scholarly journals Scattering of surface plasmon polaritons by one-dimensional inhomogeneities

2007 ◽  
Vol 75 (3) ◽  
Author(s):  
A. Yu. Nikitin ◽  
F. López-Tejeira ◽  
L. Martín-Moreno
2018 ◽  
Vol 115 ◽  
pp. 78-87 ◽  
Author(s):  
Abdolrahman Namdar ◽  
Rana Feizollahi Onsoroudi ◽  
Habib Khoshsima ◽  
Mostafa Sahrai

2021 ◽  
Vol 46 (3) ◽  
pp. 604
Author(s):  
Xiang-Jun Li ◽  
Gang Cheng ◽  
De-Xian Yan ◽  
Xiao-Mei Hou ◽  
Guo-Hua Qiu ◽  
...  

2004 ◽  
Vol 18 (23) ◽  
pp. 1181-1188 ◽  
Author(s):  
XIANGANG LUO ◽  
HAO WANG ◽  
JIEPING SHI ◽  
HANMIN YAO

The transmission properties of rectangular one-dimensional unperforated metallic periodic structures for frequencies close to the surface plasmon band are investigated experimentally and theoretically. The results reveal that it is possible to obtain unexpectedly large transmissions through thick unperforated metallic structures. The mechanisms of enhanced transmissions are attributed to resonant excitations of three kinds of plasmon radiations: coupled surface plasmon polaritons, horizontal localized groove plasmon mode, and vertical localized groove plasmons mode. Once the surface plasmon polaritons and the vertical groove plasmon modes are excited simultaneously, the transmission approaches to maximum at the coincident condition.


2015 ◽  
Vol 2015 ◽  
pp. 1-5
Author(s):  
Munazza Zulfiqar Ali

The transmission of surface plasmon polaritons through a one-dimensional periodic structure is considered theoretically by using the transfer matrix approach. The periodic structure is assumed to have alternate left-handed metamaterial and dielectric layers. Both transverse electric and transverse magnetic modes of surface plasmon polaritons exist in this structure. It is found that, for nonlinear wave propagation, tunneling structures are formed to transform nontransmitting frequencies into transmitting frequencies and hence transmission bistability is observed. It is further observed that the structure shows sensitivity with respect to the polarization of the electromagnetic field for this phenomenon.


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