Response to ‘‘Comment on ‘Short time dynamics of glass‐forming liquids’ ’’ [J. Chem. Phys. 104, 8169 (1996)]

1996 ◽  
Vol 104 (20) ◽  
pp. 8171-8172 ◽  
Author(s):  
C. M. Roland ◽  
K. L. Ngai
Keyword(s):  
Chem Phys ◽  
Time Dynamics ◽  
Glass Forming ◽  
Short Time

Short-time dynamics of glass-forming liquids: Phenyl salicylate (salol) in bulk liquid, dilute solution, and confining geometries

2003 ◽  
Vol 118 (18) ◽  
pp. 8340-8349 ◽  
Author(s):  
A. G. Kalampounias ◽  
S. N. Yannopoulos ◽  
W. Steffen ◽  
L. I. Kirillova ◽  
S. A. Kirillov
Keyword(s):  
Bulk Liquid ◽  
Dilute Solution ◽  
Phenyl Salicylate ◽  
Time Dynamics ◽  
Glass Forming ◽  
Short Time

The Dynamics of Interacting Systems: Glassy Ionic Conductors and Glass-Forming Materials

1995 ◽  
Vol 411 ◽  
Author(s):  
K. L. Ngai ◽  
A. K. Rizos
Keyword(s):  
Correlation Function ◽  
Structural Relaxation ◽  
Time Range ◽  
Relaxation Techniques ◽  
Ionic Conductors ◽  
Time Dynamics ◽  
Glass Forming ◽  
Interacting Systems ◽  
Glass Forming Materials ◽  
Short Time

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.

Short time dynamics of glass‐forming liquids

1995 ◽  
Vol 103 (3) ◽  
pp. 1152-1159 ◽  
Author(s):  
C. M. Roland ◽  
K. L. Ngai
Keyword(s):  
Time Dynamics ◽  
Glass Forming ◽  
Short Time

scholarly journals Interplay between nematicity and Bardasis-Schrieffer modes in the short-time dynamics of unconventional superconductors

2021 ◽  
Vol 103 (2) ◽  
Author(s):  
Marvin A. Müller ◽  
Pavel A. Volkov ◽  
Indranil Paul ◽  
Ilya M. Eremin
Keyword(s):  
Time Dynamics ◽  
Unconventional Superconductors ◽  
Short Time

SHORT-TIME DYNAMICS OF THE RANDOM n-VECTOR MODEL WITH LONG-RANGE INTERACTION

2003 ◽  
Vol 17 (23) ◽  
pp. 1227-1236 ◽  
Author(s):  
YUAN CHEN ◽  
ZHI-BING LI
Keyword(s):  
Long Range ◽  
High Temperature Phase ◽  
Vector Model ◽  
Temperature Phase ◽  
Range Interaction ◽  
Time Dynamics ◽  
Long Range Interaction ◽  
Renormalization Group Approach ◽  
Short Time ◽  
N Vector

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.

Short-Time Dynamics in Quasi-Two-Dimensional Colloidal Suspensions

2005 ◽  
Vol 95 (19) ◽  
Author(s):  
Jesús Santana-Solano ◽  
Angeles Ramírez-Saito ◽  
José Luis Arauz-Lara
Keyword(s):  
Colloidal Suspensions ◽  
Two Dimensional ◽  
Time Dynamics ◽  
Short Time
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