This paper proposes the design of a Ku-band filter based on dielectric
loaded combline resonators for high power space applications.
The requirements of the ESA ARTES AT project, named DOMUK
(Dielectric-loaded high-power Output de-MUltiplexer at Ku/Ka-band,
ESA Contract Number: 4000125645/19/NL/NR) were considered as
a benchmark. In this scenario, output De-Multiplexers (ODEMUXs)
are used in current multi-beam Ku/Ka systems to separate the signals
intended for each beam. A large number of identical ODEMUXs are
required in multi-beam systems due to the nature of the frequency reuse
scheme. This implies very stringent requirements for the ODEMUX
in terms of mass and footprint. There are numerous solutions in the
literature to achieve more compact and lightweight filter structures
without compromise the radio frequency (RF) performance. A
general description of the techniques and technologies related to
filter development is presented in -. Dielectric resonators (DRs) are the preferred solution to minimize volume occupancy by
high-permittivity (εr) materials. This solution is widely used for Input
Multiplexer (IMUX) channels in all bands, and for high power Output
Multiplexer (OMUX) channels in C-band. However, this approach
is limited to moderate power levels per channel when considering
K-band OMUXs with narrow bandwidth. The design of a high-power
Ku-band filter is described in this paper where the architectures and
materials have been carefully chosen to improve the performance of
the filter with respect to power handling and multipactor up to 150 W
of input RF power.
Several promising solutions could be adopted for our purpose; TM010
or TE01δ dielectric resonator mode-based filters are an example. TE01δ
modes could represent the best compromise to obtain compact
filters where low losses and high discharge handling capability are
required. On the other hand, the main drawback of this solution
concerns the thermal management  since the DR is not directly
joined to the metal cavity of the filter, but is supported by a material
with low dielectric permittivity generally characterized by a very poor
thermal conductivity. With respect to the TM010 mode solution, the
main limitation concerns the mechanical stability of the dielectricmetal
contact . In fact, the different Coefficients of Thermal
Expansion (CTE) of the metal cavity and the ceramic element can
produce detachment at the interfaces of the two materials when the
operating temperature changes. Any small airgaps are sufficient to
worsen the filter response as the boundary conditions change. In
this scenario, dielectric combline resonators  would likely be
a good compromise to minimize the critical aspects that could be
encountered using the TM010 or TE01δ approaches.
The design of a high-power sixth-order pseudo-elliptic filter based on
dielectric combline resonators is proposed in this paper. Preliminary
results are also described in  and , however this paper shows
updates in which two similar filter models are proposed using different
permittivity values of the dielectric elements. The 3D filter models
were designed using the Ansys software suite, in particular HFSS
was used for electromagnetic design while Ansys Mechanical was
chosen to simulate the mechanical/thermal performance. Details of
the software configuration and the results achieved are also presented
in the paper, along with the preliminary test results.
The basic 3D model of the dielectric loaded combline resonators
designed using Ansys HFSS software is shown in Fig. 1. The metal
cavity is loaded by the dielectric cylinder with high permittivity values
in order to increase the volume and mass saving (more than 50%)
compared to standard TE113 resonators. The dielectric element is
only joined to one side of the cavity, as shown in Fig. 1b.
Two sixth-order filter models were designed considering the different
permittivity values of commercially available dielectric elements. The
proposed resonator model for the filters is presented in Fig. 2; the
high permittivity dielectric element is mixed with “barrel-shaped”
metal cavity. Fig. 2a shows the combline resonator, which is based
on ceramic material characterized by a permittivity of 12.6 and low
loss-tangent (8e-5). This solution allows for a very compact structure
while maintaining high unloaded Q-factor values (>4500) when
considering a standard square cavity.
According to  and , along with the cavity height, the shape of the
cavity can also be optimized to improve the Q-factor. It is well-known
that a spherical shaped cavity is the best solution to maximize the
Q-factor, however this approach could become critical to achieve the
required coupling values for our filter since it increases the distance
between two adjacent resonators.
Fig. 2 - Proposed dielectric loaded combline resonator designed in Ansys HFSS: a) side view of resonator with εr=12.6, b) side view of resonator with εr=24, c) 3D view of resonator with background conditions of metallic cavity.
Fig. 3 - 3D view of sixth-order Ku-band filters: a) Model 1 (εr=12.6), b) Model 2 (εr=24).
Fig. 4 - Top views of sixth-order Ku-band filters: a) Model 1 (εr=12.6), b) Model 2 (εr=24).
Based on preliminary eigenmode analyses  performed in HFSS,
the best cavity shape to further improve the Q-factor is the “Barrel”
which allows the simulated unloaded Q-factor of the resonator in
Fig. 2a to be increased up to 6000. In ,  multiple parametric
analyses were performed in HFSS with respect to the variation of
the main parameters such as the radius of dielectric cylinder, cavity
height, and curvature of the barrel cavity. As a result, (see Fig. 2a),
the required aspect ratio of the ceramic cylinder to maximize the
unloaded Q-factor is very high but a potentially vibration-sensitive
structure is obtained. Therefore, support mechanisms (Teflon cups)
were used to lock the ceramic cylinder in place on the top of the
cavity. Along with the properties of the dielectric elements, the nonideal
characteristics of metallic material are also considered. The
finite conductivity background conditions used in the models shown
in Fig. 2a and Fig. 2b are set in order to consider the loss contribution
due to the metal casing, as shown in Fig. 2c. Aluminum’s similar bulk
conductivity (σ=3e7 S/m) was also considered despite a silvering
process having been performed on the cavity surfaces, which allows
for a margin over than the desired true Q-factor.
In Fig. 2, the first prototype resonator (Fig. 2a) is compared with a
smaller barrel-shaped resonator (Fig. 2b) in which a ceramic material
with higher permittivity is used. Due to εr=24, additional shrinkage
of the structure is achieved while maintaining a sufficiently high
unloaded Q-factor value (about 4000-5000). The barrel shape of
the cavity is less pronounced in the second resonator solution. To
increase the “barrel-shape” to be similar to the first prototype, the
diameter of the ceramic cylinder must be decreased. However, in this
case, a minimum diameter of 2 mm was chosen to avoid possible
criticality due to the robustness of the ceramic parts; for this reason a
less pronounced barrel was obtained.
Two sixth-order elliptical filter models were
designed using the dielectric loaded combline
resonators in Fig. 2. The 3D models of proposed
Ku-band filters are compared in Fig. 3 where the
difference in size is highlighted.
Both filters are based on the same folded
configuration in which all positive couplings
between adjacent resonators are used while a
negative cross-coupling has been designed
between the non-adjacent resonators 2-5 to
achieve two transmission zeros (TZs) in the lower
and upper stop bands. The difference in footprint
is shown in Fig. 4 where top views of the filters are
Fig. 5 - Ku-band filter duplet for coupling design: a) Input coupling design model, b) Intra-positive coupling design model, c) Negative cross-coupling design Model 1, d) Negative cross-coupling design Model 2.
The intra-couplings were designed by simulating odd and even
resonant modes (eigenmode analysis) between each resonator
duplet; whereas the Group Delay (GD) method was used to design the
input couplings  where the WR75 waveguide interface was used.
In this scenario, the GD of the reflection characteristic was simulated
by performing a Driven Modal analysis of the S-parameters in HFSS.
The models used to design the input and intra-couplings are shown
in Figs. 5a and 5b, respectively, while Figs. 5c and 5d are the models
used to design the negative cross-couplings.
In the first filter model in Fig. 3a, the negative cross-coupling was
achieved by using a capacitive iris loaded with high-permittivity
(εr=24) material . This cross-coupling solution is impractical
in the second filter model because the smaller size of the structure
does not allow the desired negative coupling value to be achieved.
However, in this case the cross-coupling was achieved by designing
a shaped metal probe supported by a Teflon interface (Fig. 5d).
In the first filter model (Fig. 3a), tuning screws were added to the cavity
and coupling irises to compensate for the variation in filter response
due to manufacturing tolerances. Similar tuning mechanisms can be
used in the second filter model, however the structure shown in Fig.
3b is only a preliminary model, and the tuning screws are not present.
Driven Modal simulations were performed in HFSS to simulate and
optimize the S-parameters of both sixth-order Ku-band filters. In
each case, the wave-ports were defined as signal excitations of the
3D model while the adaptive meshing solutions were used for the
simulation setup. The central frequency of the filter (11 GHz) was
chosen as the single solution frequency. Concerning the mesh,
curvilinear elements were applied since the models show numerous
curved surfaces. The full-wave response of the first sixth-order filter
model (Fig. 3a) is shown in Fig. 6, while the simulated S-parameters
of the second prototype (Fig. 3b) are depicted in Fig. 7. Both
simulations converged with a maximum Delta-S magnitude of less
All in-band and out-of-band requirements (Fig. 6) are satisfied in
the case of the first filter model. Return loss (RL) greater than 19 dB
and insertion loss (IL) less than 0.8 dB are over the entire passband
(240 MHz), while all near-band rejection requirements are met due to the TZs. Regarding the second filter model, similar results were
obtained but a wider bandwidth was achieved despite using the
higher permittivity values of the ceramic elements have been used.
This shows that “strong” coupling values can be achieved with the
proposed design even though the E-field is more confined within the
Fig. 6 - Simulated response of Ku-band filter Model 1 (blue line is transmission
characteristic, red line is reflection characteristic).
Fig. 7 - Simulated response of Ku-band filter Model 2 (blue line is transmission
characteristic, red line is reflection characteristic).
Fig. 8 - Ansys vibration analysis of the sixth-order filter Model 1.
Fig. 9 - Ansys and HFSS high-power thermal simulations of the sixth-order filter Model 1
at the central frequency.
The first model was chosen for manufacturing because it is less
critical in terms of manufacturing tolerances, and therefore additional
analyses were performed during the design procedure. Vibration
analyses were performed in Ansys Mechanical to identify the first
mechanical resonance mode of the sixth-order filter in Fig. 3a.
As shown in Figs. 8a and 8b, the first modes are at 4059.9 Hz for
the aluminum casing and at 2245.9 Hz for the ceramic cylinders,
respectively; these are above the range of the specification for the
vibration level (2000 Hz). Simulated results of the high-power thermal
analyses performed at the central frequency are shown in Fig. 9.
A combination of HFSS and Mechanical simulations in Ansys
Workbench was used to calculate the thermal drift with 150 W input
power and to calculate the thermal drift of the S-parameter response.
The simulations were performed including all physical properties of
the metallic and dielectric parts. The estimated change in relative
permittivity over the predicted temperature for the dielectric parts
was also considered. A similar high-power thermal analysis was
also performed at the passband edge frequency. The maximum
temperature is reached on the ceramic elements, in particular the
maximum temperature is 130 °C for the central frequency and 200 °C
for the passband edge.
Concerning the thermal drift of the frequency, the maximum shift
estimated by simulation is in the range 8÷16 MHz corresponding
to 5÷8 ppm/°C (higher for the edge frequency, and lower for the
central frequency). Fig. 10 shows the high-power thermal results of
the analysis at the passband edge frequency.
High-power thermal simulations were also performed on the second
filter model. However, the estimated temperature rise is greater due
to the smaller volume and the smaller heat transfer surfaces. The
maximum temperature reached on the ceramics is over 200°C.
Fig. 10 - Ansys and HFSS high-power thermal simulation of the sixth-order Model 1
filter at the edge of the passband.
The first sixth-order Ku-band filter model was manufactured by
achieving a volume reduction of about 50% compared to a standard
filter based on the TE113 resonators, while keeping the Q-factor values
compliant with the requirements. Fig. 11 shows the prototype of the
manufactured filter and its 3D mechanical model, the structure is made
of silver-plated aluminum. The final size (LxWxH) is 92mm x 45mm x
41mm with a mass of less than 200g in accordance with expectations.
The comparison between the measured (solid lines) and simulated
(dashed lines) responses is shown in Fig. 12. According to ,
the measured response has shifted upward in frequency by about
100 MHz compared to the simulated response in Fig. 6. This is
attributed to the actual value of the dielectric constant of the ceramic
resonators that have a tolerance that is difficult to compensate for
using only tuning screws. The actual value of the permittivity of the
dielectric elements (εr=12.4) was used in the simulation for a proper
comparison with the measurement as shown in Fig. 12.
The measured unloaded Q-factor is above 4500 as expected, and the
out-of-band attenuation is very good taking into account the frequency
shift. In addition, the insertion loss of less than 1 dB (objective) over
the entire passband is compliant.
According to , the final environmental and high-power tests
were also performed in this filter model and promising results were obtained. Fig. 13 shows the RF breakdown test setup in which the
filter is placed inside the Thermal Vacuum Chamber (TVAC).
Two compact sixth-order Ku-band elliptic filters for high-power
satellite applications were designed as part of an ESA ARTES
AT project in which compactness and power-handling in space
environment are key requirements. In this paper, filters based
on TM dielectric-loaded combline resonators combined with
barrel-shaped cavities were presented in this paper and first
experimental results are shown. Filter design and simulation were
performed using Ansys software from both electronic and thermomechanical
perspectives. In both filter cases, the geometries and
materials were carefully chosen in order to improve the highpower
performance in terms of power-handling and multipactor.
A first model was designed considering dielectric resonators with
permittivity of 12.6 achieving volume and mass savings of about 50%
compared to standard TE113 resonators. A second smaller prototype
was proposed using ceramic elements with higher permittivity
(εr=24), however only a detailed analysis of the first model was
performed and it was chosen for preliminary manufacturing and
testing processes since it is less critical in term of manufacturing
tolerances. In this scenario, the measured filter response of the
first model shows promising results with an unloaded extrapolated
Q-factor of about 4900.
According to preliminary test , multipactor discharges up to
1400 W at the central frequency were not obtained, while 130 W at
continuous wave (CW) concerns the maximum power achieved from
the power-handling point of view, which is slightly lower than the
expected value (150 W). During the power-handling test, there was a
non-negligible temperature rise in line with that predicted by thermomechanical
Newsletter EnginSoft Year 18 n°3
By Paolo Vallerotonda | RF Microtech - University of Perugia
Fabrizio Cacciamani | RF Microtech
Luca Pelliccia | RF Microtech
Francesco Aquino | RF Microtech
Cristiano Tomassoni | University of Perugia
Vittorio Tornielli di Crestvolant | ESA ESTEC
The filters described in this paper are the outcome of the ESA ARTES
AT project named DOMUK (ESA Contract Number: 4000125645/19/
NL/NR). We would like to thank the staff of ESA ESTEC (in Noordwijk,
The Netherlands), ESA-VSC Lab (in Valencia, Spain) and the University
of Perugia (in Perugia, Italy) for their contributions and support.
This work is dedicated to the memory of Prof. Roberto Sorrentino,
whose work, honesty, and integrity will forever inspire his past
students and colleagues towards excellence.
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Ku-Band Filter for High-power Space Applications based on
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Conference (EuMW), London, February 2022.
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Barrel-shaped Ku-band filter for High-power Satellite
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