PIERS Proceedings, Moscow, Russia, August 19–23, 2012 906 Design of High Isolation Electronically Switchable Bandpass Filter Shih-Fong Chao and Ming-Wei Shih National Kaohsiung Marine University, Taiwan Abstract—In this paper, a simple method to design a high isolation electronically switchable bandpass filter is proposed. The circuit integrates a microwave switch and a microwave bandpass filter into a single circuit component. The uniform impedance resonator is loaded with a pin diode to change its resonant frequencies under different bias voltages. By loading the pin diode at different positions of the constituted resonators, the resonant frequencies can be misaligned over the band of interest to achieve a wideband isolation in the isolated state. In the thru state, the circuit shows a bandpass response with a measured insertion loss of 3 dB at the center frequency of 1 GHz, and the 3 dB fractional bandwidth is 8%. In the isolated state, the measured isolation is 51 dB at the center frequency and is higher than 30 dB from dc to 5 GHz. The paper proposed a simple and effective method to realized an electronically switchable bandpass filter with high isolation, and the circuit successfully increases the level of integration of the RF front end. 1. INTRODUCTION A microwave switch is a essential component to control RF signal flow in the modern communication systems. Several literatures using passive FETs or pin diodes have been reported [1, 2]. However, these switches are wideband designs, implying that they can not provide adequate band selectivity for a system application. Therefore, a bandpass filter will be needed to cascade with a switch to reject out-of-band signals. Recently, several methods were proposed to integrated the building blocks of the RF front into a multi-function circuit [3–6]. In [3], an SPDT bandpass filter-integrated switch that integrate an SPDT switch and a bandpass filter was proposed. Switchable dual-band bandpass filters that achieve independent switching control of band selection was proposed in [4, 5]. In [6], a balunintegrated bandpass switchplexer that integrates an SPDT switch, a diplexer, and a balun was demonstrated. In this paper, a new method to design a high-isolation switchable bandpass filter is proposed. The pin diode loaded uniform resonator is used to realized the circuit instead of using steppedimpedance resonators. By connecting the pin diode at different locations of the uniform resonator, the resonant frequencies of the resonator can be controlled. Therefore, a high isolation can be obtained by interlacing the resonant frequencies over the band of interest in the isolated state. 2. CIRCUIT DESIGN Figure 1 shows the structure of the diode-loaded uniform resonator and its equivalent circuit under different bias conditions. The θ1 is the electrical length from the loading location to the open end, and θ2 is the electrical length from the loading location to the other open end. When the diode is reversed biased (off-state), the resonator is loaded with a small capacitor. If the diode is forward biased (on-state), the resonator will be connected to ground via a small resistor R. Since the R is small, the diode could be considered as a short circuit to ground. Thus, the resonant frequencies are determined by two quarter-wavelength resonator with one end short to ground. Figure 2 shows the circuit schematic of the proposed switchable bandpass filter. The circuit is composed by three diode-loaded hairpin resonators. In the thru state, the diodes are reversed biased, the first resonant frequency of each resonator is 1 GHz. The circuit was designed to have diode off θ1 θ1 θ2 θ1 θ2 θ2 diode on Figure 1: Photograph of the DPDT filter-integrated switch A. Progress In Electromagnetics Research Symposium Proceedings, Moscow, Russia, August 19–23, 2012 907 R =1 k Ω R= 1 k Ω R = 1 kΩ Port 1 Port 2 Figure 2: Circuit schematic of the proposed switchable bandpass filter. Figure 3: Photograph of the switchable bandpass filter. 0 0 EM simulation Measurement |S11| -30 |S21| -40 -50 -20 -30 |S21| -40 -50 -60 -70 EM simulation Measurement |S11 | -10 -20 |S21| & |S11| (dB) |S21| & |S11| (dB) -10 0 0.5 1 Frequency (GHz) 1.5 2 -60 0 1 2 3 (a) 4 5 Frequency (GHz) 6 7 8 8.5 (b) Figure 4: Simulation and measured results of the switchable bandpass filter in thru state. (a) Narrow band response. (b) Wideband response. a 3rd-order Butterworth bandpass response at 1 GHz, and 3-dB fractional bandwidth ∆3 dB of 8%. The coupling coefficients and the external quality factor Qext can be obtained as M12 = Qei = ∆3 dB = M23 = 0.059 √ g1 g2 g0 g1 = Qeo = 10.9 ∆3 dB (1) where Mij represents the coupling coefficient between resonators i and j, gn is the low-pass prototype parameter, and Qei and Qeo are the external quality factors associated with the input and output couplings, respectively [7]. In the isolated state, the diodes are forward biased. By loading the diodes at different locations of the resonators, the resonant frequencies can be scattered over the band of interest. Thus, a high isolation could be obtained between the input and the output ports. 3. MEASUREMENT The circuit is fabricated on the RO4003C substrate with ²r = 3.58, h = 0.8 mm, and tan δ = 0.0015. Fig. 3 is the photograph of the switchable bandpass filter. Fig. 4 shows the measured results when PIERS Proceedings, Moscow, Russia, August 19–23, 2012 908 0 |S11| EM simulation Measurement -20 -30 -40 -50 EM simulation Measurement -20 -30 |S21| -40 -50 |S21| -60 -70 |S11| -10 |S21| & |S11| (dB) |S21| & |S11| (dB) -10 0 0.5 -60 1 Frequency (GHz) (a) 1.5 2 -70 0 1 2 3 4 5 6 Frequency (GHz) 7 8 8.5 (b) Figure 5: Simulation and measured results of the switchable bandpass filter in isolated state. (a) Narrow band response. (b) Wideband response. the circuit is at thru state. It can be observed that a bandpass response with a passband insertion loss of 3.0 dB at center frequency of 1 GHz was measured, and the 3-dB bandwidth is 8.5%. The measured isolations of the circuit is shown if Fig. 5. The isolation is about 60 dB at the center frequency of 1 GHz and is better than 32 dB from dc to 5 GHz. 4. CONCLUSION In this paper, a high isolation electronically switchable bandpass filter is designed and implemented. By loading the pin diode at different positions of the constituted resonators, the resonant frequencies can be misaligned to obtain an isolation in the isolated state. In the thru state, the circuit shows a bandpass response with a measured insertion loss of 3 dB at the center frequency of 1 GHz. In the isolated state, the measured isolation is 51 dB at the center frequency. The circuit successfully integrates a microwave switch and a bandpass filter into a single circuit and thus increases the level of integration of the RF front end. ACKNOWLEDGMENT The authors would like to thank Prof. Jui-Han Lu for the support of measurement equipments. REFERENCES 1. Chao, S.-F., H. Wang, C.-Y. Su, and J. G. J. Chern, “A 50 to 94-GHz CMOS SPDT switch using traveling-wave concept,” IEEE Microw. Wireless Compon. Lett., Vol. 17, No. 2, 130–132, 2007. 2. Lai, R.-B., J.-J. Kuo, and H. Wang, “A 60–110 GHz transmission-line integrated spdt switch in 90 nm cmos technology,” IEEE Microw. Wireless Compon. 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