CLC number: O441
On-line Access: 2024-08-27
Received: 2023-10-17
Revision Accepted: 2024-05-08
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Okuno Yoichi, Suyama Taikei. Numerical analysis of surface plasmons excited on a thin metal grating[J]. Journal of Zhejiang University Science A, 2006, 7(1): 55-70.
@article{title="Numerical analysis of surface plasmons excited on a thin metal grating",
author="Okuno Yoichi, Suyama Taikei",
journal="Journal of Zhejiang University Science A",
volume="7",
number="1",
pages="55-70",
year="2006",
publisher="Zhejiang University Press & Springer",
doi="10.1631/jzus.2006.A0055"
}
%0 Journal Article
%T Numerical analysis of surface plasmons excited on a thin metal grating
%A Okuno Yoichi
%A Suyama Taikei
%J Journal of Zhejiang University SCIENCE A
%V 7
%N 1
%P 55-70
%@ 1673-565X
%D 2006
%I Zhejiang University Press & Springer
%DOI 10.1631/jzus.2006.A0055
TY - JOUR
T1 - Numerical analysis of surface plasmons excited on a thin metal grating
A1 - Okuno Yoichi
A1 - Suyama Taikei
J0 - Journal of Zhejiang University Science A
VL - 7
IS - 1
SP - 55
EP - 70
%@ 1673-565X
Y1 - 2006
PB - Zhejiang University Press & Springer
ER -
DOI - 10.1631/jzus.2006.A0055
Abstract: The authors numerically investigated the characteristics of surface plasmons excited on a thin metal grating placed in planer or conical mounting. After formulating the problem, the solution method, Yasuura’s method (a modal expansion approach with least-squares boundary matching) was described. Although the grating is periodic in one direction, coupling between TE and TM waves occurs because arbitrary incidence is assumed. This requires the employment of both TE and TM vector modal functions in the analysis. Numerical computations showed: (1) the excitation of surface plasmons with total or partial absorption of incident light; (2) the resonance character of the coefficient of an evanescent order that couples the plasmon surface wave; (3) the field profile and Poynting’s vector. The plasmons excited on the surfaces of a thin metal grating are classified into three types: SISP, SRSP, and LRSP, different from each other in the feature of field profile and energy flow. In addition, the eigenvalue of a plasmon mode was obtained by solving a sequence of diffraction problems with complex-valued angles of incidence and using the quasi-Newton algorithm to predict the real angle of incidence at which the absorption occurs.
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