Configuration of the half‐mode substrate‐integrated waveguide band‐pass filter loaded by (A) the conventional complementary split‐ring resonator unit‐cell and (B) the proposed modified complementary split‐ring resonator unit‐cell

Configuration of the half‐mode substrate‐integrated waveguide band‐pass filter loaded by (A) the conventional complementary split‐ring resonator unit‐cell and (B) the proposed modified complementary split‐ring resonator unit‐cell

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A novel super compact filter based on half‐mode substrate‐integrated waveguide (HMSIW) technology loaded by the modified complementary split‐ring resonator (MCSRR) is proposed. The working principle of the proposed filter is based on the evanescent‐mode propagation technique. According to this technique, by loading the complementary split‐ring reso...

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... Hereat, the development of the wide suppression band filters with compact size and low-cost have become a challenging issue for the researchers. So as to overcome these challenging issues, many new filter design topologies and configurations such as photonic bandgap (PBG) [8], split ring resonators (CSRR) [9], stepped impedance resonator (SIR) [10], substrate integrated waveguides (SIW) [11] and defected ground structures (DGS) [12][13][14][15][16][17][18][19][20][21][22][23] have been proposed in the literature. According to the finding of the previous studies, it was observed that DGS technique can achieve more compact and wider suppression bandwidth rather than other configurations [24]. ...
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This article deals with design and development of a novel 7th order low-pass filter with defected ground structures for S-band applications. The proposed LPF structure was comprised of dumbbell shaped interdigital defected ground structures and open stubs as series inductor and shunt capacitor in the pass band. In addition, an equivalent circuit model was derived and optimized to achieve a 3-dB cut off frequency about 4 GHz with a reflection coefficient of better than −20 dB. Moreover, proposed low-pass filter was manufactured on a Rogers RO4003C substrate with a dielectric constant of 3.38, the dissipation factor of 0.0027. The developed LPF has a very flat pass-band with a transmission coefficient less than −0.5 dB and the measured transmission coefficient better than −18 dB in the passband (DC-3.6 GHz). Meanwhile, the prototype has a 20 dB harmonic suppression level in the frequency range from 5.54 GHz up to 43.5 GHz. Furthermore, the measured peak to peak group delay variation was less than 170 ps in the passband. The proposed filter has a very compact size of 195.3 mm2.
... In [12], the back-wave evanescent-mode transmission supported by the complementary split-ring resonator (CSRR) metamaterial with negative permittivity is implemented in SIW for the first time, as well as several compact bandpass filters. Then, various reinforced versions of CSRR, including the open CSRR (OCSRR), the steppedimpedance-resonator-loaded CSRR (SIR-CSRR), the doublesided stepped-impedance complementary split-ring resonator (DS-SICSRR), the fractal open CSRR (FOCSRR), and the modified CSRR (MCSRR), are developed [13][14][15][16][17]. These novel topologies have been successfully investigated to exhibit notable advantages in terms of size miniaturization. ...
... GHz, with the RSR over conventional HMSIW-CSRR being 23.8% and 39.6%. Furthermore, the HMSIW-OCSRR and HMSIW-FOCSRR in [16] and the HMSIW-MCSRR in [17] show fundamental eigenmodes working at 1.435 GHz, 1.165 GHz and 1.176 GHz, and achieved Q c of 82.273, 72.593 and 85.801, respectively, with the frequencies of their three higher-order eigenmodes ranges from 2.369 GHz to 9.434 GHz. They have separately achieved RSR values of 55.0%, 70.3%, and 69.8% as well. ...
... Finally, table 1 summarizes a brief comparison between the proposed evanescent-mode HMSIW-IRCSRR filters and some reported similar works. Firstly, compared with the reported one-pole filters in [13,[15][16][17], the proposed one-pole filter exhibits similar transmission properties and remarkable size reduction. More exactly, the proposed one-pole filter achieves relative size-reduction of 96.3%, 84.5%, 84.5% and 66.7% over those filters of [13,[15][16][17], respectively. ...
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... Several procedures to reduce the occupation areas of the SIW structures have been developed which the most important of these methods are folding [19] and, half-mode [20]. An attractive technique for miniaturization of the SIW platform is the evanescent mode technique [21][22][23]. Based on the theory of the evanescent-mode propagation, an additional passband below the waveguide cut-off frequency can be achieved by engraving electric dipoles on the metal surface of the SIW structure [21][22][23]. ...
... An attractive technique for miniaturization of the SIW platform is the evanescent mode technique [21][22][23]. Based on the theory of the evanescent-mode propagation, an additional passband below the waveguide cut-off frequency can be achieved by engraving electric dipoles on the metal surface of the SIW structure [21][22][23]. ...
... The resonance frequencies of the MCSRR unit-cell and the FCSRR unit-cell, are less than compared to the conventional CSRR with the same sizes [21][22][23]. In fact, by choosing these new configurations, the electrical size of them are decreased without occupying the extra spaces. ...
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... Bandpass filters and power dividers are two most important and essential components in microwave circuits for selecting signals and dividing power, respectively [11][12][13][14]. At lower frequencies, these components suffer from the large size. ...
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... The concept of metamaterials with unusual electromagnetic properties is man-made electromagnetic materials that are not found available in nature. [19][20][21] These artificial materials can be realized by negative permittivity or/and permeability. [19][20][21] Metamaterial structures are good candidates for designing microwave devices with novel applications because of their unusual electromagnetic properties. ...
... [19][20][21] These artificial materials can be realized by negative permittivity or/and permeability. [19][20][21] Metamaterial structures are good candidates for designing microwave devices with novel applications because of their unusual electromagnetic properties. Metamaterials can be realized by resonance or nonresonance structures which the resonant type approach has been more used for the design of microwave components such as BPFs and PDs. ...
... Metamaterials can be realized by resonance or nonresonance structures which the resonant type approach has been more used for the design of microwave components such as BPFs and PDs. [19][20][21] In this article, a novel single-layer DB HMSIW filter and three equal/unequal DB HMSIW FPDs with supercompact sizes have been proposed. The working principle of the proposed components is based on the evanescent mode technique. ...
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... Therefore, this configuration needs a technique to decrease its dimension. Half-mode SIW (HMSIW) [20], folded SIW (FSIW) [21], ridge SIW (RSIW) [22] and the evanescent mode propagation technique [23] are some of methods to reduce the size of the conventional SIW structures. ...
... The stepped-impedance resonator (SIR) technique is introduced into SIW-CSRR filters design in [9]. A modified CSRR (MCSRR) is proposed in [10] by inner extending the split in menderline shape for HMSIW filter implementation. Moreover, the fractal open CSRR (FOCSRR) and G-shaped resonator (CGR) are presented in [11] and [12] to reduce the circuitry physical sizes, respectively. ...
... Firstly, it can be easily obtained that Table 2, the proposed HMSIW-SECSRR filters are with the smallest relative electrical size and smallest insertion loss, as well as reduced fabrication tolerance sensitivity. Although the works in [8,10,11] are with much higher center frequencies that might increase the insertion loss, the proposed filters are still with attractive performance. Actually, according to the datasheet released by Angels Electronics, the SMA connector can contribute to the insertion loss with a value of 0.06 · f 0.5 dB, where f is in GHz. ...
... Actually, according to the datasheet released by Angels Electronics, the SMA connector can contribute to the insertion loss with a value of 0.06 · f 0.5 dB, where f is in GHz. Hence, as the proposed one-pole and two-pole Type-III HMSIW-SECSRR filters are redesigned with a center frequency around 5.5 GHz, its insertion loss would be 0.52 + 0.141 = 0.661 dB and 0.96 + 0.141 = 1.101 dB, respectively, which is still much lower than that in [8,10,11]. Moreover, the proposed HMSIW-SECSRR filters also achieve similar return loss performance to those in [8][9][10], only worse than those in [11,12]. ...
... 8,9 Especially, fractional-mode SIW cavities have demonstrated a conceptual route for component miniaturization. Many miniaturized filters and antennas with good performance have been reported by using half modes, [10][11][12] quarter modes (QMs), 13,14 and even eighth modes. 15,16 So far, however, no works have been reported to integrate these filters and antennas in a single SIW cavity. ...
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... Power dividers and bandpass filters are widely used in microwave systems for power dividing and signal selection. 1,2 At low gigahertz frequency region, these components usually occupy a large area. On the other hand, the cascade of a power divider and bandpass filter will lead to a large circuit size and high insertion loss. ...
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A novel low-loss and miniaturized triple-band band-pass filter (BPF) and triple-band filtering power dividers (FPDs) with arbitrary power division ratio using half-mode substrate integrated waveguide (HMSIW) have been proposed in this paper. The working mechanism of the introduced components is based on the evanescent mode technique which is one the most important techniques to reduce the dimension of the microwave structures. Other methods which are used in this work to miniaturize the total size of the proposed configurations are the half-mode technique, the stepped-impedance resonator (SIR) technique, and the meander technique. Accordingly, a triple-band BPF and three triple-band equal/unequal FPDs with the power division ratios of 1:1, 4:1, and 8:1, have been designed and simulated working at 2.35, 3.7, and 5.65 GHz using the mentioned techniques. Therefore, the total size of the proposed components is very small and is less than 0.01 λ <sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">g</sub> <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> . The designed triple-band BPF and triple-band FPD with equal power division ratio have been fabricated under the printed circuit boards (PCBs) process and measured to demonstrate the efficiency of the proposed designs. The simulation results show good agreement with the measurement results.