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Modified Debye model parameters of metals applicable for broadba...
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The finite-difference time-domain method can provide broadband results if the excitation source is a pulse. This demands that the parameters of modeled materials have to be applicable over broad frequency bands. We optimize the modified Debye model parameters for gold, silver, copper, platinum, and aluminum using a large-scale nonlinear optimization algorithm. The complex relative permittivities calculated using the optimized parameters agree well with experimental values over broad frequency ba
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Modified Debye model parameters of metals applicable
for broadband calculations
Hongfeng Gai, Jia Wang, and Qian Tian
The finite-difference time-domain method can provide broadband results if the excitation source is a
pulse. This demands that the parameters of modeled materials have to be applicable over broad frequency
bands. We optimize the modified Debye model parameters for gold, silver, copper, platinum, and alumi-
num using a large-scale nonlinear optimization algorithm. The complex relative permittivities calculated
using the optimized parameters agree well with experimental values over broad frequency bands. The
associated root-mean-square deviations are 0.49%, 3.52%, 4.13%, 1.64%, and 0.66%, respectively. We also
provide an example of broadband calculations. The obtained broadband results are verified by a series of
steady-state calculations. © 2007 Optical Society of America
OCIS codes: 120.4530, 160.3900, 310.0310.
1. Introduction
The finite-difference time-domain (FDTD) method
1
is one of the most popular numerical methods for
solving electromagnetic problems with arbitrary
geometries
2–4
and inhomogeneous materials. One of
the major advantages of FDTD is that broadband
results can be obtained with the FDTD algorithm
run only once, taking a pulse as the excitation
source.
5
This will dramatically save calculation
time compared with a series of steady-state calcu-
lations. However, the parameters of modeled mate-
rials have to be applicable over broad frequency
bands in order to perform broadband calculations.
Here we focus our attention on real metals, which
are dispersive materials. Because the constitutive
parameters (, , , and ) must be specified as
constants in FDTD simulations,
5
the modified De-
bye model (MDM)
5
is usually used to describe the
frequency-dependent behavior of metals. It is very
difficult to optimize the MDM parameters of a metal
so that they are applicable over a broad frequency
band. Krug et al. have tried to get gold parameters in
the near-infrared range.
6
But their results deviate
seriously from the experimental values.
7
Jin et al.
have recently determined gold parameters applicable
in the wavelength range 550–950 nm.
8
Nevertheless,
the parameters for other types of metals have not
been reported to our knowledge. Because of the lack
of appropriate parameters, researchers usually take
a perfect electric conductor to construct their simu-
lation models,
9,10
where the effect of real metals can-
not be considered. The MDM parameters of metals
that are applicable over broad frequency bands are
urgently desired.
In this paper, we optimize MDM parameters for
gold, silver, copper, platinum, and aluminum, using a
large-scale nonlinear optimization algorithm. At the
end, we provide an example on calculating the broad-
band power throughputs of a circular aperture. The
broadband results are verified by a series of steady-
state calculations. This study is important because it
reports the MDM parameters of metals that are ap-
plicable over broad frequency bands.
2. Optimization Method and Results
The frequency-dependent permittivity function of the
MDM is
5
ˆ
共
兲
⫽
⬁
⫹
s
⫺
⬁
1 ⫹ i
⫹
i
0
⫽⬘ ⫺ i ⬙, (1)
where ˆ is the complex relative permittivity, is the
angular frequency,
⬁
is the infinite-frequency rela-
tive permittivity,
s
is the zero-frequency relative
permittivity (static relative permittivity), i is the
imaginary unit, is the relaxation time, is the
H. Gai (gaihf99@mails.tsinghua.edu.cn), J. Wang, and Q. Tian
are with the State Key Laboratory of Precision Measurement Tech-
nology and Instruments, Department of Precision Instruments,
Tsinghua University, Beijing 100084, China.
Received 14 November 2006; accepted 8 January 2007; posted 10
January 2007 (Doc. ID 77012); published 3 April 2007.
0003-6935/07/122229-05$15.00/0
© 2007 Optical Society of America
20 April 2007 兾 Vol. 46, No. 12 兾 APPLIED OPTICS 2229
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