Soft-Mode Behavior in the Phonon Dispersion of YS

1978 ◽  
Vol 40 (7) ◽  
pp. 465-468 ◽  
Author(s):  
P. Roedhammer ◽  
W. Reichardt ◽  
F. Holtzberg
1982 ◽  
Vol 41 (4) ◽  
pp. 345-349 ◽  
Author(s):  
F. Gervais ◽  
J.L. Servoin ◽  
J.F. Baumard ◽  
F. Denoyer
Keyword(s):  

2017 ◽  
Vol 512 (1) ◽  
pp. 52-57
Author(s):  
Shunsuke Suzuki ◽  
Toru Mogami ◽  
Shota Nakamura ◽  
Yuhji Tsujimi ◽  
Makoto Iwata
Keyword(s):  

2007 ◽  
Vol 147 (3-4) ◽  
pp. 375-386 ◽  
Author(s):  
R. Heid ◽  
K. -P. Bohnen ◽  
B. Renker ◽  
P. Adelmann ◽  
T. Wolf ◽  
...  
Keyword(s):  

2012 ◽  
Vol 31 (6) ◽  
pp. 741-747 ◽  
Author(s):  
Mustafa Cem Lider ◽  
Hamit Yurtseven

AbstractThe Raman frequencies of the lattice modes (147 cm−1 and 207 cm−1) are analyzed for the α-β transition in quartz according to a power-law formula with the critical exponent by using the experimental data. The temperature dependence of the Raman frequency is associated with the order parameter (polarization P) for this transition in the quartz crystal.The damping constant of the lattice modes studied here is calculated using the Raman frequencies at various temperatures for the α-β transition in quartz (Tc = 846 K) using the soft mode – hard mode and the energy fluctuation models. Our calculations for the damping constant (bandwidths) give an evidence that the lattice mode of the 147 cm−1 exhibits a soft mode behavior for the α-β transition in quartz.


1984 ◽  
Vol 2 (5) ◽  
pp. 161-170 ◽  
Author(s):  
F. Gervais ◽  
J. L. Servoin ◽  
B. Jannot
Keyword(s):  

2020 ◽  
Vol 124 (39) ◽  
pp. 21329-21337 ◽  
Author(s):  
Akun Liang ◽  
Saqib Rahman ◽  
Placida Rodriguez-Hernandez ◽  
Alfonso Muñoz ◽  
Francisco Javier Manjón ◽  
...  

2009 ◽  
Vol 95 (23) ◽  
pp. 232902 ◽  
Author(s):  
D. Nuzhnyy ◽  
J. Petzelt ◽  
S. Kamba ◽  
P. Kužel ◽  
C. Kadlec ◽  
...  

1974 ◽  
Vol 14 (11) ◽  
pp. 1137-1139 ◽  
Author(s):  
D. Bäuerle ◽  
Y. Yacoby ◽  
W. Richter
Keyword(s):  

2002 ◽  
Vol 718 ◽  
Author(s):  
Graeme J. Ackland ◽  
Neil D. Drummond

AbstractWhile phase transition pressures and zero temperature thermodynamic properties can be accurately determined from electronic structure calculation, transition temperatures are more problematic because of the need to sample phase space and quantise vibrations. The quasiharmonic method has proved extremely accurate for calculating thermodynamic properties up to 90% of the melting point without explicit phase space sampling for most materials, but has low temperature divergences for soft mode materials such as perovskites. Here we present a modified quasiharmonic method which avoids these difficulties. Using a simple model system, we demonstrate trends of behaviour in both the classical and quantum limits showing the importance of phonon quantisation in soft-mode behavior.


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