
Vol 04 (01) ◽  
pp. 1450001 ◽  
Author(s):  
Jun Luo ◽  
Shujun Zhang ◽  
Wesley Hackenberger ◽  
Thomas R. Shrout

In this work, crystal growth and characterization of PIN–PMN–PT (29–59% PIN and 28–35% PT) were conducted to understand how PIN ratio in the PIN–PMN–PT system impacts its phase stability during crystallization. High-quality PIN–PMN–PT crystals with 36% PIN were obtained using the self-seeded Bridgman process, even though the cubic phase In 2 O 3 formed at the very beginning of solidification. The melt became more unstable when the PIN ratio in the PIN–PMN–PT system increased to 49% and above, which affected the composition and quality of the as-grown crystals significantly. By increasing the PIN to 36% in PIN–PMN–PT crystal, the rhombohedral-to-tetragonal phase transition temperatures and the coercive field reached 115–135°C and 4.5~5.6 kV/cm, respectively, that greatly expanded the operation domains compared to PMN–PT crystals.


2011 ◽  
Vol 485 ◽  
pp. 19-22
Author(s):  
Yoshiki Iwazaki ◽  
Tatsuo Sakashita ◽  
Toshimasa Suzuki ◽  
Youichi Mizuno ◽  
Shinji Tsuneyuki

Structural changes induced by oxygen vacancies in tetragonal phase BaTiO3are studied with first principles calculations within density functional theory. In our calculations, the incorporation of oxygen vacancies greatly decreases c/a ratio of the tetragonal phase BaTiO3, and a phase transition from tetragonal to cubic phase occurs when the incorporation of the oxygen vacancies reaches about 4%. Our results also shows that the generation of the oxygen vacancies slightly increases the volume of BaTiO3, and the increases are typically less than 0.5% even in heavily reduced conditions.


2020 ◽  
Vol 62 (12) ◽  
pp. 2169
Author(s):  
А.С. Анохин ◽  
А.Г. Разумная ◽  
А.В. Павленко

The lattice dynamics of strontium ferrotungsten ceramics have been studied by Raman spectroscopy in the temperature range 300−700 K. The spectra analysis confirmed tetragonal symmetry of strontium ferrotungsten which is consistent with the XRD results. The features of the temperature behaviour of the phonon modes of strontium ferrotungsten are revealed, and it is shown that a diffuse phase transition from the tetragonal to the cubic phase occurs at temperatures of 410–500 K.


2003 ◽  
Vol 784 ◽  
Author(s):  
V. M. Naik ◽  
M. Smith ◽  
H. Dai ◽  
P. Talagala ◽  
R. Naik ◽  
...  

ABSTRACTPb1-x Srx TiO3 (x = 0 to 1.0) films of thickness ∼ 4 μ m have been prepared on sapphire and Pt substrates by metalorganic decomposition (MOD) method. X-ray diffraction results show that the films are polycrystalline with a perovskite tetragonal phase at room temperature for x < 0.5 and a cubic phase for x > 0.5. Room temperature Raman spectra show a systematic variation of lattice vibrational modes with x. The most notable changes in the Raman spectra with x are the decrease in the splitting of A1(3TO) and E(3TO) modes and the disappearance of E(3TO) mode at x ∼ 0.6. Although the x-ray diffraction peaks for films with x > 0.5 show a cubic phase at room temperature, the Raman spectra show the characteristic phonon modes of a tetragonal phase even at x = 0.7. The dielectric permittivity versus temperature measurements for films with x ≤ 0.7 show a broad dielectric anomaly corresponding to a diffuse ferroelectric to paraelectric phase transition. The phase transition temperature (Tc) values are consistently lower than the corresponding bulk ceramic alloys. Furthermore, Tc are also determined by monitoring the temperature dependence of the splitting between E(3TO) and A1(3TO) phonon modes in the Raman spectra of Pb1-x Srx TiO3 films for x ≤ 0.6. There has been good agreement between the two methods.


2021 ◽  
Author(s):  
Mark Stockham ◽  
Alice Griffiths ◽  
Bo Dong ◽  
Peter Slater

Lithium garnets are promising solid-state electrolytes for next generation lithium-ion batteries. These materials have high ionic conductivity, a wide electrochemical window and stability with Li metal. However, lithium garnets have a maximum limit of 7 lithium atoms per formula unit (e.g. La3Zr2Li7O12), before the system transitions from a cubic to a tetragonal phase with poor ionic mobility. This arises from full occupation of the Li sites. Hence, the most conductive lithium garnets have Li between 6-6.55 Li per formula unit, which maintains the cubic symmetry and the disordered Li sub-lattice. The tetragonal phase, however, forms the highly conducting cubic phase at higher temperatures, thought to arise from increased cell volume and entropic stabilisation permitting Li disorder. However, little work has been undertaken in understanding the controlling factors of this phase transition, which could enable enhanced dopant strategies to maintain room temperature cubic garnet at higher Li contents. Here, a series of nine tetragonal garnets were synthesised and analysed via variable temperature XRD to understand the dependence of site substitution on the phase transition temperature. Interestingly the octahedral site cation radius was identified as the key parameter for the transition temperature with larger or smaller dopants altering the transition temperature noticeably. A site substitution was, however, found to make little difference irrespective of significant changes to cell volume.


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