Quasinormal mode theory and applications of light-matter interactions in nanoplasmonics

2014 ◽  
Author(s):  
R.-C. Ge ◽  
S. Hughes
Keyword(s):  
Quasinormal Mode ◽  
Mode Theory

scholarly journals Quasinormal mode theory and design of on-chip single photon emitters in photonic crystal coupled-cavity waveguides

2016 ◽  
Vol 24 (12) ◽  
pp. 13574 ◽  
Author(s):  
T. Malhotra ◽  
R.-C. Ge ◽  
M. Kamandar Dezfouli ◽  
A. Badolato ◽  
N. Vamivakas ◽  
...  
Keyword(s):  
Photonic Crystal ◽  
Single Photon ◽  
Quasinormal Mode ◽  
Mode Theory ◽  
Single Photon Emitters ◽  
On Chip ◽  
Coupled Cavity

Intrinsic mode theory of tapered optical waveguides

1985 ◽  
Vol 132 (6) ◽  
pp. 314 ◽  
Author(s):  
J.M. Arnold ◽  
A. Belghoraf ◽  
A. Dendane
Keyword(s):  
Optical Waveguides ◽  
Mode Theory

Review of the holographic Lifshitz theory

2014 ◽  
Vol 29 (24) ◽  
pp. 1430049 ◽  
Author(s):  
Chanyong Park
Keyword(s):  
Field Theory ◽  
Finite Temperature ◽  
Quasinormal Mode ◽  
Thermodynamic Quantities ◽  
Black Brane ◽  
Zero Temperature ◽  
Hydrodynamic Properties ◽  
Relativistic Field ◽  
Thermal Entropy ◽  
Lifshitz Theory

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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