Near- and Far-Field Properties of Plasmonic Oligomers under Radially and Azimuthally Polarized Light Excitation

ACS Nano ◽  
2014 ◽  
Vol 8 (5) ◽  
pp. 4969-4974 ◽  
Author(s):  
Avner Yanai ◽  
Meir Grajower ◽  
Gilad M. Lerman ◽  
Mario Hentschel ◽  
Harald Giessen ◽  
...  
1996 ◽  
Vol 13 (5) ◽  
pp. 1000 ◽  
Author(s):  
D. Robart ◽  
T. Amand ◽  
X. Marie ◽  
M. Brousseau ◽  
J. Barrau ◽  
...  

2020 ◽  
Vol 59 (8) ◽  
pp. 2621
Author(s):  
Zhou Hui ◽  
Li Song ◽  
Zhang Wenhao ◽  
Chen Yuwei

1991 ◽  
Vol 30 (Part 1, No. 11A) ◽  
pp. 2797-2801 ◽  
Author(s):  
Masami Susaki ◽  
Hiromichi Horinaka ◽  
Nobuyuki Yamamoto

Symmetry ◽  
2020 ◽  
Vol 12 (11) ◽  
pp. 1790
Author(s):  
Mehmet Ali Kuntman ◽  
Ertan Kuntman ◽  
Oriol Arteaga

We study the scattering of polarized light by two equal corner stacked Au nanorods that exhibit strong electromagnetic coupling. In the far field, this plasmonic dimer manifests very prominent asymmetric scattering in the transverse direction. Calculations based on a system of two coupled oscillators, as well as simulations based on the boundary element method, show that, while in one configuration both vertical and horizontal polarization states are scattered to the detector, when we interchange the source and the detector, the scattered intensity of the horizontal polarization drops to zero. Following Perrin’s criterion, it can be shown that this system, as well as any other linear system not involving magneto-optical effects, obeys the optical reciprocity principle. We show that the optical response of the plasmonic dimer, while preserving electromagnetic reciprocity, can be used for the non-reciprocal transfer of signals at a subwavelength scale.


2016 ◽  
Vol 24 (10) ◽  
pp. 11002 ◽  
Author(s):  
Gang Chen ◽  
Kun Zhang ◽  
Anping Yu ◽  
Xianyou Wang ◽  
Zhihai Zhang ◽  
...  

2007 ◽  
Vol 06 (03n04) ◽  
pp. 191-195
Author(s):  
G. V. BENEMANSKAYA ◽  
V. P. EVTIKHIEV ◽  
G. E. FRANK-KAMENETSKAYA

The method of photoyield spectroscopy with s- and p-polarized light excitation is developed for studies of 2D collective modes. The formation of nanoclusters has been studied for the Cs / GaAs (100) Ga -rich interface in a wide coverage range up to ~ 2 ML. Two adsorption phases with the strong Cs – Ga bonding and weak Cs – Cs bonding are found by using both stepwise and dynamic Cs deposition regimes. In the first adsorption phase, local interaction of Cs adatoms with Ga dimers occurs. The transition from the first to the second phase is found to take place at ~ 0.7 ML that corresponds to the saturation of all the Ga -dangling bonds. In the second phase, collective modes in quasi-2D Cs clusters of several sizes depending on the coverage and surface plasmon are revealed.


2021 ◽  
Vol 2015 (1) ◽  
pp. 012145
Author(s):  
N S Solodovchenko ◽  
T Z Seidov ◽  
K B Samusev ◽  
M F Limonov

Abstract In this paper we present the results of numerical calculations of electromagnetic properties for cylindrical ring resonators (RRs) with rectangular cross-section and a dielectric permittivity corresponding to silicon ε = 12. The calculation of the scattering spectrum (Radar Cross Section) and the field distribution of the modes were performed at in-plane polarized light excitation. The presence of four side walls in the RRs determines a richer spectrum of eigenmodes in comparison with cylindrical whispering gallery modes of disk resonators and creates more possibilities and diversity for their practical applications.


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