
- •Contents
- •Preface
- •Chapter 1 Introduction (K. Fujimoto)
- •Chapter 2 Small antennas (K. Fujimoto)
- •Chapter 3 Properties of small antennas (K. Fujimoto and Y. Kim)
- •Chapter 4 Fundamental limitation of small antennas (K. Fujimoto)
- •Chapter 5 Subjects related with small antennas (K. Fujimoto)
- •Chapter 6 Principles and techniques for making antennas small (H. Morishita and K. Fujimoto)
- •Chapter 7 Design and practice of small antennas I (K. Fujimoto)
- •Chapter 8 Design and practice of small antennas II (K. Fujimoto)
- •Chapter 9 Evaluation of small antenna performance (H. Morishita)
- •Chapter 10 Electromagnetic simulation (H. Morishita and Y. Kim)
- •Chapter 11 Glossary (K. Fujimoto and N. T. Hung)
- •Acknowledgements
- •1 Introduction
- •2 Small antennas
- •3 Properties of small antennas
- •3.1 Performance of small antennas
- •3.1.1 Input impedance
- •3.1.4 Gain
- •3.2 Importance of impedance matching in small antennas
- •3.3 Problems of environmental effect in small antennas
- •4 Fundamental limitations of small antennas
- •4.1 Fundamental limitations
- •4.2 Brief review of some typical work on small antennas
- •5 Subjects related with small antennas
- •5.1 Major subjects and topics
- •5.1.1 Investigation of fundamentals of small antennas
- •5.1.2 Realization of small antennas
- •5.2 Practical design problems
- •5.3 General topics
- •6 Principles and techniques for making antennas small
- •6.1 Principles for making antennas small
- •6.2 Techniques and methods for producing ESA
- •6.2.1 Lowering the antenna resonance frequency
- •6.2.1.1 SW structure
- •6.2.1.1.1 Periodic structures
- •6.2.1.1.3 Material loading on an antenna structure
- •6.2.2 Full use of volume/space circumscribing antenna
- •6.2.3 Arrangement of current distributions uniformly
- •6.2.4 Increase of radiation modes
- •6.2.4.2 Use of conjugate structure
- •6.2.4.3 Compose with different types of antennas
- •6.2.5 Applications of metamaterials to make antennas small
- •6.2.5.1 Application of SNG to small antennas
- •6.2.5.1.1 Matching in space
- •6.2.5.1.2 Matching at the load terminals
- •6.2.5.2 DNG applications
- •6.3 Techniques and methods to produce FSA
- •6.3.1 FSA composed by integration of components
- •6.3.2 FSA composed by integration of functions
- •6.3.3 FSA of composite structure
- •6.4 Techniques and methods for producing PCSA
- •6.4.2 PCSA employing a high impedance surface
- •6.5 Techniques and methods for making PSA
- •6.5.2 Simple PSA
- •6.6 Optimization techniques
- •6.6.1 Genetic algorithm
- •6.6.2 Particle swarm optimization
- •6.6.3 Topology optimization
- •6.6.4 Volumetric material optimization
- •6.6.5 Practice of optimization
- •6.6.5.1 Outline of particle swarm optimization
- •6.6.5.2 PSO application method and result
- •7 Design and practice of small antennas I
- •7.1 Design and practice
- •7.2 Design and practice of ESA
- •7.2.1 Lowering the resonance frequency
- •7.2.1.1 Use of slow wave structure
- •7.2.1.1.1 Periodic structure
- •7.2.1.1.1.1 Meander line antennas (MLA)
- •7.2.1.1.1.1.1 Dipole-type meander line antenna
- •7.2.1.1.1.1.2 Monopole-type meander line antenna
- •7.2.1.1.1.1.3 Folded-type meander line antenna
- •7.2.1.1.1.1.4 Meander line antenna mounted on a rectangular conducting box
- •7.2.1.1.1.1.5 Small meander line antennas of less than 0.1 wavelength [13]
- •7.2.1.1.1.1.6 MLAs of length L = 0.05 λ [13, 14]
- •7.2.1.1.1.2 Zigzag antennas
- •7.2.1.1.1.3 Normal mode helical antennas (NMHA)
- •7.2.1.1.1.4 Discussions on small NMHA and meander line antennas pertaining to the antenna performances
- •7.2.1.2 Extension of current path
- •7.2.2 Full use of volume/space
- •7.2.2.1.1 Meander line
- •7.2.2.1.4 Spiral antennas
- •7.2.2.1.4.1 Equiangular spiral antenna
- •7.2.2.1.4.2 Archimedean spiral antenna
- •7.2.2.1.4.3.2 Gain
- •7.2.2.1.4.4 Radiation patterns
- •7.2.2.1.4.5 Unidirectional pattern
- •7.2.2.1.4.6 Miniaturization of spiral antenna
- •7.2.2.1.4.6.1 Slot spiral antenna
- •7.2.2.1.4.6.2 Spiral antenna loaded with capacitance
- •7.2.2.1.4.6.3 Archimedean spiral antennas
- •7.2.2.1.4.6.4 Spiral antenna loaded with inductance
- •7.2.2.2 Three-dimensional (3D) structure
- •7.2.2.2.1 Koch trees
- •7.2.2.2.2 3D spiral antenna
- •7.2.2.2.3 Spherical helix
- •7.2.2.2.3.1 Folded semi-spherical monopole antennas
- •7.2.2.2.3.2 Spherical dipole antenna
- •7.2.2.2.3.3 Spherical wire antenna
- •7.2.2.2.3.4 Spherical magnetic (TE mode) dipoles
- •7.2.2.2.3.5 Hemispherical helical antenna
- •7.2.3 Uniform current distribution
- •7.2.3.1 Loading techniques
- •7.2.3.1.1 Monopole with top loading
- •7.2.3.1.2 Cross-T-wire top-loaded monopole with four open sleeves
- •7.2.3.1.3 Slot loaded with spiral
- •7.2.4 Increase of excitation mode
- •7.2.4.1.1 L-shaped quasi-self-complementary antenna
- •7.2.4.1.2 H-shaped quasi-self-complementary antenna
- •7.2.4.1.3 A half-circular disk quasi-self-complementary antenna
- •7.2.4.1.4 Sinuous spiral antenna
- •7.2.4.2 Conjugate structure
- •7.2.4.2.1 Electrically small complementary paired antenna
- •7.2.4.2.2 A combined electric-magnetic type antenna
- •7.2.4.3 Composite structure
- •7.2.4.3.1 Slot-monopole hybrid antenna
- •7.2.4.3.2 Spiral-slots loaded with inductive element
- •7.2.5 Applications of metamaterials
- •7.2.5.1 Applications of SNG (Single Negative) materials
- •7.2.5.1.1.2 Elliptical patch antenna
- •7.2.5.1.1.3 Small loop loaded with CLL
- •7.2.5.1.2 Epsilon-Negative Metamaterials (ENG MM)
- •7.2.5.2 Applications of DNG (Double Negative Materials)
- •7.2.5.2.1 Leaky wave antenna [116]
- •7.2.5.2.3 NRI (Negative Refractive Index) TL MM antennas
- •7.2.6 Active circuit applications to impedance matching
- •7.2.6.1 Antenna matching in transmitter/receiver
- •7.2.6.2 Monopole antenna
- •7.2.6.3 Loop and planar antenna
- •7.2.6.4 Microstrip antenna
- •8 Design and practice of small antennas II
- •8.1 FSA (Functionally Small Antennas)
- •8.1.1 Introduction
- •8.1.2 Integration technique
- •8.1.2.1 Enhancement/improvement of antenna performances
- •8.1.2.1.1 Bandwidth enhancement and multiband operation
- •8.1.2.1.1.1.1 E-shaped microstrip antenna
- •8.1.2.1.1.1.2 -shaped microstrip antenna
- •8.1.2.1.1.1.3 H-shaped microstrip antenna
- •8.1.2.1.1.1.4 S-shaped-slot patch antenna
- •8.1.2.1.1.2.1 Microstrip slot antennas
- •8.1.2.1.1.2.2.2 Rectangular patch with square slot
- •8.1.2.1.2.1.1 A printed λ/8 PIFA operating at penta-band
- •8.1.2.1.2.1.2 Bent-monopole penta-band antenna
- •8.1.2.1.2.1.3 Loop antenna with a U-shaped tuning element for hepta-band operation
- •8.1.2.1.2.1.4 Planar printed strip monopole for eight-band operation
- •8.1.2.1.2.2.2 Folded loop antenna
- •8.1.2.1.2.3.2 Monopole UWB antennas
- •8.1.2.1.2.3.2.1 Binomial-curved patch antenna
- •8.1.2.1.2.3.2.2 Spline-shaped antenna
- •8.1.2.1.2.3.3 UWB antennas with slot/slit embedded on the patch surface
- •8.1.2.1.2.3.3.1 A beveled square monopole patch with U-slot
- •8.1.2.1.2.3.3.2 Circular/Elliptical slot UWB antennas
- •8.1.2.1.2.3.3.3 A rectangular monopole patch with a notch and a strip
- •8.1.2.1.2.3.4.1 Pentagon-shape microstrip slot antenna
- •8.1.2.1.2.3.4.2 Sectorial loop antenna (SLA)
- •8.1.3 Integration of functions into antenna
- •8.2 Design and practice of PCSA (Physically Constrained Small Antennas)
- •8.2.2 Application of HIS (High Impedance Surface)
- •8.2.3 Applications of EBG (Electromagnetic Band Gap)
- •8.2.3.1 Miniaturization
- •8.2.3.2 Enhancement of gain
- •8.2.3.3 Enhancement of bandwidth
- •8.2.3.4 Reduction of mutual coupling
- •8.2.4 Application of DGS (Defected Ground Surface)
- •8.2.4.2 Multiband circular disk monopole patch antenna
- •8.2.5 Application of DBE (Degenerated Band Edge) structure
- •8.3 Design and practice of PSA (Physically Small Antennas)
- •8.3.1 Small antennas for radio watch/clock systems
- •8.3.2 Small antennas for RFID
- •8.3.2.1 Dipole and monopole types
- •8.3.2.3 Slot type antennas
- •8.3.2.4 Loop antenna
- •Appendix I
- •Appendix II
- •References
- •9 Evaluation of small antenna performance
- •9.1 General
- •9.2 Practical method of measurement
- •9.2.1 Measurement by using a coaxial cable
- •9.2.2 Method of measurement by using small oscillator
- •9.2.3 Method of measurement by using optical system
- •9.3 Practice of measurement
- •9.3.1 Input impedance and bandwidth
- •9.3.2 Radiation patterns and gain
- •10 Electromagnetic simulation
- •10.1 Concept of electromagnetic simulation
- •10.2 Typical electromagnetic simulators for small antennas
- •10.3 Example (balanced antennas for mobile handsets)
- •10.3.2 Antenna structure
- •10.3.3 Analytical results
- •10.3.4 Simulation for characteristics of a folded loop antenna in the vicinity of human head and hand
- •10.3.4.1 Structure of human head and hand
- •10.3.4.2 Analytical results
- •11 Glossary
- •11.1 Catalog of small antennas
- •11.2 List of small antennas
- •Index

8.3 Design and practice of PSA |
347 |
|
|
1.05 inch (2.67 cm)
cm) 24.(2 inch 88.0
50 Ω Coaxial cable |
(capacitively coupled) |
Figure 8.98 Microstrip (MS) DBE layout on a 2 × 2 (in inches) substrate ([83], copyright C 2009 IEEE).
Theta |
13 dB directivity |
|
11.7 dB realized gain |
|
2% bandwidth |
Z
X
array elements |
Y |
|
Figure 8.99 Radiation pattern of a 4 × 4 MS-DBE array using element in Fig. 8.98 ([83], copyright C 2009 IEEE).
and the bandwidth is increased to 3.5%. Tangential electric field magnitude on the top surface around the antenna element is shown in Figure 8.100(b).
8.3Design and practice of PSA (Physically Small Antennas)
A PSA is an antenna that is not necessarily ESA, but simply is a physically small antenna, including ESA. Various recently emerged wireless systems, for not only

348 |
Design and practice of small antennas II |
|
|
(a)
|
|
|
2 inch (5.08 cm) |
0.85 inch (2.16 cm) |
|
1.5000e+004 |
|
|
|
1.4000e+004 |
|
.0 |
|
1.3000e+004 |
|
|
1.2000e+004 |
|
|
88 |
|
|
|
|
1.1000e+004 |
cm)08.(5inch2 |
|
cm)24.(2inch |
|
||
|
1.0000e+004 |
||
|
|
|
|
|
|
9.0004e+003 |
|
|
(b) |
8.0005e+003 |
|
|
7.0005e+003 |
|
|
|
|
|
|
|
|
6.0006e+003 |
|
|
|
5.0007e+003 |
|
|
|
4.0007e+003 |
|
|
|
3.0008e+003 |
|
|
|
2.0009e+003 |
|
50 Ω Coaxial cable |
|
1.0009e+003 |
|
|
1.0000e+003 |
|
Figure 8.100 (a) Small-sized MS-DBE layout on a 2 × 2 (in inches) substrate and (b) tangential electric field magnitude on the top surface ([83], copyright C 2009 IEEE).
communications, but also for control, sensor, data transmission, identification, remote sensing, wireless power transmission, and so forth, require small antennas to fit into the units of small pieces of equipment for those systems. Typical wireless applications are such systems as various short-range communications, for instance NFC (Near Field Communications), including RFID (Radio Frequency Identification), where numerous applications have been deployed practically in the recent decade, and radio watches/clocks, which operate very precisely with nearly standard time, being synchronized automatically by receiving time signals from long-wave standard-time broadcasting stations.
Types of antennas are not necessarily specific to these applications, but generally they are conventional types. However, most of them are specifically designed to fit into the small equipment used in the various applications and yet satisfy the requirements for each system. Antennas are not necessarily ESAs; however, antennas in almost all these cases need to be miniaturized and ESA techniques are employed as almost inevitable means. The techniques include application of slow-wave concepts, lowering resonance frequency, filling space with radiation elements, increase of radiation modes, and so forth, as covered previously in this chapter.
As the antenna dimensions become smaller, evaluation of antenna performances tends to become harder to obtain correct results. Special techniques to evaluate antenna performances often are required. However, the appropriate electromagnetic simulations may gain greater importance for replacing the measurements when evaluating antenna performances. The simulation can be used even for design of small antennas.
Another important problem is impedance matching of antenna to the load, conventionally a resistance of 50 . In cases of very small RFID equipment, for example, the antenna is often directly connected to the RF circuits, which has impedance not of 50, but usually a much higher impedance. Further, connection of a type of balanced antenna with unbalanced circuits or vice versa may often be encountered. Without good

8.3 Design and practice of PSA |
349 |
|
|
Antenna
(a) |
(b) |
Figure 8.101 (a) A wristwatch front view and (b) inside view to show a small coil antenna installed wristwatch ([84], copyright C 2007 IEEE, and [85], copyright C 2006 IEEE).
matching between the antenna and the load, the best system performance cannot be realized, meaning the desired operation range in the RFID system, for instance, might never be attained. Unfortunately, it has so far been recognized that there have been many systems operating in mismatched condition without careful considerations on the design. It may not be easy to obtain the perfect matching conditions, especially when the system operates over a wide frequency band; however, since it is an indispensable requirement, a means must be contrived to achieve suitably good matching. The method is not very specific, but conventional ways of matching can be applied.
8.3.1Small antennas for radio watch/clock systems
Standard-time signals are broadcast from numerous radio stations of the world. In
Japan, there are two long-wave broadcasting stations for JST (Japan Standard Time), which provide accuracy of ±1 × 10−12. A watch/clock, into which a very small receiver
with a small magnetic-core loop antenna is integrated, receives the JST signal through the broadcasting of either 40 or 60 kHz from one of the two stations and automatically adjusts the time display to agree closely with the JST. A view of a wristwatch, in which a small receiver with a coil antenna is installed, is illustrated in Figure 8.101; (a) the front view and (b) the inside view, where the antenna is indicated with an arrow [84]. An example of a coil antenna is shown in Figure 8.102 [84, 85]. In the case of amorphous metal material, the core is composed of multilayered very thin film materials as shown in Figure 8.102. The amorphous material has permeability μr of around 8800, the thickness of a film is 0.16 µm, and a core is comprised of 40 films, half of which are bent slightly upward at the edge of the core to improve the sensitivity, Figure 8.103 shows a fabricated antenna. The antenna is designed to operate at 40 and/or 60 kHz, with length