диафрагмированные волноводные фильтры / 74401997-02d4-4392-9774-fc584e0ba0be
.pdfWaveguide Switchable Bandstop and Bandpass
Filters Using RF MEMS Switches
K. Y. Chan, R. Ramer
School of Electrical Engineering and Telecommunications
The University of New South Wales
Sydney, Australia kyc@unsw.edu.au, ror@unsw.edu.au
Abstract—Waveguide switchable bandstop and bandpass |
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filter designs are demonstrated in this paper. The designs are |
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based on the design of rectangular waveguide that has |
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switching |
planar |
bandstop |
resonators |
inserted |
on the |
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Switching |
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MEMS model |
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ON-state |
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OFF-state |
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sidewall. These |
switchable |
bandstop |
resonators |
consist |
of |
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Elements |
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Resonator |
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two identical metal patches separated by switching elements. |
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Length (L) |
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The |
switching |
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elements |
can |
be |
of |
RF |
MEMS |
or |
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b |
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semiconductor transistor type. These resonators allow |
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electrically switching of the waveguide while providing close |
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(a) |
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Transistor model |
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ON-state |
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OFF-state |
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to ideal on-state insertion loss and narrow stop band during |
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off-state. These switches permit the switchable bandstop and |
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bandpass filters design. The concept is demonstrated for a |
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switchable five-pole bandstop filter and a switchable three- |
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pole bandpass filter, both at the centre frequency of 14.25 |
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GHz and for 500 MHz bandwidth. |
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Switches off |
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Switches on |
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I. INTRODUCTION |
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(c) |
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Multi-band operation will become |
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a |
standard |
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Fig. |
1. |
(a) |
Switchable |
planar |
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resonator located |
inside |
a |
typical |
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in rectangular |
waveguide, |
(b) |
the |
designs |
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and |
circuit models |
when |
using |
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adaptive |
and |
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reconfigurable |
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RF |
frontends. |
Achieving |
MEMS and transistors, and (c) the EM propagation when the switches |
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multi-standard |
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while |
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maintaining |
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low-cost |
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andare off and on. |
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compactness are becoming a trend in |
communication |
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II. WAVEGUIDE SWITCH DESIGN |
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systems. Devices in the RF frontend, such as antennas, |
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switches, matching networks, phase shifters, directional |
to |
The design of our waveguide switch is based on a low |
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couplers |
and |
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filters, |
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will |
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all |
be |
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required |
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be |
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Q-factor switchable planar resonator. This resonator is |
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reconfigurable in the future. Some |
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antenna |
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designs designed |
to |
operate |
within a |
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rectangular |
waveguide, |
in |
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showing promising results have been |
reported |
[1-5]. |
particular, attached |
on |
the |
narrow sidewall, |
as illustrated |
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However, |
the most |
critical |
ones, |
switches and |
filters, |
still |
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in |
Fig. |
1. |
The concept |
utilizes |
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the |
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planar |
resonator |
to |
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require significant research and development, especially in |
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create |
a |
bandstop |
notch |
at |
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a narrow band of frequencies |
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the |
waveguide |
technology. |
If |
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conventional |
waveguide |
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when |
the switches |
between the |
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two |
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patches are |
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enabled. |
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switches, typically rotary mechanical are well researched |
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When the switches are disabled, the band |
stop |
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notch |
is |
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and competing with the semiconductor PIN diodes, FET |
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switches |
and |
RF |
MEMS |
the |
reconfigurable |
waveguide |
also disabled and therefore, the waveguide will permit |
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filter research is still limited [6]-19]. |
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transmission. |
The |
switching |
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elements |
can |
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be |
of |
RF |
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Reconfigurable filters reported in the literature |
were |
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MEMS type or semiconductor transistor type. Due to the |
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most utilizing semiconductor PIN diodes and FET types, |
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planar nature, only low Q-factor value could be achieved |
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ferroelectric type, and RF MEMS type |
switches |
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and |
even when the resonator is operating inside a waveguide. |
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varactors. They offer the necessary reconfigurability and |
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They |
are |
easy |
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to |
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fabricate |
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and |
can |
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be |
switche |
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the required bandwidth; their achievable |
Q-factors |
are |
electronically with minimal special modification to the |
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limited when compared with the waveguide counterparts. |
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waveguide. |
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One solution to achieve waveguide reconfigurable filters is |
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to combine waveguide switches with filters. To authors’ |
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knowledge, partial research has been performed. Most |
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researchers only reported waveguide switches aiming to |
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improve either size and cost or the RF performance. One |
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group reported movable MEMS cantilevers with ridge |
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waveguide [20]. Another utilised a reconfigurable mesh |
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with MEMS actuator that covers the entire propagation |
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plane |
[21]. |
In this paper, a concept |
of |
combining |
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waveguide switches together with filters |
together |
is |
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presented. The basic waveguide switch will be discussed, |
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followed by the bandstop and bandpass filter examples. |
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(a) |
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978-1-7281-2168-0/19/$31.00 ©2019 IEEE
Authorized licensed use limited to: University of Canberra. Downloaded on June 06,2020 at 13:23:39 UTC from IEEE Xplore. Restrictions apply.
(b)
(c)
Fig. 2. Simulated (a) centre frequency 0(),f (b) phase(φ), and (c)x/Z0, with different L and W values.
III. WAVEGUIDE SWITCHABLE BANDSTOP FILTER DESIGN
A bandstop filter (5-pole) using Fig. 2 and the topology in Fig. 3, with the simulation model, is given in Fig. 4; the planar resonators are placed on a quartz substrate (500um
thick) at the narrow sidewall of the WR62 |
waveguide. |
With switches inserted at the centre of each resonator, on |
|
and off states were achieved, and Fig. |
5 shows the |
simulation results. As can be seen from the simulations, when the switches are on, the desired bandstop filter is enabled. This stop band has a 500 MHz bandwidth with a rejection of -20 dB. Due to the low Q-factor of the planar
resonators, |
the in-band return |
loss |
(S) has a significant |
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11 |
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loss. However, this is not a |
critical issue |
for most |
||
bandstop |
filter requirements |
as |
the in-band |
reflected |
power is excessive. When the resonators’ switches are on, the waveguide behaves as a typical rectangular waveguide with a minimal insertion loss and a return loss of better than 20 dB for the band of interest.
Fig. 4. Waveguide switchable bandstop filter simulation model.
With these resonators, the waveguide switch is only capable of operating with a very narrow bandwidth, as the resonance only occurs at a single frequency. In order to achieve a wider bandwidth, unique designs are required. One method of achieving wider bandwidth is to cascade band stop notches to form a bandstop filter. However, in order to design a bandstop filter properly, it is essential to
determine the equivalent circuit model of |
the |
planar |
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resonator operating in a rectangular waveguide with TE |
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mode as the only propagating mode. |
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10 |
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Three properties have to be studied in order to produce |
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an equivalent circuit model; they |
are |
the |
resonance |
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frequency, f0, the equivalent guided length,φ, and the |
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normalized reactance, x/Z0. |
These parameters |
can |
be |
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calculated by analyzing the S-parameters and correlating |
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|||||
them with the L and W of the resonator. As an example, a |
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bandstop waveguide filter with a |
centre |
frequency |
of |
|||
14.25 GHz and a bandwidth of 500 MHz will be studied. |
|
|||||
Fig. 2 demonstrated the simulation results. As can |
be |
|||||
noticed, different normalized |
reactance |
and guided |
phase |
|
lengths are achievable at a single frequency. By using a bandstop filter topology as in Fig. 3 and proper L and W
values, different filters |
with |
customised |
bandwidths can |
||
be achieved. |
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-φ1 |
-φ1 |
-φ2 |
-φ2 |
-φ3 |
-φ3 |
1 |
λ |
2 |
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λ |
3 |
4 |
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4 |
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0 |
0 |
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0 |
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Fig. 3. bandstop filter topology with guided length,φ, the normalized reactance, x/Z0, and the guided wavelength λ.
(a)
(b)
Fig. 5. Waveguide switchable bandstop filter simulation results: (a) on state and (b) off state.
IV. WAVEGUIDE SWITCHABLE BANDPASS FILTER DESIGN
These switchable resonators could be used to design
waveguide switchable |
bandpass |
filters. However, the |
designs have to be |
based |
on traditional rectangular |
bandpass filter topologies. As an example, a waveguide iris bandpass filter with a centre frequency of 14.25 GHz and a bandwidth of 500 MHz was selected as the basis of the design. The concept is to insert a switchable bandstop resonator into each rectangular waveguide cavity. Fig. 6
Authorized licensed use limited to: University of Canberra. Downloaded on June 06,2020 at 13:23:39 UTC from IEEE Xplore. Restrictions apply.
shows |
the |
circuit |
model |
of |
one |
|
switchable |
resonator |
|
Ratio and Reduced Sidelobe Level,"IEEE Antennas and Wireless |
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placed |
within |
a waveguide |
cavity. |
As |
in |
the |
figure, |
the |
[2] |
Propagation Letters, vol. 15, pp. 1835-1838, 2016. |
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cavity resonance is generated with a waveguide section of |
Y. Yang, Y. Cai, K. Y. Chan, R. Ramer, and Y. J. Guo, "MEMS- |
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Loaded Millimeter Wave Frequency Reconfigurable Quasi-Yagi |
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λ/2 long bounded by two impedance inverters. When the |
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Dipole |
Antenna," Microwave Conference Proceedings (APMC), |
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planar resonator is enabled, the switch in Fig. 6 is enabled |
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2011 Asia-Pacific, 2011, pp. 1318-1321: IEEE. |
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allowing |
a |
shorted |
path |
within |
the |
resonant |
cavity |
and |
[3] |
G. I. Kiani, T. S. Bird, and K. Y. Chan, "MEMS Enabled |
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effectively disabling the cavity resonance. Fig. 7(a) shows |
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Frequency Selective Surface for 60 GHz Applications,"Antennas |
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and Propagation (APSURSI), 2011 IEEE International |
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half of the simulated model of the switchable bandpass |
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Symposium on, 2011, pp. 2268-2269: IEEE. |
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filter (three-pole). Fig. 7(b) |
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illustrates |
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the |
simulation |
[4] |
Y. Yang, K. Y. Chan, N. Nikolic, and R. Ramer, "Experimental |
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results |
when |
the |
switches |
are |
on |
and |
off. |
As |
expected |
|
Proof for Pattern Reconfigurability of 60GHz Quasi Yagi |
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from |
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the |
circuit |
model, |
the |
passband, |
14 |
to |
14.5 |
GHz |
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Antenna," Microwave and Optical Technology Letters, vol. |
57, |
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no. 1, pp. 84-88, 2015. |
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either has a perfect transmission when the switches are |
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L. |
Gong, |
K. Chan, and R. Ramer, "A Split-Ring Structures |
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disabled (off) or has a high rejection |
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when |
the switches |
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Loaded Siw Sectorial Horn Antenna,"Antennas and Propagation |
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are enabled |
(on). However, |
as |
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noticed, |
when |
the |
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in Wireless Communications (APWC), 2015 IEEE-APS Topical |
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switches |
are |
enabled, |
the |
out-of-band |
performance |
has |
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Conference on, 2015, pp. 349-350: IEEE. |
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[6] |
F. Huang, S. Fouladi, and R. R. Mansour, "High-Q Tunable |
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significant changes and could be unacceptable for some |
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Dielectric Resonator Filters Using Mems Technology,"IEEE |
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applications. |
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Transactions on Microwave Theory and Techniques, vol. 59, no. |
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12, pp. 3401-3409, 2011. |
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λ/4 |
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λ/4 |
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[7] F. Huang and R. Mansour, "A Novel Varactor Tuned Dielectric |
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Resonator |
Filter," IEEE |
MTT-S |
International |
Microwave |
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Symposium Digest (IMS), Seattle, WA, USA, 2013, pp. 1-3. |
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Kij |
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Kij |
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[8] |
H. Joshi, H. H. Sigmarsson, M. Sungwook, D. Peroulis, and W. J. |
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Chappell, |
"High-Q Fully Reconfigurable Tunable |
Bandpass |
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Filters," IEEE Transactions on Microwave Theory and |
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Fig. 6. |
A proposed circuit model of a switchable planar resonator placed |
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[9] |
X. Liu, L. P. B. Katehi, W. J. Chappell, and D. Peroulis, "High-Q |
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within a rectangular waveguide resonator that is bounded by impedance |
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Tunable Microwave Cavity Resonators and |
Filters |
Using Soi- |
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inverters. |
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Rf |
Mems |
Tuners,"Journal |
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Systems, vol. 19, no. 4, pp. 774-784, 2010. |
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[10] |
F. Gentili, F. Cacciamani, V. Nocella, R. Sorrentino, and L. |
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rW |
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Pelliccia, "Rf Mems Hairpin Filter with Three Reconfigurable |
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WR62 |
rL |
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Bandwidth |
States," European Microwave |
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2013, pp. 802-805. |
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t |
L1 |
t |
L2 |
t |
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L1 |
t |
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[11] |
F. Gentili, V. Nocella, L. Pelliccia, F. Cacciamani, P. Farinelli, |
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and R. Sorrentino, "Mems-Based Fine Tuning of High Q-Factor |
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(a) |
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[12] F. Gentili, |
L. Pelliccia, R. Sorrentino, and G. Bianchi, "High Q- |
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Factor Compact Filters with Wide-Band Spurious Rejection," |
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[13] L. Pelliccia, P. Farinelli, R. Sorrentino, G. Cannone, G. Favre, and |
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P. |
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Coassini, |
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"K-Band |
Mems-Based |
Frequency |
Adjustable |
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[14] H. Rahman, K. Y. Chan, Y. Yang, and R. Ramer, "Fabrication of |
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RF |
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NEMS |
Series |
Switch |
Using |
Surface |
Micromachining," |
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IASTED Intl. Conf. on Nanotechnology and Applications, 2010. |
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[15] Y. X. Yang, |
K. Y. Chan, and R. Ramer, |
"Wideband |
RF Nano |
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Switch |
Matrix," Antennas |
and |
Propagation (APSURSI), 2011 |
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(b) |
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IEEE International Symposium on, 2011, pp. 1605-1608: IEEE. |
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[16] |
E. Siew, K. Y. Chan, R. Ramer, and A. Dzurak, "Design of a RF |
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Fig. 7. (a) Half of the iris waveguide filter loaded with planar switchable |
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Nems |
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Switch |
Matrix,"Antennas and Propagation (APSURSI), |
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resonators and (b) its simulation results showing the on and off states. |
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2011 IEEE International Symposium on, 2011, pp. 12-15: IEEE. |
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V. |
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CONCLUSIONS |
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[17] |
X. Li, K. Y. Chan, and R. Ramer, "Fabrication of through Via |
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Holes in Ultra-Thin Fused Silica Wafers for Microwave and |
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This paper presented electrically-controlled waveguide |
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Millimeter-Wave Applications," Micromachines, vol. 9, |
no. 3, p. |
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138, 2018. |
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switches, switchable bandpass and bandstop filter designs |
[18] |
L. Gong, K. Y. Chan, and R. Ramer, "A Third Order Bandpass |
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using |
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switchable |
resonators. |
A |
five-pole |
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bandstop |
filter |
|
Iris Filter with Reconfigurable Dielectric Irises,"Microwave and |
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and a three-pole bandpass filter demonstrating their |
|
Optical Technology Letters, vol. 60, no. 5, pp. 1287-1290, 2018. |
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[19] |
L. Gong, K. Y. Chan, and R. Ramer, "A |
Four-State |
Iris |
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corresponding on and off states with their simulated RF |
|
Waveguide Bandpass Filter with Switchable Irises,"Microwave |
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performance are shown. The design examples confirmed |
|
Symposium (IMS), 2017 IEEE MTT-S International, |
2017, pp. |
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the versatility of our approach, illustrated the potential of |
|
260-263: IEEE. |
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||||||||||||||||||||||||||
such |
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designs |
and |
|
highlighted |
the |
|
simplicity |
|
of |
their |
[20] |
M. Daneshmand, R. R. Mansour, and N. Sarkar, "RF MEMS |
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fabrication. |
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Waveguide H-Plane Horn Antenna with Improved Front-to-Back |
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