REFERENCES
1. V. Veselago, The electrodynamics of substances with simultaneously
negative values of and , Sov Phys Usp 92 (1967) 517-526.
2. D.R. Smith, W.J. Padilla, D.C. Vier, S.C. Nemat-Nasser, and S.
Schultz, Composite medium with simultaneously negative permeabil-
ity and permittivity, Phys Rev Lett 84 (2000) 4184-4187.
3. A.A. Oliner, A periodic-structure negative-refractive-index medium
without resonant elements, URSI Dig. IEEE-AP-S USNC/URSI Na-
tional Radio Science Meeting, San Antonio, TX 2002, p. 41.
4. C. Caloz and T. Itoh, Application of the transmission line theory of
left-handed (LH) materials to the realization of a microstrip LH trans-
mission line, Proc IEEE-AP-S USNC/URSI National Radio Science
Meeting, Seattle, WA vol. 2, pp. 412-415.
5. A.K. Iyer and G.V. Eleftheriades, Negative refractive index metama-
terials supporting 2-D waves, Proc IEEE MTT Int Symp 2 (2002),
412-415.
6. R. Marque ´s, J. Martel, F. Mesa, and F. Medina, Left handed media
simulation and transmission of EM waves in sub-wavelength SRR-
loaded metallic waveguides, Phys Rev Lett 89 (2002), 183901-
183903.
7. R.A. Shelby, D.R. Smith, S.C. Nemat-Nasser, and S. Schultz, Micro-
wave transmission through a two-dimensional, isotropic, left-handed
metamaterial, Appl Phys Lett 78 (2001), 489.
8. G.V. Eleftheriades, A.K. Iyer, and P.C. Kremer, Planar negative re-
fractive index media using periodically L-C loaded transmission lines,
IEEE Trans Microwave Theory Tech 50 (2002), 2702-2712.
9. A. Grbic and G.V. Eleftheriades, An isotropic three-dimensional neg-
ative-refractive-index transmission-line metamaterial, J Appl Phys 98
(2005), 043106.
10. G.V. Eleftheriades, O. Siddiqui, and A.K. Iyer, Transmission line
models for negative refractive index media and associated implemen-
tation without excess resonators, IEEE Microwave Wireless Compon
Lett 13 (2003) 51-53.
11. C. Caloz and T. Itoh, Transmission line approach of left-handed (LH)
materials and microstrip implementation of an artificial LH transmis-
sion line, IEEE Trans Antenn Propag 52 (2004), 1159-1166.
12. A. Lai, C. Caloz, and T. Itoh, Composite right/left-handed transmis-
sion line metamaterials, IEEE Microwave Mag 5 (2004), 34-50.
13. B. Jokanovic and V. Crnojevic-Bengin, Novel reconfigurable left-
handed unit cell for filter applications, Proc of PIERS 2007 Conf,
Bejing, China, March 2007.
© 2007 Wiley Periodicals, Inc.
PATTERN RECONFIGURABLE SPIRAL
ANTENNA AND ITS CURRENT
DISTRIBUTION
Amit Mehta,
1
Dariush Mirshekar-Syahkal,
2
and
Hisamatsu Nakano
3
1
Institute of Advance Telecommunications, University of Wales-
Swansea, SA2 8PP, United Kingdom; Corresponding author:
a.mehta@swan.ac.uk
2
Department of Electronics Systems Engineering, University of
Essex, Colchester, CO4 3SQ, United Kingdom
3
Department of Electronics Informatics, Hosei University, Koganei,
184-8584, Tokyo, Japan
Received 14 March 2007
ABSTRACT: Analysis of spiral antenna with open circuits on its arm is
presented for beam adaptive applications. It is shown theoretically and ex-
perimentally that when the open circuits are appropriately positioned in the
arm, the current distribution varies, causing the beam to steer. This effect
can be exploited to design various novel beam switchable antennas. © 2007
Wiley Periodicals, Inc. Microwave Opt Technol Lett 49: 2567–2570, 2007;
Published online in Wiley InterScience (www.interscience.wiley.com).
DOI 10.1002/mop.22738
Key words: spiral antenna; beam steer-ability; switched beam antennas
1. INTRODUCTION
A beam steerable antenna has the potential to improve the
overall wireless communication system performance. In mobile
voice communication, it can ensure that the link is always intact
and locked on to the maximum signal direction, irrespective of the
user movements. It can also facilitate the system to steer away
from electronic jamming, noisy environments, and improving sur-
face absorption rate, effective isotropic radiated power, etc.
Presently, some smart antenna systems for the base-stations
using phased arrays are being investigated and tested [1, 2].
However, the same cannot be implemented in handsets or small
wireless transceivers because of limited space, processing power,
and cost. To accomplish this, an innovative spiral antenna design
is proposed in this paper.
Single arm rectangular spiral antennas radiate a tilted beam
(beam cock) from the active regions [3]. In [4, 5], the authors
showed that a single element spiral antenna, can provide steerable
radiation pattern under electronic control without need of a com-
plex feeding network. The direction of the antenna beam is con-
trolled through a set of switches shorting the spiral arm to the
ground plane at selected points. In [6, 7], an implementation of
MEMS in the arm of single and multi-turn adaptive beam spiral
antennas has been successfully demonstrated.
In this paper, an investigation is presented encompassing the
current distribution and radiation pattern for the spiral antenna
with open arm at two locations. Qualitative reasoning approach is
then offered for pattern reconfigureability. A total of three antenna
configurations are analyzed, namely, SPRL (spiral antenna with no
switching element activated), One-point open spiral (1 switching
element activated) and Two-point open spiral (two switching ele-
ments activated).
The antenna characteristics in the S band, including the radia-
tion pattern, gain, and VSWR, are obtained using the finite-
difference time domain method, and are validated experimentally.
2. ANTENNA CONFIGURATION
Figure 1(a) shows a single arm rectangular spiral antenna, similar
in shape to that in [5]. The substrate for the antenna is composed
of two dielectric layers (for ease of construction) stacked together.
The substrate has side length L = 51.3 mm, net thickness h = 12
mm and effective dielectric constant
r,eff
= 3.41.
The spiral is composed of multiple straight filaments, with the
first filament end-to-end length a = 4.5 mm. The total arm length
of the spiral conductor is = 291 mm and its width is w = 1.35
mm. The antenna is fed by a coaxial line from point o. The
diameter of the feeding conductor is d = 1.3 mm. The junction
point of the top end of the feeding conductor and the starting point
of the spiral arm is referred to as o'.
Two open circuit switches SW1 and SW2 are located at dis-
tance of 125.3 and 155.3 mm from the starting point of spiral arm,
o'. When both switching elements are in deactivated state (off),
i.e., (SW1, SW2) = (off, off), the antenna configuration is referred
to as SPRL (Fig. 1). The antenna configurations with (SW1,
SW2) = (on (activated), off) and (SW1, SW2) = (on, on) are
referred to as One-point open spiral and Two-point open spiral,
respectively. In the experimental study, to simulate the short
circuiting (off) action, the gap is physically short-circuited by
soldering the two parts of the spiral arm at the position of a switch.
Figure 2 shows the prototype of the One-point open spiral and the
Two-point open spiral configurations. In this study the open circuit
gap is 1-mm wide.
DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 49, No. 10, October 2007 2567