IEEE MICROWAVE AND WIRELESS COMPONENTS LETTERS, VOL. 27, NO. 1, JANUARY 2017 31
Compact Balanced Dual-Band Bandpass Filter
Based on Modified Coupled-Embedded Resonators
Fulya Bagci, Member, IEEE, Armando Fernández-Prieto, Member, IEEE, Aintzane Lujambio,
Jesús Martel, Senior Member, IEEE , Joaquín Bernal, Member, IEEE,
and Francisco Medina, Fellow, IEEE
Abstract—A new compact balanced dual-band bandpass filter
based on coupled-embedded resonators with modified ground
plane is presented in this work. Common-mode is rejected within
the two differential passbands by symmetrically introducing
four coupled U-shaped defected ground structures below the
resonators. Common-mode rejection is significantly improved
when compared with the standard (solid ground plane) filter with
similar geometry thanks to the introduction of four extra trans-
mission zeros. Due to the symmetry, the differential mode is not
significantly affected by the presence of the U-shaped resonators.
Circuit-model data, full-wave simulations and measurements are
provided to verify the benefits of the proposed dual-band filter.
Index Terms— Balanced filter, common-mode suppression,
dual-band filter.
I. I NTRODUCTION
R
F/MICROWAVE balanced bandpass filters (BPFs) have
attracted the interest of the microwave community in
recent years due to their enhanced signal to noise ratio, noise
immunity, low crosstalk and low electromagnetic interfer-
ence (EMI) when compared with their classical single-ended
counterparts. Nowadays, with the rapid growth of multi-
band wireless communication systems, multiband BPFs with
very demanding specifications concerning both differential
mode (DM) transmission and common-mode mode (CM) sup-
pression are required. Several proposals regarding dual-band
balanced BPFs can be found in the recent literature [1]–[9].
In [1]–[4], [7] balanced dual-band operation is obtained by
means of electrically-coupled resonators. In such designs,
Manuscript received May 22, 2016; revised July 21, 2016; accepted Octo-
ber 10, 2016. Date of publication December 14, 2016; date of current version
January 6, 2017. This work has been supported in part by the Spanish
Ministerio de Economía y Competitividad with European Union FEDER
Funds (contract TEC2013-41913-P), by the Spanish Junta de Andalucía
(project P12-TIC-1435), and by TUBITAK, The Scientific and Technological
Research Council of Turkey, under grant 22B2219
F. Bagci is with the Department of Electronics and Electromagnetism,
Physics Faculty, University of Sevilla, Av. Reina Mercedes s/n, Seville 41012,
Spain and also with the Department of Engineering Physics, Faculty of
Engineering, Ankara University, Besevler, Ankara 06100, Turkey.
A. Fernández-Prieto and F. Medina are with the Department of Electronics
and Electromagnetism, Physics Faculty, University of Sevilla, Av. Reina
Mercedes s/n, Seville 41012, Spain (e-mail: armandof@us.es).
A. Lujambio is with the Skylife Engineering, Parque Tecnológico Aeroes-
pacial de Andalucía, Early Ovington Street, 24, Nave 15-16, Seville 41309,
Spain.
J. Martel is with the Department of Applied Physics II, ETS Architecture
School, Av.Reina Mercedes s/n, Seville 41012, Spain.
J. Bernal is with the Dept. of Applied Physics III, ETS Ingenieros,
University of Sevilla, Av. de los Descubrimientos, Seville 41092, Spain.
Color versions of one or more of the figures in this paper are available
online at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/LMWC.2016.2629962
CM suppression is improved by adding extra lumped capac-
itors, inductors, resistors and/or open-circuited stubs. Other
recently proposed approaches to DM filter design with CM
suppression make use of asymmetrical coupled lines [5] or
substrate integrated waveguide (SIW) technology [8]. These
designs provide good DM performance and CM rejection,
but they suffer from the problem of having large electrical
size and, moreover, the use of a large number of via-holes.
In [6] balanced dual-band filtering is achieved by using
coupled-embedded resonators. In this implementation the CM
is rejected by cascading with the filter a pair of CM rejection
differential-line stages based on the use of a low-pass DGS
structure. Unfortunately, this solution increases the design
complexity and the overall electrical size. Coupled comple-
mentary split-ring resonators (C-CSRR) have very recently
been proposed [9] for the design of compact balanced dual-
band filters with good CM rejection. In this letter, a new
compact balanced dual-band BPF based on coupled-embedded
resonators with a modified ground plane is proposed. Design
methodology and experimental validation of the structure
are illustrated with a specific filter example operating at
two wireless local area network (WLAN) bands. Measured
and simulated results show the benefit of the proposed
configuration.
II. PROPOSED DGS STRUCTURE
The layout of the proposed balanced dual-band BPF is
shown in Fig.1. The top layer geometry is based on the single-
ended and differential dual-band filters reported in [10] and [6]
respectively. It consists of the combination of two different
sub-filters that enable the generation of two different DM
passbands. These bands can be independently tuned. The
bottom layer is formed by four U-shaped slot resonators.
These resonators have been used in [11], [12] to improve
the CM rejection of differential lines. In this letter the DGS
resonators are embedded within the printed filter area, thus
yielding a more compact design. When operating in DM, the
AA
′
symmetry plane (see Fig.1) is a virtual short-circuit. The
DGS is then grounded at both ends and hence it hardly affects
the response of this mode. On the contrary, for CM operation
the AA
′
plane behaves as a virtual open-circuit. It is then
expected a strong disturbance of the CM response.
Let us first focus our attention on the role of the
U-shaped DGSs when used below a differential line
pair [see Fig.2(a)]. Each resonator can be modeled
(CM excitation) as a parallel LC -tank circuit with a couple of
electrically short lines connected at both sides [11] (see Fig.2).
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