Short time dynamics of glass‐forming liquids

1995 ◽  
Vol 103 (3) ◽  
pp. 1152-1159 ◽  
Author(s):  
C. M. Roland ◽  
K. L. Ngai
2003 ◽  
Vol 118 (18) ◽  
pp. 8340-8349 ◽  
Author(s):  
A. G. Kalampounias ◽  
S. N. Yannopoulos ◽  
W. Steffen ◽  
L. I. Kirillova ◽  
S. A. Kirillov

1995 ◽  
Vol 411 ◽  
Author(s):  
K. L. Ngai ◽  
A. K. Rizos

ABSTRACTThe dynamics of densely packed interacting systems including glass-forming materials and glassy ionic conductors of various chemical and micro structures have been investigated experimentally by many workers, covering an immense time range from microscopic times shorter than 10−12 s to macroscopic times as long as 104 s. The short time dynamics is fundamental because it can directly reveal the microscopic mechanism of the relaxation. Several experimental investigations of structural relaxation in glass-forming substances have found that the short time dynamics shows exponential relaxation with a correlation function well described by exp(−t/τo) for t<tc where tc is temperature insensitive and has the order of magnitude of a picosecond. The correlation function then crosses over at tc to assumes the stretched exponential form, exp[−(t/τ)β], for t>tc. The relaxation times τ and τo are related by the expression τ = [tc−(1−β)τo]1/β. In this work, we focus on glassy ionic conductors and ionic glass-forming materials and experiments that employ dielectric spectroscopic and conductivity relaxation techniques, the theme of this Symposium. We show that these experimental data exhibit the same feature as described above for structural relaxation and are in accord with the predictions of the coupling model proposed by one of the authors.


2021 ◽  
Vol 103 (2) ◽  
Author(s):  
Marvin A. Müller ◽  
Pavel A. Volkov ◽  
Indranil Paul ◽  
Ilya M. Eremin

2003 ◽  
Vol 17 (23) ◽  
pp. 1227-1236 ◽  
Author(s):  
YUAN CHEN ◽  
ZHI-BING LI

The short-time critical behavior of the random n-vector model with long-range interaction is studied by the theoretic renormalization-group approach. After a sudden quench to the critical temperature from the high temperature phase, the system is released to an evolution within model A dynamics. The initial slip exponents and the dynamic exponent are calculated to two-loop order.


2005 ◽  
Vol 95 (19) ◽  
Author(s):  
Jesús Santana-Solano ◽  
Angeles Ramírez-Saito ◽  
José Luis Arauz-Lara

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