Abstract:A new class of compact, high-Q, tunable coaxial filters is presented in this paper based on a novel inset resonator concept. The tuning concept is based on the displacement of movable resonators inside a properly modified metallic housing which features wide tuning capabilities and stable high Qfactor performance with minimum variation throughout the tuning window. Various prototypes are designed and implemented to demonstrate and validate the proposed concept. A single tunable inset resonator is first designe… Show more
“…It is known from [42] that the physical inter-resonator (IR) and input-output (IO) couplings should also change with the frequency tuning to maintain a constant ABW and a stable return loss level. In practice, keeping this harmony is a very challenging task, especially for broad tuning ranges.…”
Section: B Design Guidelines Of Octave Tunable Filters With Constant ...mentioning
confidence: 99%
“…The desired design is an octave tunable filter from 2.67 GHz to 1.17 GHz (tuning ratio 2.28:1) with a constant 20-dB bandwidth of 38 MHz. Following the design procedure of CABW tunable filters detailed in [42], the required K 12 × f product and reflection group delay are calculated as 0.063 and 11.2 nS, respectively. Then, one M5 tuning screw and two M2 tuning screws were introduced at both filters to obtain the desired IR and IO couplings, respectively.…”
Section: Tunable Cabw Two-pole Bandpass Filter: Re-entrant Caps Vs Tu...mentioning
confidence: 99%
“…The filter is designed to operate from 2.86 GHz to 1.34 GHz with a constant 20-dB bandwidth of 71 MHz. Similar to the previous example, the design procedure begins from the desired reflection group delay (8.3 nS) and IR couplings (K (12,34) × f = 0.066, K 23 × f = 0.05) calculation based on [42]. Next, the required reflection group delay is realized through the IO feeding structure with the aid of two M3 tuning screws as shown in Fig.…”
“…For instance, a 4-pole 180 MHz K-band reconfigurable TE 311 waveguide filter was presented in [29] with 1.74% of frequency tuning and a Q factor from 3100 to 2600 using dielectric plates. To this end, coaxial and dielectric-loaded waveguides have gained more interest in many tunable filter applications due to their advantages of miniaturized structures, high Q, and good power handling capabilities [3], [30], [31], [32], [33], [34], [35], [36], [37], [38], [39], [40], [41], [42], [43], [44], [45], [46], [47], [48], [49]. For example, a CABW tunable coaxial filter was reported in [3] for future agile 5G Base Transceiver Stations (BTSs).…”
Section: Introductionmentioning
confidence: 99%
“…The filter operates from 942.5 MHz to 737.5 MHz (24.4%) with a CABW of 23 MHz±8% and a quality factor ranges from 2900 to 2300. Also in [41] and [42], our group recently presented 40% tunable CABW coaxial filters with the least variation of Q factor over the tuning window using inset resonators. To provide more compactness and a higher Q factor than the coaxial filters, a couple of tunable dielectric resonator (DR) filters were proposed [43], [44], [45], [46], [47], [48], [49].…”
This paper reports octave tunable dielectric combline bandpass filters with constant absolute bandwidth (CABW) using a novel re-entrant cap tuning technique. The resonant frequency is tuned by the hollow re-entrant cap penetrating into the filter cavity as an envelope around the dielectric resonator. This mechanism of tuning provides wider tuning capabilities and better spurious performance than the conventional screw-based tuning. Also, the cap tuners can be employed effectively to tune the input-output and inter-resonator couplings simultaneously with the frequency reconfiguration, enabling a CABW over a wide frequency tuning window. For proof of concept purposes, a single widely tunable resonator is presented with octave tuning ratio of 2.64:1, high quality factor from 1705 to 5480, and spurious-free band up to 3.44• f 0 . Afterwards, two octave tunable re-entrant cap filters are designed, fabricated, and tested. The first filter is a 78% widely tunable two-pole filter with a CABW of 43.5±12% MHz, low insertion loss equals to 0.28±0.03 dB, and a compact volume of 39 cm 3 . The second design is a four-pole octave tunable bandpass filter from 2.96 GHz to 1.36 GHz with a constant 69±13% MHz bandwidth, low insertion loss better than 0.6 dB, return loss higher than 16 dB, and a compact 62 cm 3 structure. According to our own knowledge, thanks to the proposed tuning mechanism, the presented designs are the first CABW octave tunable high Q waveguide-based filters, having the widest tuning ranges over all similar state-of-the-art-designs. Cap, constant bandwidth, dielectric resonator, high-performance, re-entrant, tunable.
INDEX TERMS
“…It is known from [42] that the physical inter-resonator (IR) and input-output (IO) couplings should also change with the frequency tuning to maintain a constant ABW and a stable return loss level. In practice, keeping this harmony is a very challenging task, especially for broad tuning ranges.…”
Section: B Design Guidelines Of Octave Tunable Filters With Constant ...mentioning
confidence: 99%
“…The desired design is an octave tunable filter from 2.67 GHz to 1.17 GHz (tuning ratio 2.28:1) with a constant 20-dB bandwidth of 38 MHz. Following the design procedure of CABW tunable filters detailed in [42], the required K 12 × f product and reflection group delay are calculated as 0.063 and 11.2 nS, respectively. Then, one M5 tuning screw and two M2 tuning screws were introduced at both filters to obtain the desired IR and IO couplings, respectively.…”
Section: Tunable Cabw Two-pole Bandpass Filter: Re-entrant Caps Vs Tu...mentioning
confidence: 99%
“…The filter is designed to operate from 2.86 GHz to 1.34 GHz with a constant 20-dB bandwidth of 71 MHz. Similar to the previous example, the design procedure begins from the desired reflection group delay (8.3 nS) and IR couplings (K (12,34) × f = 0.066, K 23 × f = 0.05) calculation based on [42]. Next, the required reflection group delay is realized through the IO feeding structure with the aid of two M3 tuning screws as shown in Fig.…”
“…For instance, a 4-pole 180 MHz K-band reconfigurable TE 311 waveguide filter was presented in [29] with 1.74% of frequency tuning and a Q factor from 3100 to 2600 using dielectric plates. To this end, coaxial and dielectric-loaded waveguides have gained more interest in many tunable filter applications due to their advantages of miniaturized structures, high Q, and good power handling capabilities [3], [30], [31], [32], [33], [34], [35], [36], [37], [38], [39], [40], [41], [42], [43], [44], [45], [46], [47], [48], [49]. For example, a CABW tunable coaxial filter was reported in [3] for future agile 5G Base Transceiver Stations (BTSs).…”
Section: Introductionmentioning
confidence: 99%
“…The filter operates from 942.5 MHz to 737.5 MHz (24.4%) with a CABW of 23 MHz±8% and a quality factor ranges from 2900 to 2300. Also in [41] and [42], our group recently presented 40% tunable CABW coaxial filters with the least variation of Q factor over the tuning window using inset resonators. To provide more compactness and a higher Q factor than the coaxial filters, a couple of tunable dielectric resonator (DR) filters were proposed [43], [44], [45], [46], [47], [48], [49].…”
This paper reports octave tunable dielectric combline bandpass filters with constant absolute bandwidth (CABW) using a novel re-entrant cap tuning technique. The resonant frequency is tuned by the hollow re-entrant cap penetrating into the filter cavity as an envelope around the dielectric resonator. This mechanism of tuning provides wider tuning capabilities and better spurious performance than the conventional screw-based tuning. Also, the cap tuners can be employed effectively to tune the input-output and inter-resonator couplings simultaneously with the frequency reconfiguration, enabling a CABW over a wide frequency tuning window. For proof of concept purposes, a single widely tunable resonator is presented with octave tuning ratio of 2.64:1, high quality factor from 1705 to 5480, and spurious-free band up to 3.44• f 0 . Afterwards, two octave tunable re-entrant cap filters are designed, fabricated, and tested. The first filter is a 78% widely tunable two-pole filter with a CABW of 43.5±12% MHz, low insertion loss equals to 0.28±0.03 dB, and a compact volume of 39 cm 3 . The second design is a four-pole octave tunable bandpass filter from 2.96 GHz to 1.36 GHz with a constant 69±13% MHz bandwidth, low insertion loss better than 0.6 dB, return loss higher than 16 dB, and a compact 62 cm 3 structure. According to our own knowledge, thanks to the proposed tuning mechanism, the presented designs are the first CABW octave tunable high Q waveguide-based filters, having the widest tuning ranges over all similar state-of-the-art-designs. Cap, constant bandwidth, dielectric resonator, high-performance, re-entrant, tunable.
INDEX TERMS
This article reports a novel inset resonator configuration for coaxial filter applications with quasi-elliptic responses. The design and analysis of the inset resonator are discussed in detail and accurately modeled as a capacitively-loaded stepped-impedance half-wavelength resonator featuring more compactness, high quality factor, and enhanced spurious responses in comparison with conventional halfwavelength and combline resonators. Additionally, the operating frequency can be tuned intrinsically through the displacement of the coaxial resonator, eliminating the need for any additional tuning elements and maintaining a stable quality factor. Two quasi-elliptic inset resonator type filters are implemented in planar and longitudinal coupling configurations, respectively. The first takes the form of a folded four-pole 2.93 GHz filter with two symmetrical transmission zeros. The fabricated filter has a compact structure of 29.76 cm 3 , an insertion loss better than 0.73 dB, a return loss better than 18 dB, and a wide spurious-free band up to 3.5•f 0 . The second inset-type quasi-elliptic filter is realized in a longitudinal inline arrangement. An example of a 2.53 GHz three-pole filter is presented with a closely-positioned transmission zero, wide spurious-free band (≈3•f 0 ), and a very compact structure of 55.7×33×33 mm 3 .
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