6120 IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, VOL. 65, NO. 11, NOVEMBER 2017
Communication
Beamwidth Properties of Endfire 1-D Leaky-Wave Antennas
Walter Fuscaldo, David R. Jackson, and Alessandro Galli
Abstract— In this communication, the beam properties
of one-dimensional leaky-wave antennas (1-D LWAs) are explored
when the LWA scanning approaches endfire. By increasing the phase
constant beyond the ordinary endfire condition, smaller beamwidths
can be produced at the expense of increased sidelobe level (SLL). This
tradeoff is quantified here for the first time for endfire 1-D LWAs. Simple
CAD formulas are also proposed that describe accurately the beamwidth
and SLL for 1-D LWAs operating at endfire. This communication is
conducted for different radiation efficiencies covering most practical
ranges. A closed-form expression for the beamwdith of a 1-D LWA with
an infinite aperture is also given, in which case there are no sidelobes.
These results allow for a better understanding and efficient design of
LWAs radiating at endfire.
Index Terms—Beamwidth, endfire antennas, Hansen-Woodyard condi-
tion (HW condition), leaky-wave antennas (LWAs), sidelobe level (SLL).
I. I NTRODUCTION AND MOTIVATION
It is well known that for continuous antenna arrays, as well as for
1-D LWAs, the pointing angle θ
0
and the phase constant β are related
through β = k
0
cos θ
0
, where k
0
is the wavenumber in vacuum. As a
matter of fact, this relation is exact as long as β ≤ k
0
. When β ≥ k
0
the beam points at endfire (θ
0
= 0). Hansen and Woodyard [1] have
shown that a particular value of β allows for improving the directivity
at endfire for a linear array. In particular, they found that the optimum
condition for maximizing directivity at endfire is given by the so-
called Hansen-Woodyard condition (HW condition) [1]
β = k
0
+ 2.94/L (1)
where L is the length of the antenna (see Fig. 1). Since β = k
0
(i.e., θ
0
= 0) corresponds to the ordinary endfire condition
(OE condition), it is seen that the phase shift (β ) given by
β = 2.94/L (2)
represents the perturbation of the OE condition to achieve maximum
directivity at endfire for antenna arrays.
This condition applies only for antenna arrays with a constant
aperture distribution. However, it has recently been demonstrated [2]
that a modified version of (2) can suitably be applied to endfire 1-D
LWAs (see Fig. 1 for an example), which are equivalent to antenna
arrays with an exponentially decaying aperture distribution of the
form exp(- jk
z
z ) where k
z
= β - j α is the complex longitudinal
wavenumber, and α is the attenuation constant (or leakage constant ).
Manuscript received February 8, 2017; revised August 1, 2017; accepted
August 26, 2017. Date of publication September 1, 2017; date of current
version October 27, 2017. (Corresponding author: Walter Fuscaldo.)
W. Fuscaldo is with the Department of Information Engineering, Electronics
and Telecommunications, Sapienza University of Rome, 00184 Rome, Italy,
and also with the Institut d’Électronique et de Télécommunications de Rennes,
UMR CNRS, 6164 Rennes, France, and also with the Université de Rennes 1,
35042 Rennes, France (e-mail: fuscaldo@diet.uniroma1.it).
D. R. Jackson is with the Department of Electrical and Computer Engineer-
ing, University of Houston, Houston, TX 77204-4005 USA.
A. Galli is with the Department of Information Engineering, Electronics
and Telecommunications, Sapienza University of Rome, 00184 Rome, Italy.
Color versions of one or more of the figures in this communication are
available online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TAP.2017.2748363
Fig. 1. Example of a 1-D LWA. A leaky mode is excited at the source
location z = 0. The metallic top wall of a rectangular waveguide is replaced
by a partially reflecting screen to allow the propagating mode to leak out
along the z -axis. The antenna is terminated with a matched load at z = L .
This new condition is known as the modified HW condition (mHW
condition) and it states that
β = τ/L (3)
where τ is a parameter that depends on the radiation efficiency e
r
of
the antenna due to load termination [2].
The above condition gives the phase constant necessary for achiev-
ing the maximum directivity from a 1-D LWA. This does not imply,
however, a minimum beamwidth. In this communication, we explore
the beamwidth properties of a 1-D LWA when the beam is scanned
beyond OE (β > k
0
) showing that beamwidths smaller than in
the HW condition are possible, but at the expense of an increased
sidelobe level (SLL). This tradeoff is quantified, and simple CAD
formulas are introduced for the beamwidth and the SLL in terms of
the phase constant and the radiation efficiency of the antenna. These
formulas are accurate for the range of radiation efficiencies usually
encountered in LWA design, where the efficiency e
r
(due to a load
termination) is less than 95%.
The nature of the beam changes when the aperture becomes very
large, corresponding to very high radiation efficiencies. A separate
formula, which is exact, is derived for the beamwidth in the infinite
aperture case, when the beam is scanned to or beyond OE. In this
case there are no sidelobes, and the beamwidth is only a function of
the phase and attenuation constants.
The formulas derived here assume a single leaky wave on the
aperture, with a complex wavenumber. In a practical LWA, there will
usually be some amount of space-wave radiation or mode coupling
that takes place as the beam is scanned to and beyond endfire, since
the leaky mode is then entering into the “spectral gap” region where
it begins to lose physical significance [3]. The degree to which this
happens is structure specific, however, and such effects should be
considered on a case-by-case basis. An example of this is discussed
in [4].
It is worth mentioning here that general beamwidth formulas for
1-D unidirectional LWAs have recently appeared in [5]. However,
in that work, exact and approximate analytical expressions are
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