64 IEEE ANTENNAS AND WIRELESS PROPAGATION LETTERS, VOL. 8, 2009
Design and Realization of a Linearly Polarized
Eleven Feed for 1–10 GHz
Jian Yang, Xiaoming Chen, Niklas Wadefalk, and Per-Simon Kildal, Fellow, IEEE
Abstract—A new linearly polarized Eleven feed for operation
between 1 and 10 GHz is presented. This frequency band is higher
than the realized before, and the input reflection coefficient is
better than dB over the frequency range, which also is an
improvement over previous models. The log-periodic dipole petals
have been designed by using a simple one-by-one parameter
optimization scheme with a simulation tool based on moment
method. The final analysis has been improved by applying an
finite-difference time-domain (FDTD)-based solver for the central
part of the feed and then a circuit network program to combine
the results of the center part with the result of the dipole panels.
The antenna has been manufactured by printed circuit board
(PCB) technology on a metalized Kevlar sheet in order to obtain
better tolerances and smaller dimensions than in previous models.
Measurements show agreement with the analysis.
Index Terms—Eleven antenna, optimization, reflector feed.
I. INTRODUCTION
W
IDE-FREQUENCY band antenna systems are re-
quired for many new and future applications, such
as in radio astronomy and ultrawideband (UWB) communi-
cation technology [1], [2]. Therefore, research on more than
octaves bandwidth antennas has gained a lot of attentions
[2]–[5]. The radio astronomy applications are mainly the SKA
project ( Square Kilometer Array) and the VLBI2010
project ( Very Long Baseline Interferometry). Both of
these projects have reflector antennas as candidates covering
1–13 GHz or even higher, whereas the UWB systems require
small direct radiating antennas covering typically 3–10 GHz.
Thus, the frequency ranges are similar, although the require-
ments are quite different.
Chalmers University of Technology in Gothenburg, Sweden,
has during the last years been developing a new decade band-
width log-periodic dual-dipole antenna referred to as the Eleven
antenna [6], which has resulted in dually polarized hardware
below 3 GHz for use in different radio telescopes [7]–[9]. The
development of Eleven feed has also gained attention from other
researchers and been applied to other applications [10]. The
Manuscript received November 11, 2008; revised December 04, 2008. First
published December 22, 2008; current version published April 17, 2009. This
work was supported in part by the Swedish Foundation for Strategic Research
(SSF) within the Strategic Research Center Charmant.
J. Yang, X. Chen, and P.-S. Kildal are with the Department of Signals and Sys-
tems, Chalmers University of Technology, 412 96 Gothenburg, Sweden (e-mail:
jian.yang@chalmers.se).
N. Wadefalk is with the Department of Microtechnology and Nanoscience,
Chalmers University of Technology, 412 96 Gothenburg, Sweden.
Color versions of one or more of the figures in this letter are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/LAWP.2008.2011148
Fig. 1. Configuration of Eleven feed of single polarization.
basic geometry of the Eleven antenna is two parallel dipoles
separated by half wavelength and located above a ground plane.
Both dipoles are cascaded in log-periodic arrays in order to
achieve the wide bandwidth (see Fig. 1). The cascading was
most easily performed by folded dipoles. The Eleven antenna
has very good features: nearly constant beamwidth with about
10 dBi directivity and fixed phase center location over the whole
bandwidth, low profile, and simple geometry. Therefore, the
Eleven antenna is well-suited to feed reflectors, and at frequen-
cies above 1 GHz its size is so small that it would fit into a
Dewar and could be cooled together with the low-noise am-
plifier (LNA) in low-noise applications such as VLBI2010 and
SKA. The Eleven antenna could also provide tracking patterns
for use in Earth terminals for satellite communications [11]. The
purpose of the present letter is to present a new design of an
Eleven antenna with better performance and realized at higher
frequencies than before, which can make it a better candidate
for the SKA and VLBI2010 projects.
In low-noise systems one of the most critical performance
parameters is the input reflection coefficient because strong
reflection at the antenna input port will cause noise mismatch
to the LNA and increase the system noise level. In the present
work, we are therefore focusing on optimizing the geometry
of the feed to obtain better performance of the reflection
coefficient than in previous models. We also introduce a man-
ufacturing technology that can be used at 10 GHz and higher.
Due to the very wide frequency band, the size of the whole
feed becomes very large in terms of wavelength at the highest
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