Research Article | Open Access

Wei-Qiang Pan, Xiao-Lan Zhao, Yao Zhang, Jin-Xu Xu, "High Selectivity Dual-Band Bandpass Filter with Tunable Lower Passband", *International Journal of Antennas and Propagation*, vol. 2015, Article ID 762504, 6 pages, 2015. https://doi.org/10.1155/2015/762504

# High Selectivity Dual-Band Bandpass Filter with Tunable Lower Passband

**Academic Editor:**Dimitrios Sounas

#### Abstract

This paper presents a novel method to design dual-band bandpass filters with tunable lower passband and fixed upper passband. It utilizes a trimode resonator with three controllable resonant modes. Discriminating coupling is used to suppress the unwanted mode to avoid the interference. Varactors are utilized to realize tunable responses. The bandwidth of the two bands can be controlled individually. Transmission zeros are generated near the passband edges, resulting in high selectivity. For demonstration, a tunable bandpass filter is implemented. Good agreement between the prediction and measurement validates the proposed method.

#### 1. Introduction

The bandpass filters which are used to reject the unwanted signals have been widely investigated [1]. Meanwhile, to meet the requirement of the multiband operations, various methods have been proposed to design multiband bandpass filters [2–5]. Recently, electronically tunable bandpass filters have drawn much attention due to their capacity to deal with various operating frequencies in a system. Varactors are loaded at the ends of the resonators to adjust the operating frequencies [6]. Besides the frequency, the bandwidth of a tunable filter also should be taken into consideration [7–9]. In [7], suitable coupling region is selected to keep the bandwidth constant. Besides tunable single-band bandpass filters, tunable dual-band bandpass filters also have been widely researched [10–16]. In [11, 12], varactors are equipped at the center of stub-loaded open-ended resonator, resulting in a fixed lower passband and a tunable upper passband. To realize frequency tuning at both passbands, varactors are loaded not only at the center stub but also at the end of main transmission line [13]. For further convenient adjustment, two sets of resonators are employed [14–16]. By controlling different voltages, both of the two bands can be tuned.

However, most of the above references focus on designing dual-band filters with tunable upper passband, and few literatures address bandpass filters with a tunable lower passband and a fixed upper passband. The potential problem associated with this type of tunable filters is that the harmonic of the lower passband may overlap with the fixed upper passband.

To avoid this problem, we propose a novel method of using trimode resonators to design the tunable dual-band bandpass filter. The second mode (middle frequency) and third mode (highest frequency) of the trimode resonator are utilized to form the lower and upper passbands, respectively. The first mode (lowest frequency) is suppressed by discriminating coupling to eliminate the interference with the passband so that the selectivity can be enhanced. The second mode can be tuned by the varactors without affecting third mode, resulting in a tunable lower passband and fixed upper passband. Meanwhile, transmission zeros are synchronously changed with the passband, ensuring high skirt selectivity.

#### 2. Design Theory

Figure 1(a) shows the proposed stub-loaded trimode resonator. It consists of a main transmission line and three open stubs. The characteristic admittance and the electronic length of each stub are shown. It is symmetric in structure; thus, even- and odd-mode method can be used to characterize it and its odd- and even-mode equivalent circuits are shown as in Figures 1(b) and 1(c). Since Figures 1(b) and 1(c) are still symmetric, even- and odd-mode method can be further used to analyze them. The corresponding equivalent circuits are shown as Figures 1(d)–1(g). Under the special condition of , the resonant frequencies of Figures 1(d), 1(e), 1(f), and 1(g) can be deduced as follows [2]:where is the light speed in free space and denotes the effective dielectric constant of the substrate. Comparing the four frequencies, and are the same, and we use to denote them. Meanwhile, we can obtain , while the relationship of and could not be determined since it is related to . Small results in while large results in . Moreover, it can be observed that only affects without affecting and . affects both and without affecting . Thus, the trimode can be controlled individually. To demonstrate this, some simulations are carried out by using ADS. In the simulations, the parameters are chosen as follows: mm, mm, mm, S, and . When one parameter is swept, the other parameters are fixed. The simulated results are shown in Figure 2. It can be observed that when is changed, and are also changed while is fixed. When is changed, only is changed and the other two modes are fixed. Thus, we can design a dual-band filter with tunable lower passband which is formed by (the second mode) and fixed upper passband formed by (the highest mode) and suppressed (the lowest mode).

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Figure 3 shows the structure of the proposed dual-band filter with tunable lower passband. It utilizes a second order stub-loaded trimode resonator and the stubs are folded to reduce the size. The varactors are loaded at the center stubs. The capacitor (2 pF) is used to block the DC signals. The with the high resistance of 47 kΩ can prevent the RF signals and is used as DC feed. The feed lines are coupled with the resonators. There is an important issue that should be noticed: the feed line should be mirror symmetrical with respect to the port and the center of the resonator. With such a structure, the mode of can be suppressed and the tunable lower passband and fixed upper passband can be realized.

The mechanism of suppression is addressed as follows. For a parallel coupled microstrip line with a length of , the electric coupling can be approximated as [17]where and are voltage-wave functions on the two lines and represents a constant. When the voltage-wave function is odd on one line and even on the other, the integrand in the numerator is an odd function and it yields a zero value upon integration, which implies that the electric coupling coefficient is zero. Similarly, the magnetic coupling coefficient is also zero. Thus, no energy can pass at this frequency, resulting in mode suppression.

According to the analysis, is determined by and . In Figure 3, if the mode is not suppressed, it corresponds to a passband which is affected by . It is a half-wavelength resonator and the voltage distribution at the two open ends (AB and CD) with regard to the feed point is odd symmetrical. However, the voltage distribution at the two sides of feed line with regard to the feed point is even symmetrical. Thus, according to (2), the mode of is suppressed without affecting and . In the suppression mechanism, the key point is the mirror symmetry of the resonator and the feed line with regard to the feed point. To demonstrate this, simulations are carried out under the condition of the port at and not at the center of the feed line. To observe the modes, the varactors are replaced by capacitors. Figure 4 shows the simulated results. It can be observed that when the port is not located at the center of the feed line there will be three passbands, corresponding to the mode: , and . If the port is located at the center of the feed line, the first passband will be suppressed and the other two bands are kept unchanged. Moreover, the selectivity of the lower passband is improved. Using such a feed method, the can be suppressed without any extra circuit.

To design a tunable dual-band bandpass filter, we can first design a dual-band filter with fixed centre frequencies of and . The frequencies and bandwidths can be individually controlled as follows. For the operating frequencies, it can be controlled individually. We can first obtain by tuning the length of , which is nearly quarter-wavelength at . Then, and are used to control without affecting . For the bandwidth, it is determined by the external quality factor () and coupling coefficient (). For the , it is determined by the coupling lengths and gaps, for example, , , , and . Small gaps ( and ) and large lengths ( and ) result in small and large bandwidths at both passbands. For , it is determined by the coupling strength between the two resonators, for example, and . Since has little effect on , can be used to control at with little effect on . To determine the initial value of these parameters, we can use simulation software to extract . The second passband is fixed with 3 dB bandwidth of 6% and 0.5 dB ripple. Thus, the required is 0.06. Figure 5 shows the extracted against and . Using this figure, the and can be determined as 0.2 and 3 mm. Similarly, the initial value of can be determined as 0.3 mm. Figure 6 shows the simulated results against and . It can be observed that when increases, the bandwidth of upper passband decreases and the bandwidth of the lower passband decreases. When is changed, only the bandwidth of lower passband changes and the upper passband is fixed. These results indicate that the bandwidth of the two bands can be controlled individually. After the nontunable filter is well-designed, varactors are loaded at the end of to realize tunable responses. Then, fine tuning is used to obtain the optimal performance.

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#### 3. Experiment

To demonstrate the proposed idea, a circuit is implemented on the substrate with a relative dielectric constant of 3.38, loss tangent of 0.0027, and thickness of 0.81 mm. The varactors employed in this design are 1sv277 from Toshiba. The capacitors are from Murata and we use the Murata model in simulation. The final values are selected as follows (all in mm): , , , , , , , , , , , , , , , , and . And kΩ; pF. The overall size of the filter is 14.9 mm × 24 mm or , where represents the guided wavelength at 2.04 GHz, which is the lowest frequency of the tunable passband. The photograph of the fabricated filter is shown in Figure 7.

The simulation and measurement are accomplished by IE3D, ADS, and 8753ES network analyzer, respectively. Figure 8 shows the simulated and measured results. The upper passband is fixed at 3.5 GHz with 3 dB bandwidth of 200 MHz or 5.7%, which covers the WiMAX system. The measured minimum insertion loss is 1.5 dB and the return loss is better than 30 dB. Two transmission zeros with the frequencies of 3.15 and 4.25 GHz are generated at both sides of the passband. For the lower passband, with the voltage increasing from 0 to 6 V, the operating frequency changes from 2.04 to 2.62 GHz with 3 dB bandwidth changing from 90 to 135 MHz. The return losses are better than 15 dB in each state. The insertion losses change from 3.7 dB to 1.7 dB, which is a little higher than the nontunable bandpass filter. It is mainly due to the loss of the varactors. Meanwhile, the two transmission zeros located at the two sides of the lower passbands synchronously change with the passband, ensuring high selectivity. Among the four transmission zeros, the first one is generated by the source-load coupling; the second and last ones are generated by the stub with length of and . The third one is introduced by the feed line and + is quarter-wavelength at the frequency of the third transmission zero.

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#### 4. Conclusion

This paper has presented a novel method for designing dual-band bandpass filters with a tunable lower passband and fixed upper passband. Both theory and experiments have been provided, showing that the filter exhibits good performance. Transmission zeros are generated near the passbands, resulting in high selectivity.

#### Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

#### Acknowledgments

This work is supported by the NSFC under Grant 61271209 and the Fundamental Research Funds for the Central Universities under Grant 2013ZM0106.

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#### Copyright

Copyright © 2015 Wei-Qiang Pan et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.