Broadbanding techniques of MSA for implantable devices.

1. Review of Various Broadband
Techniques for MSAs

2. Definition of Bandwidth

3. Modified Shape Patches
The regularMSA configurations, such as rectangular and circular patches have
been modified to rectangular ring [38] and circular ring [39], respectively, to
enhance the BW. The larger BW is because of a reduction in the quality
factor Q of the patch resonator, which is due to less energy stored beneath
the patch and higher radiation. When a U-shaped slot is cut inside the
rectangular patch, it gives a BW of approximately 40% for VSWR £ 2 [40].
Similar results are obtained when a U-slot is cut inside a circular or a
triangular MSA [41, 42]. These configurations are discussed in detail in
Chapter 6.
Planar Multiresonator Configurations
The planar stagger–tuned coupled multiple resonators yield wide BW in the
same way as in the case of multistage tuned circuits. Several configurations
are available yielding BW of 5–25% [43–49]. Various parasitic patches like
narrow strips, shorted quarter-wavelength rectangular patches, and rectangular
resonator patches have been gap-coupled to the central-fed rectangular
patch. Three combinations of gap-coupled rectangular patches are shown in
Figure 1.5. To reduce the criticality of the gap coupling, direct coupling as
depicted in Figure 1.6 has been used to obtain broad BW. Both gap and
direct (hybrid) coupling have been used with circular MSAs (CMSAs) and
equilateral triangular MSAs (ETMSAs) to yield broad BW.

5. Multilayer Configurations
In the multilayer configuration, two or more patches on different layers of
the dielectric substrate are stacked on each other. Based on the coupling
mechanism, these configurations are categorized as electromagnetically coupled
or aperture-coupled MSAs.

8. The concept of log-periodic antenna has been applied to MSA to obtain a
multi-octave BW. In this configuration, the patch dimensions are increased logarithmically
and the subsequent patches are fed at 180° out of phase
with respect to the previous patch [67–70]. The main disadvantage of this
configuration is that the radiation pattern varies significantly over the impedance
BW as described in Chapter 5.

9. Ferrite Substrate-Based Broadband MSAs
The multiresonant behavior of a patch on a ferrite substrate yields a broadBW of about
three octaves by changing the magnetic field. Also, the dimensions of the patch are
reduced because of the high dielectric constant of the ferrite substrate. However, the
efficiency of these antennas is poor because of lossy substrate and requires external
magnetic fields, which makes it bulky [71–73]. The methods for increasing the BW of MSA
are continuously getting upgraded. The search for an ideal broadband MSA is still
continuing. Perhaps a combination of various approaches would lead to an optimum
broadband configuration.
Broadband Compact MSAs
The size of a half-wavelength (l /2) RMSA is too large in the ultra-high frequency (UHF) band.
There is a need for a compact MSA for personal mobile communication and other
applications. A shorted l /4 RMSA has the same resonance frequency as that of a l /2 RMSA,
with half the area [74]. The resonance frequency reduces further as the width of the shorting
plate decreases [74, 75]. Similarly, compact MSA in circular and triangular configurations is
realized by placing shorting posts at the zero potential lines [76, 77]. A single shorting post
yields a maximum reduction in the resonance frequency of the rectangular, circular, and
triangular MSAs [78–80]. The compact antennas have also been realized by cutting slots in
regularly shaped antennas. The requirements of these compact broadband MSAs will
increase in the future due to the ever-growing miniaturization of communication systems.
The BW of the compact MSA has been increased in both planar as well as multilayer
configurations

10. Tunable and Dual-Band MSAs
Tunable MSAs are of interest in many systems as they can be tuned over a large
frequency range. These tunable antennas provide an alternative to large- BW antennas,
especially when a large BW is required for encompassing several narrowband channels.
The tunable MSA is realized by changing the length of the small stub attached to the
regularly shaped MSA [84, 85], or by changing the number of shorting posts used to
make a compact configuration [74, 76, 77]. Tunability is also achieved by integrating
active devices such as varactor or PIN diodes along with the MSA [86]. When an antenna
must operate at two frequencies that are far apart, a dual-frequency antenna can be
used to avoid the use of two separate antennas. When two or more resonance
frequencies of a MSA are close to each other, a broad BW is obtained. When these are
separated, dual-band operation is obtained. In general, all the methods described earlier
for increasing the BW of MSAs can be utilized to obtain dual-band characteristics. In the
single-layer MSA, dual-band operation is achieved by using either slot or shorting pins or
varactor or optically tuned diodes or by selecting the proper length of a stub [9, 85–89].
In multilayer configurations, either electromagnetic or aperture coupling could be used
for dual-frequency operation [90–92]. The separation between the two frequencies is
obtained by adjusting the air gap between the two layers or by changing the dimensions
of the patches.

11. Broadband Circularly Polarized MSAs
CP is particularly useful for a number of radar, communication, and navigation systems because
the rotational orientations of the transmitter and the receiver antennas are unimportant in
relation to the received signal strength. With linearly polarized signals, on the other hand, there
will be only very weak reception if the transmitter and receiver antennas are nearly orthogonal.
Also, the circularly polarized wave reverses its sense of polarization from right-hand to left-hand
CP and vice versa after reflection from regular objects. The system will then tend to discriminate
the reception of such reflected signals from other signals arising from direct paths on reflections
from irregular shapes. CP is generated when two orthogonal modes are excited in a phase
quadrature with equal magnitude. A rectangular or circular MSA generates CP when fed at two
orthogonal points with equal amplitude and 90° phase difference. CP can also be generated by
using a single-feed MSA. Singlefeed MSA configurations include diagonal fed nearly square,
corner chopped square, and square with diagonal slot. Similar variations are possible for
circular and triangular MSAs. Broadband CP is obtained by using dual-feed multiple planar or
stacked patches, or single-feed MSA in a sequential rotation array configuration.

12. Broadband Planar Monopole Antennas
MSA in its regular shape cannot yield multi-octaveBWbecause of its resonant
nature. Some modification of the MSA configuration is required to obtain
an octave BW. If a rectangular patch without the substrate and ground plane
is fed at the edge by a coaxial feed with a perpendicular ground plane, then
the patch will have an effective dielectric constant equal to 1 with large h.
Both of these factors yield broad BW. This modified configuration can be
thought of as a planar rectangular monopole antenna [99]. Other configurations
such as triangular, hexagonal, circular, and elliptical monopoles also
yield broad BW. An elliptical monopole with an ellipticity of 1.1 yields BW
of 1:11 for VSWR > 2.

13. L-shaped probe:
Capacitive “top hat” on probe:
Top view
13
Improving Bandwidth
Probe Compensation
As the substrate
thickness increases the
probe inductance limits
the bandwidth – so we
compensate for it.

14. SSFIP: Strip Slot Foam Inverted Patch (a version of the ACP).
Microstrip
substrate
Patch
Microstrip line Slot
Foam
Patch substrate
 Bandwidths greater than 25% have been achieved.
 Increased bandwidth is due to the thick foam substrate and
also a dual-tuned resonance (patch+slot).
14
Improving Bandwidth
Note: There is no probe inductance to worry about here.
J.-F. Zürcher and F. E. Gardiol, Broadband Patch Antennas, Artech House, Norwood, MA, 1995.

15.  Bandwidth increase is due to thick low-permittivity antenna
substrates and a dual or triple-tuned resonance.
 Bandwidths of 25% have been achieved using a probe feed.
 Bandwidths of 100% have been achieved using an ACP feed.
Microstrip
substrate
Driven patch
Microstrip line
Slot
Patch substrates
Parasitic patch
15
Improving Bandwidth
Stacked Patches

16. Bandwidth (S11 = -10 dB) is about 100%
Stacked patch with ACP feed
3 4 5 6 7 8 9 10 11 12
Frequency (GHz)
-40
-35
-30
-25
-20
-15
-10
-5
0
ReturnLoss(dB)
Measured
Computed
16
Improving Bandwidth
Stacked Patches
(Photo courtesy of Dr. Rodney B. Waterhouse)

17. Stacked patch with ACP feed
0
0.2
0.5
1
2
5
10
180170160
150
140
130
120
110 100 90 80
70
60
50
40
30
20
100-10-20
-30
-40
-50
-60
-70
-80-90-100-110
-120
-130
-140
-150
-160-170
4 GHz
13 GHz
Two extra loops are observed on the Smith chart.
17
Stacked Patches
Improving Bandwidth
(Photo courtesy of Dr. Rodney B. Waterhouse)

18. Radiating Edges Gap Coupled
Microstrip Antennas
(REGCOMA).
Non-Radiating Edges Gap
Coupled Microstrip Antennas
(NEGCOMA)
Four-Edges Gap Coupled
Microstrip Antennas
(FEGCOMA)
Bandwidth improvement factor:
REGCOMA: 3.0, NEGCOMA: 3.0, FEGCOMA: 5.0?
Mush of this work
was pioneered by
K. C. Gupta.
18
Improving Bandwidth
Parasitic Patches

19. Radiating Edges Direct
Coupled Microstrip Antennas
(REDCOMA).
Non-Radiating Edges Direct
Coupled Microstrip Antennas
(NEDCOMA)
Four-Edges Direct Coupled
Microstrip Antennas
(FEDCOMA)
Bandwidth improvement factor:
REDCOMA: 5.0, NEDCOMA: 5.0, FEDCOMA: 7.0
19
Improving Bandwidth
Direct-Coupled Patches

20. The introduction of a U-shaped slot can give a
significant bandwidth (10%-40%).
(This is due to a double resonance effect, with two different modes.)
“Single Layer Single Patch Wideband Microstrip Antenna,” T. Huynh and K. F. Lee,
Electronics Letters, Vol. 31, No. 16, pp. 1310-1312, 1986.
20
Improving Bandwidth
U-Shaped Slot

21. A 44% bandwidth was achieved.
Y. X. Guo, K. M. Luk, and Y. L. Chow, “Double U-Slot Rectangular Patch Antenna,”
Electronics Letters, Vol. 34, No. 19, pp. 1805-1806, 1998.
21
Improving Bandwidth
Double U-Slot

22. A modification of the U-slot patch.
A bandwidth of 34% was achieved (40% using a capacitive “washer” to
compensate for the probe inductance).
B. L. Ooi and Q. Shen, “A Novel E-shaped Broadband Microstrip Patch Antenna,”
Microwave and Optical Technology Letters, vol. 27, No. 5, pp. 348-352, 2000.
22
Improving Bandwidth
E Patch

23. Multi-Band Antennas
General Principle:
Introduce multiple resonance paths into the antenna.
A multi-band antenna is sometimes more desirable than a broadband
antenna, if multiple narrow-band channels are to be covered.
23

24. Dual-band E patch
High-band
Low-band
Low-band
Feed
Dual-band patch with parasitic strip
Low-band
High-band
Feed
24
Multi-Band Antennas

25. 1.4 Methods of Analysis
The MSA generally has a two-dimensional radiating patch on a thin dielectric
substrate and therefore may be categorized as a two-dimensional planar
component for analysis purposes. The analysis methods for MSAs can be
broadly divided into two groups.
In the first group, the methods are based on equivalent magnetic current
distribution around the patch edges (similar to slot antennas). There are
three popular analytical techniques:
· The transmission line model;
· The cavity model;
· The MNM.
In the second group, the methods are based on the electric current
distribution on the patch conductor and the ground plane (similar to dipole
antennas, used in conjunction with full-wave simulation/numerical analysis
methods). Some of the numerical methods for analyzing MSAs are listed as
follows:
· The method of moments (MoM);
· The finite-element method (FEM);
· The spectral domain technique (SDT);
· The finite-difference time domain (FDTD)
method.
This section briefly describes these methods.

26. 1.4.1 Transmission Line Model
The transmission line model is very simple and helpful in understanding
the basic performance of a MSA. The microstrip radiator element is viewed
as a transmission line resonator with no transverse field variations (the field
only varies along the length), and the radiation occurs mainly from the
fringing fields at the open circuited ends. The patch is represented by two
slots that are spaced by the length of the resonator. This model was originally
developed for rectangular patches but has been extended for generalized
patch shapes. Many variations of this method have been used to analyze the
MSA [9, 20–22].
Although the transmission line model is easy to use, all types of configurations
can not be analyzed using this model since it does not take care of
variation of field in the orthogonal direction to the direction of propagation.

27. 1.4.2 Cavity Model
In the cavity model, the region between the patch and the ground plane is
treated as a cavity that is surrounded by magnetic walls around the periphery
and by electric walls from the top and bottom sides. Since thin substrates
are used, the field inside the cavity is uniform along the thickness of the
substrate [23–25]. The fields underneath the patch for regular shapes such
as rectangular, circular, triangular, and sectoral shapes can be expressed as
a summation of the various resonant modes of the two-dimensional resonator.
The fringing fields around the periphery are taken care of by extending
the patch boundary outward so that the effective dimensions are larger than
the physical dimensions of the patch. The effect of the radiation from the
antenna and the conductor loss are accounted for by adding these losses to
the loss tangent of the dielectric substrate. The far field and radiated power
are computed from the equivalent magnetic current around the periphery.
An alternate way of incorporating the radiation effect in the cavity
model is by introducing an impedance boundary condition at the walls of
the cavity. The fringing fields and the radiated power are not included inside the cavity
but are localized at the edges of the cavity. However, the solution
for the far field, with admittance walls is difficult to evaluate

28. 1.4.3 MNM
The MNM for analyzing the MSA is an extension of the cavity model [9,
26, 27]. In this method, the electromagnetic fields underneath the patch
and outside the patch are modeled separately. The patch is analyzed as a
two-dimensional planar network, with a multiple number of ports located
around the periphery. The multiport impedance matrix of the patch is
obtained from its two-dimensional Green’s function. The fringing fields
along the periphery and the radiated fields are incorporated by adding an
equivalent edge admittance network. The segmentation method is then used
to find the overall impedance matrix. The radiated fields are obtained from the
voltage distribution around the periphery. Appendix C details this method.
The above three analytical methods offer both simplicity and physical
insight. In the latter two methods, the radiation from the MSA is calculated
from the equivalent magnetic current distribution around the periphery
of the radiating patch, which is obtained from the corresponding voltage
distribution. Thus, the MSA analysis problem reduces to that of finding the
edge voltage distribution for a given excitation and for a specified mode.
These methods are accurate for regular patch geometries, but—except for
MNMwith contour integration techniques—they are not suited for arbitrary
shaped patch configurations. For complex geometries, the numerical techniques
described below are employed [9].

29. 1.4.4 MoM
In the MoM, the surface currents are used to model the microstrip patch,
and volume polarization currents in the dielectric slab are used to model
the fields in the dielectric slab. An integral equation is formulated for the
unknown currents on the microstrip patches and the feed lines and their
images in the ground plane [28]. The integral equations are transformed
into algebraic equations that can be easily solved using a computer. This
method takes into account the fringing fields outside the physical boundary
of the two-dimensional patch, thus providing a more exact solution. This
book makes extensive use of a commercially available software IE3D [29]
based on MoM to analyze various MSA configurations.

30. 1.4.5 FEM
The FEM, unlike the MoM, is suitable for volumetric configurations. In
this method, the region of interest is divided into any number of finite surfaces
or volume elements depending upon the planar or volumetric structures to
be analyzed [30]. These discretized units, generally referred to as finite
elements, can be any well-defined geometrical shapes such as triangular
elements for planar configurations and tetrahedral and prismatic elements
for three-dimensional configurations, which are suitable even for curved
geometry. It involves the integration of certain basis functions over the entire
conducting patch, which is divided into a number of subsections. The
problem of solving wave equations with inhomogeneous boundary conditions
is tackled by decomposing it into two boundary value problems, one with
Laplace’s equation with an inhomogeneous boundary and the other corresponding
to an inhomogeneous wave equation with a homogeneous boundary
condition

31. 1.4.6 SDT
In the SDT, a two-dimensional Fourier transform along the two orthogonal
directions of the patch in the plane of substrate is employed. Boundary
conditions are applied in Fourier transform plane. The current distribution
on the conducting patch is expanded in terms of chosen basis functions,
and the resulting matrix equation is solved to evaluate the electric current
distribution on the conducting patch and the equivalent magnetic current
distribution on the surrounding substrate surface. The various parameters
of the antennas are then evaluated
1.4.7 FDTD Method
The FDTD method is well-suited for MSAs, as it can conveniently model
numerous structural inhomogenities encountered in these configurations
[10]. It can also predict the response of the MSA over the wide BW with
a single simulation. In this technique, spatial as well as time grid for the
electric and magnetic fields are generated over which the solution is required.
The spatial discretizations along three Cartesian coordinates are taken to be
same. The E cell edges are aligned with the boundary of the configuration
and H-fields are assumed to be located at the center of each E cell. Each
cell contains information about material characteristics. The cells containing
the sources are excited with a suitable excitation function, which propagates
along the structure. The discretized time variations of the fields are deter

32. mined at desired locations. Using a line integral of the electric field, the
voltage across the two locations can be obtained. The current is computed
by a loop integral of the magnetic field surrounding the conductor, where
the Fourier transform yields a frequency response.
The above numerical techniques, which are based on the electric current
distribution on the patch conductor and the ground plane, give results
for any arbitrarily shaped antenna with good accuracy, but they are timeconsuming.
These methods can be used to plot current distributions on
patches but otherwise provide little of the physical insight required for
antenna design.

33. Feeding Techniques

34. Feeding Techniques:
 Coaxial feed
 Microstrip feed
 Proximity coupled microstrip feed
 Aperture coupled microstrip feed
 Coplanar wave guide
 Line Feed
1-Microstrip Line Feed :
In this type of feed technique, a conducting
strip is connected directly to the edge of the
microstrip patch.
This kind of feed arrangement has the
advantage that the feed can be etched on the
same substrate to provide a planar structure.

35. 2-Coaxial Feed :-
The Coaxial feed or probe feed is a very common
technique used for feeding Microstrip
patch antennas.
Probe fed Rectangular Microstrip Patch
Antenna from top
Probe fed Rectangular Microstrip Patch Antenna from
side view
The main advantage of this type of feeding
scheme is that the feed can be placed at any
desired location inside the patch in order to
match with its input impedance.
This feed method is easy to fabricate and has
low spurious radiation.
However, its major disadvantage is that it
Coaxial Ground Plane Connector Substrate
Patch provides narrow bandwidth and is
difficult to model since a hole has to be drilled
in the substrate . and the connector protrudes
outside the ground plane, thus not making it
completely planar for thick substrates .

36. 3-Aperture Coupled Feed
In this type of feed technique, the radiating patch
and the microstrip feed line are separated by the
ground plane .
Coupling between the patch and the feed
line is made through a slot or an aperture in
the ground plane.
Aperture-coupled feedThe coupling aperture is usually centered under the patch,
leading to lower cross polarization due to symmetry of the
configuration.
The amount of coupling from the feed line to the patch is determined by the shape, size and
location of the aperture.

37. Comparing the different feed techniques :-