scholarly journals Nonuniqueness of the quasinormal mode expansion of electromagnetic Lorentz dispersive materials

2020 ◽  
Vol 37 (7) ◽  
pp. 1219 ◽  
Author(s):  
A. Gras ◽  
P. Lalanne ◽  
M. Duruflé
2017 ◽  
Vol 7 (2) ◽  
Author(s):  
Filippo Alpeggiani ◽  
Nikhil Parappurath ◽  
Ewold Verhagen ◽  
L. Kuipers

1995 ◽  
Vol 74 (23) ◽  
pp. 4588-4591 ◽  
Author(s):  
E. S. C. Ching ◽  
P. T. Leung ◽  
W. M. Suen ◽  
K. Young

2020 ◽  
Vol 102 (3) ◽  
Author(s):  
Felix Binkowski ◽  
Fridtjof Betz ◽  
Rémi Colom ◽  
Martin Hammerschmidt ◽  
Lin Zschiedrich ◽  
...  

1998 ◽  
Vol 70 (4) ◽  
pp. 1545-1554 ◽  
Author(s):  
E. S. C. Ching ◽  
P. T. Leung ◽  
A. Maassen van den Brink ◽  
W. M. Suen ◽  
S. S. Tong ◽  
...  

1991 ◽  
Vol 43 (1) ◽  
pp. 1-8 ◽  
Author(s):  
Wai-Mo Suen ◽  
Kenneth Young

2001 ◽  
Vol 48 (1) ◽  
pp. 67-84 ◽  
Author(s):  
Omar Di Stefano ◽  
Salvatore Savasta ◽  
Raffaello Girlanda
Keyword(s):  

2014 ◽  
Vol 29 (24) ◽  
pp. 1430049 ◽  
Author(s):  
Chanyong Park

We review interesting results achieved in recent studies on the holographic Lifshitz field theory. The holographic Lifshitz field theory at finite temperature is described by a Lifshitz black brane geometry. The holographic renormalization together with the regularity of the background metric allows to reproduce thermodynamic quantities of the dual Lifshitz field theory where the Bekenstein–Hawking entropy appears as the renormalized thermal entropy. All results satisfy the desired black brane thermodynamics. In addition, hydrodynamic properties are further reviewed in which the holographic retarded Green functions of the current and momentum operators are studied. In a nonrelativistic Lifshitz field theory, intriguingly, there exists a massive quasinormal mode at finite temperature whose effective mass is linearly proportional to temperature. Even at zero temperature and in the nonzero momentum limit, a quasinormal mode still remains unlike the dual relativistic field theory. Finally, we account for how adding impurity modifies the electric property of the nonrelativistic Lifshitz theory.


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