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19 Sep 2019

19 Sep 2019

# Design of leaky-wave antennas with transverse slots for end-fire radiation with optimized radiation efficiency

Thomas Vaupel and Claudius Löcker

**Thomas Vaupel and Claudius Löcker**Thomas Vaupel and Claudius Löcker

- Fraunhofer Institute for High Frequency Physics and Radar Techniques, Fraunhofer Str. 20, 53343 Wachtberg, Germany

- Fraunhofer Institute for High Frequency Physics and Radar Techniques, Fraunhofer Str. 20, 53343 Wachtberg, Germany

**Correspondence**: Thomas Vaupel (thomas.vaupel@fhr.fraunhofer.de)

**Correspondence**: Thomas Vaupel (thomas.vaupel@fhr.fraunhofer.de)

Received: 19 Feb 2019 – Revised: 03 May 2019 – Accepted: 08 May 2019 – Published: 19 Sep 2019

A substrate integrated waveguide (SIW) with transverse slots on the top plane can be used to design an effective leaky-wave antenna with good frequency beam-scanning and platform integration capability. For a main beam near end-fire, the phase constant of the radiating wave must be near to the free space wavenumber or slightly larger. In this context, the modified Hansen-Woodyard condition gives an optimum phase constant to maximize the directivity at end-fire. For the analysis of the wave propagation we have implemented a modal analysis for rectangular waveguides with transverse slots. Near end-fire, three types of modal solutions exists, a leaky improper mode, a surface wave mode and a proper waveguide mode. The leaky mode can reach phase constants larger than the free space wavenumber to fulfill the Hansen-Woodyard condition, but loses strongly its physical significance in this slow wave region, thus the excitation of the leaky-wave becomes negligible there, whereas the proper waveguide mode is dominant but exhibits only a negligible radiation loss leading to a strong drop of the antenna efficiency. Therefore, the optimum efficiency of 86 % for maximizing the gain as proposed in the literature cannot be reached with this kind of leaky wave antenna.

But it will be shown in this contribution by analyzing antenna structures with finite aperture lengths, that the efficiency can reach nearly 100 % if the phase constant of the leaky-wave meets exactly the free space wavenumber (ordinary end-fire condition) and the aperture length is adjusted with regard to the attenuation constant of the leaky-wave from the modal analysis. For a given aperture length, a procedure is outlined to adjust the attenuation constant in several steps at the desired ordinary end-fire frequency to reach maximum gain and efficiency.

Figure 1a, shows the configuration with infinite length and filled
rectangular waveguide used for the modal analysis in the space domain (Liu
and Jackson, 2011). This analysis searches for the complex propagation
wavenumber ${k}_{z}=\mathit{\beta}-j\mathit{\alpha}$ which sets the corresponding
transcendental equation to zero (Eq. 7 in Liu and Jackson, 2011). For this
search, we use the downhill-method (Bach, 1969), leading to convergent
results typically with around 50 steps. The first design is based on the
following values related to a wavelength *λ*_{o, e}, which
corresponds to the free space wavenumber at the frequency of ordinary
end-fire operation *f*_{o, e}, see text below. Due to non-disclosure
reasons, the exact frequencies (in the *K*_{u}-band) and design parameters
must not be specified: slot length $L=\mathrm{0.16}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$, slot width
$W=\mathrm{0.025}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$, periodicity $p=\mathrm{0.15}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$,
$b=\mathrm{0.44}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$, $a={w}_{\mathrm{eff}}=\mathrm{0.3}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$ and the dielectric
filling *ε*_{r}=3.5. In Fig. 2b, the modal analysis of
the propagation constant *β*∕*k*_{0} is given. For frequencies larger
than *f*_{o, e}, the leaky-wave (blue) and the proper waveguide mode (green)
have a $\mathit{\beta}/{k}_{\mathrm{0}}>\mathrm{1}$. According to O'Connor and Jackson (2011), the (modified) Hansen-Woodyard condition for highest directivity and
gain with an aperture length of $\approx \mathrm{20}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$ should be
fulfilled for $\mathit{\beta}/{k}_{\mathrm{0}}\approx \mathrm{1.023}$ reached around $\mathrm{1.0076}{f}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}={f}_{H.W.}$, the frequency where
the Hansen-Woodyard condition is fulfilled. According to Fig. 2b, the attenuation
constant with dielectric losses reaches $\mathit{\alpha}/{k}_{\mathrm{0}}=\mathrm{0.0161}$ at ${f}_{H.W.}$ (blue curve at red bar). But if the structure is analyzed with a finite
length as in Fig. 1b, the attenuation drops down for frequencies
beyond the ordinary end-fire operation.

This can be recognized by the behaviour of |*S*_{12}| reaching a
minimum exactly at the ordinary end-fire frequency with −9.21 dB and a
radiation efficiency of *e*_{r}=88 *%* and then increases strongly to −4.73 dB (*e*_{r}=66 *%*) where the modified Hansen-Woodyard condition should be
fulfilled (see Fig. 3b).

This is due to the fact, that the leaky mode becomes unphysical beyond
end-fire and the proper waveguide mode becomes dominant with a low
attenuation only due to dielectric and metallic losses, thus |*S*_{12}| becomes larger.

This can also be observed in Fig. 2b, where the red curve shows only
a small increase somewhat before *f*_{o, e}. Figure 3b shows the
radiation pattern at ordinary end-fire (blue) with a maximum gain of 18.19 dBi, whereas the gain curve at the Hansen-Woodyard condition shows only a
maximum of 14.93 dBi mainly due to the lower radiation efficiency. According
to Liu and Jackson (2012), the contribution of the leaky-wave drops down to
about 10 % at ordinary end-fire, whereas the surface-wave mode may
show a maximum contribution around this frequency.

Obviously the leaky-wave is transformed into the surface-wave over the aperture length in such a way that the attenuation constant for the leaky-wave derived from the modal analysis is still valid for the radiating mechanism of both leaky and surface-wave mode up to the frequency of ordinary end-fire. Since the excitation of the surface wave drops down beyond the ordinary end-fire frequency, the efficiency of 86 % at the modified Hansen-Woodyard condition for gain maximization as proposed in O'Connor and Jackson (2010) cannot be reached. Therefore we propose as follows a gain improvement at the ordinary end-fire frequency by a procedure of step-wise increasing the attenuation constant to maximize the efficiency derived by

and to maximize the gain at ordinary end-fire.

The attenuation constant can be increased by enlarging the slot length
and/or the slot width and/or decreasing the slot periodicity. But with fixed
width of the waveguide, also the values of *β*∕*k*_{0} are increasing.
This can be compensated by decreasing the width of the waveguide. A good
estimation for the modification of the width by Δ*w*_{eff} is given by
(similar as in Liu and Jackson, 2014)

where $\mathit{\beta}(L,\phantom{\rule{0.125em}{0ex}}W,\phantom{\rule{0.125em}{0ex}}{w}_{\mathrm{eff}},\phantom{\rule{0.125em}{0ex}}p)$ is the propagation constant with the current
*w*_{eff} and *β*_{desired} is the desired propagation constant for
the given $L,\phantom{\rule{0.125em}{0ex}}W,\phantom{\rule{0.125em}{0ex}}p$ of the slots. However, in most cases it is faster to use a
linear interpolation to find the exact *w*_{eff}: If *β* is too large,
*w*_{eff} is slightly decreased and from the new value for *β*, the
exact *w*_{eff} can be often determined with one interpolation step. We have
now implemented this method as an iterative procedure in our modal analysis
program showing typically a very good convergence in 2 to 4 steps with a
maximum deviation for *β*_{desired}∕*k*_{0} of 0.001.

In Table 1, the *α*∕*k*_{0} with the parameter set No. 1 is doubled in 6 steps only by reduction of the periodicity *p*
($L=\mathrm{0.173}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$, and $W=\mathrm{0.0254}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$ remain constant),
keeping the *β*∕*k*_{0} at the ordinary end-fire value for the constant
frequency *f*_{o, e} using the modal analysis and the interpolation sketched
above. The values for the maximum gain are derived with HFSS with the
aperture length of the structure in Fig. 1b. Further results of the
simulations with HFSS are given in Fig. 4. The minima of |*S*_{12}| become monotonously smaller, for the parameter sets No. 1 to No. 4
we have still a small frequency offset, but from parameter set No. 5 the
frequency with maximum attenuation at the desired frequency *f*_{o, e} is
also met by the HFSS-simulations. With Eq. (1) we get an efficiency of 97 % for No. 6 and 99 % for No. 7, thus a further increase of the
attenuation constant is not meaningful and would lead to a gain reduction.
Figure 4b shows the gain pattern of No. 7 for different frequencies .

The gain is, depending on frequency, up to 1.4 dBi higher for No. 7 compared with the parameter set No. 1. A radiation exactly in end-fire direction is not possible due to diffraction effects of the finite groundplanes.

Since the antennas are fabricated in SIW-technology, we still need a
SI-waveguide with width *w* and the same propagation constant as the
rectangular waveguide with width *w*_{eff}=*a* (see also Fig. 5a). In
many cases the formula (e.g. Kumar and Jadhav, 2012)

Equation (3) is not correct enough. With *d*=0.6 mm and *s*=0.8815 mm we get
$w=\mathrm{0.3229}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$ with Eq. (3) what leads to a minimum of |*S*_{12}| around 100 MHz higher than the desired *f*_{o, e}. But if we
take the formula

derived in Kordiboroujeni and Bornemann (2013), we get $w=\mathrm{0.3248}{\mathit{\lambda}}_{\mathrm{o},\phantom{\rule{0.125em}{0ex}}\mathrm{e}}$ slightly higher, the minimum is shifted to the desired *f*_{o, e} again and
we get the same gain behaviour as with a rectangular waveguide.

For the practical implementation we need also a microstrip-SIW transition, which is sketched in Fig. 5, showing a good matching behavior with low losses and a bandwidth of about 18 %.

To reach a higher gain also for frequencies below end-fire, we have also examined structures with two antenna branches. In this context we need a power divider with low losses. A suitable microstrip divider with additional detour line is outlined in Fig. 6 with the input port 3. We have used rounded bends to minimize the parasitic radiation leading to losses of only about 0.6 dB (Weisshaar and Tripathi, 1990). A power divider with mitered bends could be optimized for a good matching behaviour, but the losses amount to about 1.5 dB mainly due to the parasitic radiation of the mitered bends. A structure with two antenna branches with a center distance of 10 mm is given in Fig. 7a.

Figure 7b shows the peak gain comparison with one and two branches. Due to mechanical constraints, the SMP-connector must be located alongside the branches thus the additional detour line is needed. The SMP-connector is linked to the microstrip line with an additional matching section .

The maximum gain of the structure with one branch drops down to 18.4 dBi at
*f*_{o, e} (compared with the structure No. 7 with 19.58 dBi) due to the
additional detour line, microstrip-SIW transition and the SMP-connector. But
with two branches we get a maximum gain of 19.42 dBi and for frequencies
below end-fire, the peak gain is typically 3 dB higher compared with the
structure with only one branch.

Leaky-wave antennas in SIW-technology with transverse slots are a good candidate, if a frequency scanning capability up to end-fire and a cheap fabrication is desired. To increase the directivity and gain at end-fire operation, the (modified) Hansen-Woodyard condition may be applied. To fulfill this condition, the propagation constant of the radiating mode must be slightly higher than the free space wavenumber. However, in this slow wave region the leaky-wave becomes unphysical and also the excitation of the surface wave mode drops down strongly beyond the ordinary end-fire operation. But it could be found, that the leaky-wave is transformed into the surface wave at the frequency of ordinary end-fire and that for the radiation loss computation along the aperture still the attenuation constant of the leaky-wave can be used which is derived from a modal analysis based on rectangular waveguides. With this modal analysis, we have outlined a procedure to stepwise increase the attenuation constant e.g. by decreasing the periodicity of the slots and decreasing the width of the waveguide to get a radiation efficiency of about 99 % adjusted to the length of the aperture. After a careful transformation of the rectangular waveguide into a SIW together with an efficient microstrip-SIW transition, a cheap fabrication is possible. With the use of power dividers with low losses, structures with two antenna branches can be designed leading to a gain improvement also for frequencies below end-fire operation.

There are no underlying research data for the presented work due to non-disclosure reasons. The results can be reproduced with the design methods and equations given in the paper.

The authors declare that they have no conflict of interest.

This article is part of the special issue “Kleinheubacher Berichte 2018”. It is a result of the Kleinheubacher Tagung 2018, Miltenberg, Germany, 24–26 September 2018.

This paper was edited by Thomas Eibert and reviewed by three anonymous referees.

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