13. J. Anguera, I. Sanz, J. Mumbru, and C. Puente, Multi-band handset
antenna with a parallel excitation of PIFA and slot radiators, IEEE
Trans Antenna Propag 58 (2010), 348–356.
14. X. Jing, Z. Du, and K. Gong, A compact multiband planar antenna
for mobile handsets, IEEE Antenna Wireless Propag Lett 5 (2006),
343–345.
15. C.Y.D. Sim, Mutiband planar antenna design for mobile handset,
Microwave Opt Technol Lett 50 (2008), 1543–1545.
16. C. Mahatthanajatuphat, S. Saleekaw, and P. Akkaraekthalin, A
Rhombic patch monopole antenna with modified Minkowski fractal
geometry for UMTS, WLAN, and mobile WiMAX application,
Prog Electromagn Res 89 (2009), 57–74.
17. B.C. Jang and C.Y. Kim, Internal antenna design for a triple band
using an overlap of return loss, J Electromagn Wave Appl 21
(2007), 1099–1108.
18. D. Pozar, Microwave engineering, 3rd ed., Wiley, New York,
2005.
19. P.-S. Kildal and K. Rosengren, Correlation and capacity of MIMO
systems and mutual coupling, radiation efficiency and diversity
gain of their antennas: Simulations and measurements in reverbera-
tion chamber, IEEE Commun Mag 42 (2004), 102–112.
20. K. Rosengren and P.S. Kildal, Radiation efficiency, correlation, di-
versity gain and capacity of a six-monopole antenna array for a
MIMO system: Theory, simulation and measurement in reverbera-
tion chamber, IEE Proc Microwave Antennas Propag 152 (2005),
7–16.
21. J. Carlsson, U. Carlberg, A. Hussain, and P. Kildal, About meas-
urements in reverberation chamber and isotropic reference environ-
ment, In: 2010 20th International Conference on Applied
Electromagnetics and Communications (ICECom), 20–23 Septem-
ber 2010, Piscataway, NJ, 2010, p. 4.
22. C. Xiaoming, P.S. Kildal, and J. Carlsson, Measurement uncertain-
ties of capacities of multi-antenna system in anechoic chamber and
reverberation chamber, In: Wireless Communication Systems
(ISWCS), 2011 8th International Symposium, 2011, pp. 216–220.
23. C.-L. Liu, Y.-F. Lin, C.-M. Liang, S.-C. Pan, and H.-M. Chen,
Miniature internal penta-band monopole antenna for mobile phone,
IEEE Trans Antenna Propag 58, (2010).
24. O. Owais, M. Karlsson, S. Gong, Z. Ying, M. Grud�en, and M. Job,
Wideband planar antenna with modified ground plane, Microwave
Opt Technol Lett 52 (2010).
25. H. Carrasco, H.D. Hristov, R. Feick, and D. Cofr�e, Mutual cou-
pling between planar inverted-F antennas, Microwave Opt Technol
Lett 42 (2004), 224–227.
VC 2012 Wiley Periodicals, Inc.
NOVEL LOW-PROFILE FOAMDIELECTRIC OVER-THE-SHOULDERANTENNA BASED ON COUPLEDPATCHES TECHNIQUE
Milan Svanda, Milan Polivka, and Premysl HudecDepartment of Electromagnetic Field, Faculty of ElectricalEngineering, Czech Technical University in Prague, Technicka 2,16627 Prague 6, Czech Republic; Corresponding author:[email protected]
Received 27 June 2012
ABSTRACT: The article presents a novel wearable antenna composedof two coupled patches excited by an overlapping folded dipole. In spiteof being operated in a relatively low frequency band 380 � 390 MHz,the antenna shows a very low profile and other dimensions areacceptable as well. Besides a very low absorption of the radiated RFpower by any nearby human body, it also ensures a very good immunityagainst influence on antenna parameters. In comparison to commonlyused simple conformal monopole antennas, the presented solutionprovides a double-side radiation pattern and a substantially higher gain.
The antenna can be manufactured using very light and twistable foamdielectric and conductive fabric, and can be worn as a strap placedover the shoulder. It is intended to be used together with personal radiocommunication transceivers operated in the given frequency band. VC
2012 Wiley Periodicals, Inc. Microwave Opt Technol Lett 55:593–597,
2013; View this article online at wileyonlinelibrary.com. DOI 10.1002/
mop.27389
Key words: body centric communication; coupled patches; low-profileantenna; wearable antenna
1. INTRODUCTION
The research in the field of wearable antennas to be operated in
a close vicinity of a human body represents a topical issue.
Antennas of this kind should fulfil the following requirements.
First, it is required to provide as the highest possible immunity
from undesirable influences of a nearby human body on antenna
parameters. Accordingly, it should ensure as low irradiation of
the communicating person by the RF power as possible. Eventu-
ally, it is required to have small dimensions and show a low
weight and good flexibility.
To date, possible applications range from special RFID sys-
tems to body-centric communications intended especially for
paramedics, firefighters, military personnel, and so forth [1–3].
Although at higher RF and microwave frequencies, a number of
very good solutions fulfilling all the above-stated requirements
have been presented, so far, the design of flexible conformal
radiators for communications in the UHF band has not been
tackled in a satisfactory manner.
In case of common antennas (e.g., monopole or dipole
types), the presence of a nearby human body causes significant
frequency detuning and absorption of the radiated or received
RF energy, which results in low radiation efficiency and gain
[4–7]. Both problems can be, in principle, solved by inserting a
screening metallic plate. The latter can act as an additional
shielding or an inherent part of the antenna; [4]. The coupled
patches structure presented by the authors in Ref. 8 represents
the mentioned shielding principle.
This technique can be applied for minimizing the majority of
disadvantages of simple (2n þ 1) k/4 long monopole antennas
Figure 1 Underarm holder with radio transceiver and simple monop-
ole antenna hidden in shoulder strap
DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 55, No. 3, March 2013 593
that are frequently used in connection with personal radio trans-
ceivers. An example of such antenna and 380 � 390 MHz per-
sonal transceiver can be seen in Figure 1. The radio transceiver
is placed in the underarm holder, which is fixed to a shoulder
strap. An approximately 3=4k-long wire installed in the strap is
used as an antenna (see the first connector from the left).
The operation of this type of monopole antennas in a very
close vicinity to the human body gives rise to several major
problems. Usually, a nonnegligible absorption of the RF power
by the human body, together with the detuning of antenna input
impedance and significant decrease in its radiation efficiency
result in a substantial drop in the antenna gain; see Table 1.
Moreover, the resulting radiation pattern is hard to predict and
often attains minima in the forward and backward directions,
where the maxima of communication traffic can be expected.
The presented coupled patches structure solves the majority
of the aforementioned problems. This technique enables to
design and manufacture low-profile wearable antennas with sat-
isfactory radiation efficiency and a very low level of frequency
detuning even if it is located directly on the human body.
Besides, the antenna shows two identical radiation maxima tar-
geted at the mostly required forward and backward directions.
2. COUPLED PATCHES TECHNIQUE
As mentioned above, the employment of coupled patches struc-
ture enables to design extremely low profile antennas with a
very good immunity from the influence of a human body situ-
ated in the close vicinity. The structure was derived from the
standard patch antenna. Despite many virtues, the latter suffers
from a significant fall in its radiation efficiency (under 50%) if
the relative thickness of the used substrate drops below �0.01
k0 (i.e., 8 mm at 385 MHz); see Ref. 4. This phenomenon can
be eliminated provided that two half-wavelength long patches
that are strongly coupled by a narrow gap are used; see
Figure 2.
Radiation properties of this coupled structure are significantly
enhanced even in case of low-profile substrates with thicknesses
below 0.01 k0 and are, to a large extent, insensitive to the width
of coupling gap. The electric field distribution of the coupled
structure is demonstrated in Figure 3. Due to the strong coupling
of the two half-wavelength patches, three radiating slots are
present, (out of which two are located on the outer sides,
whereas the third one is situated within the coupling gap).
The structure is excited by the folded dipole, etched on a
very thin (0.25 mm) separate upper substrate. For these pur-
poses, even other radiator shapes might be considered, such as
meander dipole, loop antenna, and so forth; see Refs. 8–10.
Change of length of the folded dipole enables to tune the
antenna input impedance to the required level (50 X).
The following paragraph shows that antenna based on the
coupled patches structure with a profile thinner than 0.003 k0
enables to reach �50% radiation efficiency, which is about four
times better than the radiation efficiency of the common patch
antenna made of comparable substrate and showing similar
dimensions.
3. DESIGN, REALIZATION, AND MEASUREMENT
To verify parameters of the coupled patches antenna for the
over-the-shoulder application in the operational 380 � 390 MHz
frequency band, the test sample was designed and manufactured.
The antenna takes the form of a strap to be placed over the
shoulder. To ensure its low weight and high flexibility, the foam
TABLE 1 Comparison of Maximum Gain and 26 dBBandwidth for Simple Monopole Antenna and ProposedCoupled Patches Antenna in the Over-the-ShoulderApplication at f 5 385 MHz
Gain (dBi) BW�6 dB (%)
Stimulated Measured Stimulated Measured
Monopole in free space 1.2 – 16 –
Monopole folded over
human shoulder
�11.3 – 0.3 –
Coupled patches antenna
in free space
�1.3 �1 2.9 3.1
Coupled patches folded
over human shoulder
�2.5 �2.2 3.4 2.9Figure 2 Coupled half-wavelength patches excited by folded dipole
Figure 3 Electric field distribution of coupled half-wavelength patches antenna. Grey arrows indicate orientation of fictive magnetic currents in radiat-
ing slots
594 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 55, No. 3, March 2013 DOI 10.1002/mop
dielectric was used as a substrate; see Figure 4. Although the
metallic layers of the test sample were manufactured using a
copper adhesive tape, the practical implementation is intended
to be based on more flexible and resistant conductive fabric.
The total size of the unfolded antenna amounts to 790 � 50
� 5.6 mm3 (1.014 � 0.064 � 0.0072 k0), while the expected di-
ameter of the fold is equal to 150 mm. The thicknesses of the
lower and upper substrates reach 4.8 and 0.8 mm, respectively.
The dielectric constant of the foam dielectric accounts for er ¼1.3, while its loss tangent reaches tan d ¼ 0.02. The width of
coupling slot equals g ¼ 2.5 mm and the folded dipole footprint
is 570 � 6 mm (0.73 � 0.0077 k0). The antenna feeding is
ensured by a thin RG-174 flexible micro-coaxial cable termi-
nated with a SMA connector.
Figure 5 involves the photograph of manufactured sample in
the intended position over the human shoulder. Figure 6 com-
pares the simulated and measured input reflection coefficients,
both in free space and in the close vicinity of a human body. A
very good agreement between the simulation and measurement
as well as a high immunity from the impact of a nearby human
body can be observed.
Figure 7 present the simulated antenna radiation patterns,
both in free-space and in the close vicinity of a human body,
which were modelled as a definite volume that is merely slightly
exceeding the dimensions of folded antenna. They are filled
with a material having in principle the same parameters as
human body. The maxima of radiation in the forward and back-
ward directions are very well-defined and are nearly identical in
both cases. Figure 8 shows the simulated and measured radiation
patterns in the horizontal (xz) plane. Because it was impossible
for the person wearing the antenna to stand at the antenna turn-
table, the measurements of radiation pattern were performed
only from several discrete angles. Taking into account a small
tilt caused by the asymmetrical position of antenna with respect
to the body, the agreement between the measurement and simu-
lation is also fairly good. The antenna feeding cable was
Figure 4 Drawing of designed coupled patches antenna (a) and detail
of excitation folded dipole (b)
Figure 5 Photograph of manufactured coupled patches antenna placed
over shoulder during tests
Figure 6 Measurement and simulation of reflection coefficient of
coupled patches antenna in a free space and in the close vicinity to the
human body
DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 55, No. 3, March 2013 595
connected directly to ends of the folded dipole. Because the
antenna is operated in a very complex environment, the imple-
mentation of symmetrization was neither used nor advisable.
Table 1 provides comparison of simulated and measured pa-
rameters of both, the coupled patches antenna and simple
monopole antenna described in Section 1. The obtained results
show a very good agreement of simulations and measurement.
Furthermore, in comparison to simple monopole types, the novel
antenna shows obvious advantages.
4. CONCLUSION
The novel wearable antenna based on coupled patches technique
for the over-the-shoulder application in the 380 � 390 MHz fre-
quency band was developed and its parameters were subject to
verification. Despite having a very low profile (0.0072 k0), it
shows the satisfactory radiation efficiency and very good immu-
nity from the presence of nearby human body. The resulting
gain reaches �1 dBi in free space and �2.2 dBi in the over-the-
shoulder application, which can exceed by up to 8.8 dB the gain
of the simple monopole antenna operated under similar condi-
tions. The antenna radiation patterns have two nearly identical
maxima oriented to the forward and backward directions, where
the communication traffic maxima can be expected. The antenna
is very light, twistable, and can be worn as a separate fixable
over-the-shoulder strap. Alternatively, it can be incorporated
into the article of clothing. It is intended to be used together
with personal communication transceivers operated, for example,
by paramedics, firefighters, or military personnel.
ACKNOWLEDGMENTS
The present research was undertaken at the Department of Electro-
magnetic Field at the Czech Technical University in Prague. It was
jointly supported by the Czech Science Foundation—(project No.
P102/12/P863 ‘‘Electromagnetic Properties of Radiating Structures
and Artificial Screening Surfaces in the Close Vicinity of the Human
Body’’) and the COST project (No. LD 12055 AMTAS: ‘‘Advanced
Modelling and Technologies for Antennas and Sensors’’) that repre-
sents a subpart of the COST project No. IC 1102 VISTA: ‘‘Versatile,
Integrated, and Signal-aware Technologies for Antennas.’’
REFERENCES
1. P.S. Hall and H. Yang, Antennas and propagation for body-centric
wireless communications, Artech House, Norwood, MA, 2006.
2. D.C. Ranasinghe, D.M. Hall, P.H. Cole, and D.W. Engels, An em-
bedded UHF RFID label antenna for TAGing metallic objects, In:
Proceeding of intelligent sensors, sensor networks and information
processing conference, ISBN 0-7803-8894-1, December 2004, pp.
343–347.
3. J. Siden, H.-E. Nilsson, A. Koptyug, and T. Olsson, A distanced
RFID dipole for a metallic supply chain label, In: Proceedings of
IEEE Antennas and Propagation Society International Symposium,
Albuquerque, New Mexico, July 2006, pp. 3229–3232.
4. M. Polivka, M. Svanda, and P. Hudec, UHF RFID of people, In:
Development and implementation of RFID technology, In-Tech,
Vienna, ISBN 978-3-902613-54-7, 2009.
5. P. Raumonen, et al. Folded dipole antenna near metal plate, In:
Proceedings of IEEE Antennas and Propagation Society Interna-
tional Symposium, Columbus, OH, 2003, ISBN 0-7803-7846-6,
June 2003, pp. 848–851.
6. J.D. Griffin, G.D. Durgin, A. Haldi, and B. Kippelen, RF TAG
antenna performance on various materials using radio link budgets,
IEEE Antennas Wireless Propag Lett 5 (2006), 247–250.
Figure 7 Simulated three-dimensional radiation pattern (directivity) of
coupled patches antenna in free space (a), in the close vicinity of human
body phantom (b)
Figure 8 Comparison of simulated and measured radiation patterns in
horizontal (xz) plane of coupled patches antenna operated in over-the-
shoulder position
596 MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 55, No. 3, March 2013 DOI 10.1002/mop
7. D.M. Dobkin and Weigand, Environmental effects on RFID TAG
antennas, In: Proceedings of IEEE Antennas and Propagation Soci-
ety International Symposium 2005, ISBN 0-7803-8845-3, Washing-
ton, USA, July 2005.
8. M. Svanda and M. Polivka, Two novel extremely low-profile slot-
couplet two-element patch antennas for uhf RFID of people,
Microwave Opt Technol Lett 52 (2010), 249–252.
9. P. Hudec, M. Svanda, and M. Polivka, Communication antenna
intended for fastening on human body, Czech Republic Patent,
302377, March 2011.
10. M. Polivka, M. Svanda, P. Hudec, and S. Zvanovec, UHF radiofre-
quency identification of persons in buildings and open areas, IEEE
Trans Microwave Theory Tech, 57 (2009).
11. G. Marrocco, RFID antennas for the UHF remote monitoring of
human subjects, IEEE Trans Antennas Propag 55 (2007).
12. P.S. Hall and Y. Hao, Antennas and propagation for body centric
communications, In: European Conference on Antennas and Propa-
gation (EuCAP), November 2006.
13. J.G. Santas, A. Alomainy, and H. Yang, Textile antennas for on-
body communications: Techniques and properties, In: European
Conference on Antennas and Propagation (EuCAP), 2007.
VC 2012 Wiley Periodicals, Inc.
UWB POWER DIVIDER WITH ONENARROW NOTCH-BAND AND WIDESTOP-BAND
Lei Chen,1 Feng Wei,2 Chang Jia Gao,2 and Wei Qiang Liu21 School of Electronic and Information Engineering, Xi’anTechnological University, Xi’an 710032, People’s Republic ofChina; Corresponding author: [email protected] National Key Laboratory of Antennas and Microwave Technology,Xidian University, Xi’an 710071, People’s Republic of China
Received 3 July 2012
ABSTRACT: A compact ultrawideband (UWB) microstrip powerdivider (PD) with one sharply rejected notch-band and wide stopband isanalyzed and designed in this article. The proposed UWB PD is based
on conventional Wilkinson PD, while interdigital hairpin resonators areintroduced in two symmetrical output ports to widen passband. The
stepped impedance resonator is studied and used to generate onedesired notched band. Defected ground structure is introduced toimproved stopband performance. Theoretical and simulated results are
presented, which are in good agreement with the measured results.VC 2012 Wiley Periodicals, Inc. Microwave Opt Technol Lett 54:597–
600, 2013; View this article online at wileyonlinelibrary.com. DOI
10.1002/mop.27365
Key words: ultrawideband; power divider; stepped impedanceresonator; defected ground structure
1. INTRODUCTION
Since the ultrawideband (UWB: 3.1–10.6 GHz) spectrum was
regulated for unlicensed use in 2002, many UWB devices and
circuits have been presented and investigated extensively. Power
dividers (PDs) are key components of many microwave systems,
such as balanced mixers and antenna array feed networks. The
most popular PD is the Wilkinson divider, which has good isola-
tion between two output ports while the fractional bandwidth is
less than 20%. Owing to the growth of UWB technology, some
new types of UWB PDs with different structures have been
recently designed [1–3]. In Refs.1 and 2, a novel UWB PD with
UWB bandpass filtering response based on multilayer slotline
structure is proposed, but it requires complex technology and is
hardly compatible with the existing microwave-integrated circuit
(MIC). A UWB microstrip PD with the sharp roll-off skirt using
a pair of stepped-impedance open-circuited stubs and parallel
coupled lines in two output ports is developed in Ref. 3. The
aforementioned PDs exhibit good performance over the UWB
range.
However, the existing undesired narrow band radio signals
such as WLAN signals may interfere with the UWB system. As
a result, a PD designed for UWB applications should also incor-
porate one notch band to suppress interference. UWB PD with a
notched band characteristic is achieved by using stepped imped-
ance resonator (SIR) in Ref. 4. However, the proposed UWB
PD has narrow stopband, which cannot suppress the high-order
harmonics and limits its applications.
A compact UWB microstrip PD with wide pass-band, one
highly rejected notched band, and wide stopband is designed
and implemented in this article [4]. The proposed UWB PD is
based on single-layer microstrip topology structure and one iso-
lation resistor. Good performances in terms of equal power split-
ting and high notch-band rejection are achieved over the UWB
range. Measured results agree well with the simulated results.
2. INTERDIGITAL HAIRPIN RESONATOR
Figure 1 shows the configuration of the microstrip interdigital
hairpin resonator unit, which is composed of three identical
microstrip coupling fingers. The width of the coupling finger is
W2 and the distance between the adjacent coupling fingers is
W3. The coupling-finger length is about one-quarter guided
wavelength with respect to the center frequency of 6.85 GHz.
The microstrip interdigital hairpin resonator unit can be seen
as a six-port network. The network can be equivalent to a two-
port admittance inverter circuit, as shown in Figure 2 [5].
The frequency characteristics of the interdigital hairpin reso-
nator unit are simulated by HFSS 11.0, as shown in Figure 3. It
can be seen from the simulation results that the interdigital hair-
pin resonator can achieve a wide pass-band performance, but the
cutoff frequency response is gradual and the stopband is relative
narrow, which limits its application in UWB system. Figure 4
shows the frequency response of the interdigital hairpin resona-
tor unit with various dimensions. It can be seen that the width
of passband is decreases as L1 increases and increases as W3
decreases [6].
3. STEPPED IMPEDANCE RESONATOR
The proposed folded SIR is constructed by cascading a low-
impedance section in the center accompanied with the two high-
impedance sections in the two sides, and two low-impedance
sections are located in the two terminals. The two
Figure 1 Configuration of the microstrip interdigital hairpin resonator
unit
DOI 10.1002/mop MICROWAVE AND OPTICAL TECHNOLOGY LETTERS / Vol. 55, No. 3, March 2013 597