Design of Compact Ultra-Wideband Filter with Low Insertion Loss and Wide Stopband
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(2) IEICE TRANS. ELECTRON., VOL.E93–C, NO.9 SEPTEMBER 2010. 1482. coupling between TL1 and TL2 will produce a transmission zero [12]. In our implementation, quasi-lumped elements are adopted to approximate the quasi-lumped prototype. As depicted in Fig. 1(b), the inductors L2 , L3 and L4 are implemented by high-impedance microstrip line sections, and the shunt transmission lines TL1 and TL2 are implemented by microstrip shorted stubs connected to ground. The capacitors C1 and C3 are implemented by low-impedance microstrip line sections and the series capacitor C2 is realized by the microstrip-to-CPW transition. Besides, Cc originates from the microstrip-to-CPW transition, thus its layout including the slot in the bottom layer and the gap in the top layer should be simulated carefully. Furthermore, the capacitive coupling between C1 and C3 will affect Cc , thus the distance between those capacitors should be desinged suitably to optimize the selectivity of the filter. The filter skillfully utilizes the capacitive and magnetic coupling between the elements implemented in the three- dimension layout, thus we can obtain good selectivity with a small number of passive/lossy elements. Furthermore, because a small number of passive/lossy elements are used, low insertion loss over the wide passband and compact size won’t be compromised. 3.. Experimental Results. To verify the feasibility of the quasi-lumped prototype and to account for the discontinuities between the elements which are not considered in the prototype, the filter is simulated over its entire layout using Ansoft HFSS v10 and is then fabricated using Rogers RO4003C (with εr = 3.38, tan δ = 0.0027, and thickness h = 0.508 mm). Figure 2(a) shows the top-/bottom-layer layout, and the photograph of the proposed filter is shown in Fig. 2(b). The overall dimension of the device is 4.6 mm × 7.4 mm, which is approximately 0.23λ × 0.31λ, where λ is the guided wavelength of the microstrip structure at the center frequency f0 = 7.1 GHz. The dimensions confirm the very compact size of the developed device. Figure 3 shows the measured S parameters of the proposed wideband filter. The filter has a measured 3 dB fractional bandwidth of 128% from 2.8 GHz to 11.4 GHz. The return loss is greater than 13 dB within the pass-band, and the minimum insertion loss is 0.3 dB at 5 GHz. It also exhibits good selectivity and stopband rejection, which is better than 20 dB from 12.4 GHz to about 24 GHz. The discrepancies between the simulated and measured results are due to the fabrication errors. Moreover, from the measured S -parameters, we determine that the implemented filter exhibits a flat group-delay ranging from 0.32 ns to 0.44 ns over the whole passband, as shown in Fig. 4. Comparison with other filters is summarized in Table 1. In terms of size, stopband rejection, stopband bandwidth and insertion loss, our wideband filter has similar or better performance.. Fig. 2 (a) The top-/bottom-layer circuit layout of the proposed filter. (b) The photograph of the filter.. Fig. 3 Simulated (dashed curves) and measured (solid curves) insertion loss, and return loss of the fabricated filter.. Fig. 4. Measured group delay of the fabricated filter..
(3) LETTER. 1483 Table 1. 4.. Performance comparison of filters presented in prior works and the proposed filter.. Conclusions. In this paper, a 2.8–11.4 GHz filter was designed and fabricated using Rogers RO4003C (with εr = 3.38, tan δ = 0.0027, and thickness h = 0.508 mm). Compared with other filters in a similar frequency range, our circuit simultaneously achieves low insertion loss, wide-stopband, good selectivity, and compact size. Acknowledgement Authors would like to thank National Science Council of Taiwan for the financial support, and the anonymous reviewers for suggestions and encouragement. References [1] W. Menzel, L. Zhu, K. Wu, and F. B¨ogelsack, “On the design of novel compact broadband planar filters,” IEEE Trans. Microw. Theory Tech., vol.51, no.2, pp.364–369, Feb. 2003. [2] J.-T. Kuo and E. Shih, “Wideband bandpass filter design with threeline microstrip structures,” IEEE MTT-S Int. Dig., pp.1593–1596, 2001. [3] L. Zhu, S. Sun, and W. Menzel, “Ultra-wideband (UWB) bandpass filters using multiple-mode resonator,” IEEE Microw. Wireless Compon. Lett., vol.15, no.11, pp.796–798, Nov. 2005.. [4] H. Wang, L. Zhu, and W. Menzel, “Ultra-wideband bandpass filter with hybrid microstrip/CPW structure,” IEEE Microw. Wireless Compon. Lett., vol.15, no.12, pp.844–846, March 2005. [5] J. Gao, L. Zhu, W. Menzel, and F. B¨ogelsack, “Short-circuited CPW multiple-mode resonator for ultra-wideband (UWB) bandpass filter,” IEEE Microw. Wireless Compon. Lett., vol.16, no.3, pp.104–106, March 2006. [6] T.-N. Kuo, S.-C. Lin, and C.H. Chen, “Compact ultra-wideband bandpass filters using composite microstrip-coplanar-waveguide structure,” IEEE Trans. Microw. Theory Tech., vol.52, no.10, pp.3772–3778, Oct. 2006. [7] C.-W. Tang and M.-G. Chen, “A microstrip ultra-wideband bandpass filter with cascaded broadband bandpass and bandstop filters,” IEEE Trans. Microw. Theory Tech., vol.55, no.11, pp.2412–2418, Nov. 2007. [8] J. Garcia-Garcia, J. Bonache, and F. Martin, “Application of electromagnetic bandgaps to the design of ultra-wide bandpass filters with good out-of-band performance,” IEEE Trans. Microw. Theory Tech., vol.54, no.12, pp.4136–4140, Dec. 2006. [9] Z.-C. Hao and J.-S. Hong, “Ultra-wideband bandpass filter using multilayer liquid-crystal-polymer technology,” IEEE Trans. Microw. Theory Tech., vol.56, no.9, pp.2095–2100, Sept. 2008. [10] S.W. Wong and L. Zu, “Quadruple-mode UWB bandpass filter with improved out-of-band rejection,” IEEE Microw. Wireless Compon. Lett., vol.19, no.3, pp.152–154, March 2009. [11] D. Pozar, Microwave Engineering, Wiley, New York, 2005. [12] T. Ishizaki, M. Fujita, H. Kagata, T. Uwano, and H. Miyake, “A very small dielectric planar filter for portable telephones,” IEEE Trans. Microw. Theory Tech., vol.42, no.11, pp.2017–2022, Nov. 1994..
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