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© 2003 Wiley Periodicals, Inc.
META-MATERIAL SURFACE DESIGN
USING THE HIERARCHICAL GENETIC
ALGORITHM
Yuan Yuan,
1
Chi Hou Chan,
1
Kim Fung Man,
2
and
Kwai Man Luk
1
1
Wireless Communications Research Laboratory
City University of Hong Kong
83 Tat Chee Ave, Kowloon, Hong Kong SAR, China
2
Department of Electronic Engineering
City University of Hong Kong
83 Tat Chee Ave, Kowloon, Hong Kong SAR, China
Received 14 April 2003
ABSTRACT: In this paper, we design a meta-material surface emulat-
ing a perfect magnetic conducting plane (PMC) using the hierarchical
genetic algorithm (HGA). This is achieved by manipulating the unit-cell
geometry of frequency-selective surface screens and the electrical prop-
erties of the supporting dielectric medium in the optimization process.
The properties of the structure are evaluated using a method of mo-
ments (MoM)-based electromagnetic solver. By virtue of the HGA, prior
information of the number of FSS screens and dielectric layers is not
required. The designed PMC is employed as a dipole-antenna reflector
for gain enhancement. © 2003 Wiley Periodicals, Inc. Microwave Opt
Technol Lett 39: 226 –230, 2003; Published online in Wiley InterScience
(www.interscience.wiley.com). DOI 10.1002/mop.11176
Key words: meta material; genetic algorithm; electromagnetic simula-
tion
INTRODUCTION
Meta-material is a complex “artificial” material that does not exist
in nature; one example is the perfect magnetic conductor (PMC),
which can be very useful in a wide variety of microwave applica-
tions. Recently, electromagnetic bandgap (EBG) structures have
been widely investigated for mimicking a PMC [1, 2]. They are in
the form of frequency-selective surfaces with multiple screens and
multiple dielectric layers backed by a perfect electric conducting
ground plane [3–5]. This configuration is desirable for its low cost
and easy realization. However, the design procedure is very chal-
lenging as there are many parameters involved, for instance, the
unit-cell geometry of each screen, and the thickness of the dielec-
tric layers and their electric properties. More importantly, the
number of FSS screens and dielectric layers needs to be specified
a priori before adopting an optimization procedure.
The hierarchical genetic algorithm (HGA) [8] is an emerging
optimization algorithm, which can simultaneously precede struc-
tural and parametric system optimization [6, 7]. The desirable
properties of the meta-material surface are the magnitude and
phase of the reflection coefficient equal to unity and 0°, respec-
tively. The reflection coefficient is computed by the method of
moments (MoM)-based electromagnetic solver [5] and is con-
verted into a fitness value based on the design specification.
Following the rule of “survival of the fittest,” HGA can globally
find the best solution whose properties mostly match the design
specification. The realization of the frequency-selective-based
PMC demonstrates the efficiency and suitability of HGA.
In this paper, the design of a 5.8-GHz meta-material surface
acting as a PMC using HGA is presented. The number of FSS
screens and dielectric layers are not specified, but will be deter-
mined by the optimization process. This PMC surface is employed
as a reflector for a dipole antenna. For the dipole antenna’s
resonance frequency shifting, the dipole should be placed at a little
distance from the PMC. The measured gain of the dipole is
increased by 3 dB in the broadside direction when compared to the
same dipole radiating in free space. The same measured gain is
obtained if the dipole is backed by a PEC reflector that is set at a
quarter-wavelength distance away from the dipole. This measure-
ment confirms that the meta-material surface indeed acts as a
PMC.
HIERARCHICAL GENETIC ALGORITHM
Hierarchical genetic algorithm (HGA) has a newly formulated
chromosome structure inspired by the complex hierarchical chro-
mosome structure in nature. The hierarchical chromosome consists
of two levels of genes, the control and parametric genes, so that it
can provide a unique solution for simultaneous parametric and
system structural search.
For the frequency-selective-surface-based meta-material, there
are many design parameters that should be taken into consider-
ation. These include the number of screen and dielectric layers,
dielectric constant, thickness of each dielectric layer, and unit-cell
geometry. Even for the conventional genetic algorithm, there are
too many parameters to be optimized. However, the control genes
Figure 1 Unit-cell geometry of the FSS screen. [Color figure can be
viewed in the online issue, which is available at www.interscience.wiley.
com.]
Figure 2 Structure of the designed FSS-based meta-material surface to
be operated at 5.8 GHz. [Color figure can be viewed in the online issue,
which is available at www.interscience.wiley.com.]
226 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 39, No. 3, November 5 2003