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MOHAMMAD ABEDIAN KASGARI

A thesis submitted in fulfilment of the requirements for the award of the degree of Doctor of Philosophy (Electrical Engineering)

Faculty of Electrical Engineering Universiti Teknologi Malaysia

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To my beloved parents, who their enthusiasm and encouragement, I would never step in this way

and

To my beloved, mindful understanding wife, Shadi, who supported me each step of the way.

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ACKNOWLEDGEMENT

I would like to acknowledge my supervisor Associated Professor Ir. Dr. Sharul Kamal Abdul Rahim who has given me support and guidance throughout the period of this project. His patience and perseverance towards the outcome of this study is of the highest standard. Without him this project report will not become a reality.

None of this would have been possible without the love, support and encouragement of my family. Mom and Dad, I did it. I am forever thankful to them for allowing me to fulfill my dream. To my sister, Roja, thanks for all the love and support. I am sure you would be so proud of me if you were here. I love you.

Words fail me to express my appreciation to my beloved wife, Shadi Danesh, whose dedication, love and persistent confidence in me, has taken the load off my shoulder. I owe her for being unselfishly let her intelligence, passions, and ambitions collide with mine. I can’t thank you enough. I love you.

Thanks all of you

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ABSTRACT

UWB communication systems were newly regenerated when the Federal Communications Commission (FCC) defined the 3.1-10.6 GHz unlicensed band for UWB applications. Based on an investigation in designing UWB antennas, researchers have encountered more difficulties compared to a narrow band antenna. UWB antennas should have extremely wide impedance bandwidth while preserving high radiation efficiency with compact size. In some cases, a band-notched function should have been created to avoid electromagnetic interference between nearby existing systems and UWB systems. In this research, various promising UWB Dielectric Resonator Antennas (DRAs) have been demonstrated to overcome several challenges. The impedance bandwidth of the UWB DRAs has been improved for more than 110% by using some techniques such as connecting a strip to the ground plane and modifying structure of Dielectric Resonator (DR). The efficiency issue of UWB antennas is overcome by implementing DR as a resonator element which is excited by various shape structures feed lines to achieve more than 90% efficiency. The electromagnetic interferences between UWB systems and nearby existing systems in the frequency bands of 3.22-4.06 GHz, 4.84-5.96 GHz and 5.71-6.32 GHz are eliminated by using a stub connected to the hollow centre of feed line, an inverted-T shape parasitic strip near DR and modified metallic sheet underneath the DR, respectively. Compared with UWB monopole antennas, UWB DRAs obviate the problem of radiation pattern by utilizing dielectric resonator characteristics. In parallel, the broadside radiation pattern is obtained by implementing various shapes of microstrip feed line at a proper location to excite the DRA that provides symmetry radiation patterns with a consistent stability across the desired bandwidth.

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ABSTRAK

Sistem komunikasi UWB adalah baru tumbuh semula apabila Suruhanjaya Komunikasi Persekutuan (FCC) mentakrifkan 3.1-10.6 GHz band yang tidak berlesen untuk aplikasi UWB. Berdasarkan kajian di dalam mereka bentuk antena UWB, para penyelidik menghadapi lebih kesukaran berbanding dengan mereka bentuk antena jalur sempit. Antena UWB harus mempunyai lebar jalur galangan masukan yang sangat luas di samping kecekapan pada radiasi tinggi dengan saiz yang kompak. Dalam beberapa kes, fungsi jalur-bertakuk dicipta untuk mengelakkan gangguan elektromagnet di antara sistem sedia ada dan sistem UWB. Di dalam kajian ini, pelbagai UWB bentuk Antena Penyalun Dielektrik (DRAs) dicipta bagi mengatasi beberapa cabaran berkaitan UWB. Lebar jalur galangan masukan daripada DRAs UWB dipertingkatkan dengan lebih daripada 110% menggunakan beberapa teknik seperti menghubungkan jalur dengan satah tanah dan mengubah suai struktur Penyalun Dielektrik. Isu kecekapan antena UWB diatasi dengan melaksanakan DR sebagai elemen resonator yang teruja dengan pelbagai struktur bentuk talian untuk mencapai kecekapan yang lebih daripada 90%. Gangguan elektromagnetik antara sistem UWB dan sistem sedia ada yang berdekatan dalam jalur frekuensi 3.22-4.06 GHz, 4.84-5.96 GHz, dan 5.71-6.32 GHz dapat dikurangkan dengan menggunakan puntung yang dihubungkan dengan pusat berongga talian makanan bentuk-T terbalik jalur parasit berhampiran DR dan lembaran logam diubah suai bawahnya DR, masing-masing. Berbanding dengan UWB antena monopole, DRAs UWB menyelesaikan masalah corak sinaran dengan menggunakan ciri-ciri resonator dielektrik. Pada masa yang sama, corak sinaran selebaran diperolehi dengan melaksanakan pelbagai bentuk garis jalur mikro di lokasi yang betul, untuk merangsang DRA yang menyediakan corak sinaran simetri dengan kestabilan yang konsisten di seluruh lebar jalur yang dikehendaki.

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TABLE OF CONTENTS CHAPTER TITLE PAGE DECLARATION ii DEDICATION iii ACKNOWLEDGEMENT iv ABSTRACT v ABSTRAK vi

TABLE OF CONTENTS vii

LIST OF TABLES xi

LIST OF FIGURES xii

LIST OF ABBREVIATIONS xvi

LIST OF SYMBOLS xviii

LIST OF APPENDICES xix

1 INTRODUCTION 1

1.1 Background of the Study 1

1.2 Problem Statement 2

1.3 Research Objective 3

1.4 Scopes of Project 3

1.5 Contribution of the Research 4

1.6 Signification of the Research 5

1.7 Thesis Outlines 5

2 LITRATURE REVIEW 7

2.1 Introduction 7

2.2 History of UWB Antennas 8

2.3 Dielectric Resonators Antennas 11

2.3.1 Geometries and Characteristics of

Dielec-tric Resonator 12

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2.3.1.2 Cylindrical DRA 14

2.3.1.3 Rectangular DRA 15

2.4 Coupling Mechanisms of DRAs 18

2.4.1 Microstrip Feed Line 19

2.4.2 Coaxial Probe Feed 22

2.4.3 Coplanar Waveguide Feed 23

2.4.4 Dielectric Image Guide Coupling 24

2.4.5 Aperture Coupling 25

2.4.6 Summary of Coupling Mechanisms 27

2.5 Bandwidth Enhancement of DRAs 27

2.5.1 Single Element Methods 27

2.5.1.1 Modified Shape of the DRAs 27 2.5.1.2 Modified Feed Geometries 30 2.5.1.3 Introducing an Air Gap

Be-tween the DR and Ground Plane 32

2.5.1.4 Multi-Segment DRAs 34

2.5.1.5 Attaching Parasitic Patch on the

DRAs 36

2.5.2 Multiple DRAs 37

2.5.2.1 Stacked DRAs 37

2.5.2.2 Embedded DRAs 39

2.5.3 Hybrid DRAs 41

2.5.4 Summary of Bandwidth Enhancement 42

2.6 UWB Antennas with Band Rejection 43

2.6.1 Band Rejection Techniques 43

2.6.2 Summary of UWB DRAs with Band

Rejection 49

2.7 Summary 52

3 RESEARCH METHODOLOGY 53

3.1 Introduction 53

3.2 Methodology 53

3.3 Design of UWB DRA with and without Band

Rejection 56

3.3.1 Specifications of Design 56

3.3.2 Dielectric Resonator Specifications 57

3.3.3 Substrate Material 58

3.4 Software and Measurement Equipment 59

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4 DESIGN OF COMPACT UWB DIELECTRIC

RES-ONATOR ANTENNA 62

4.1 Introduction 62

4.2 Design of Two-Segment Compact UWB DRA 63 4.2.1 Two-Segment Compact UWB DRA

Con-figuration 64

4.2.2 Parametric Study of Two-Segment

Com-pact UWB DRA 64

4.2.3 Experimental Results of Two-Segment

Compact UWB DRA 68

4.3 Design of a Compact UWB Rectangular DRA 72 4.3.1 Geometry of a Compact UWB

Rectangu-lar DRA 72

4.3.2 Parametric Study of a Compact UWB

Rectangular DRA 73

4.3.3 Experimental Results of a Compact UWB

Rectangular DRA 74

4.4 Performance Comparison Between Two-Segment

and Rectangular UWB DRAs 78

4.5 Summary 80

5 UWB DIELCTRIC RESONATOR ANTENNA DESIGN

WITH BAND REJECTION FUNCTION 81

5.1 Introduction 81

5.2 UWB DRA with single Band-Notch for Upper

WLAN Band at 5.8 GHz 82

5.2.1 Geometry of Single Band-notch UWB

DRA 82

5.2.2 Parametric Study of Single Band-notch

UWB DRA 82

5.2.3 Experimental Results of Single

Band-notch UWB DRA 88

5.3 Compact UWB DRA with Dual Band Rejection

Characteristics for WiMAX/WLAN Bands 92 5.3.1 UWB DRA with Dual Band Rejection

Configuration 92

5.3.2 Parametric Study and Key Parameters of

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5.3.3 Experimental Results of UWB DRA with

Dual Band Rejection 102

5.4 Performance Comparison between Single and Dual

Band-notch UWB DRAs 106

5.5 Summary 106

6 CONCLUSION AND FUTURE WORK 108

6.1 Conclusion 108

6.2 Recommendations for Future Works 109

REFERENCES 110

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LIST OF TABLES

TABLE NO. TITLE PAGE

2.1 Microstrip feed line technique to excite DRAs 20

2.2 Coaxial probe feed technique to excite DRAs 23

2.3 Coplanar waveguide feed technique to excite DRAs 24

2.4 Aperture coupling mechanism to excite DRAs 26

2.5 Modified shape of the DRAs 29

2.6 Modified feed geometries 31

2.7 Introducing an air gap between the DR and ground plane 33

2.8 Multi-segment DRAs 35

2.9 Attaching parasitic patch on the DRAs 37

2.10 Stacked DRAs 38

2.11 Embedded DRAs 40

2.12 Hybrid DRAs technique 42

2.13 Band rejection UWB antenna 50

3.1 Design specifications 57

3.2 Dielectric resonator specification 58

3.3 Substrate dimensions 59

4.1 Two-segment compact UWB DRA parameters 69

4.2 Compact UWB rectangular DRA dimensions 72

4.3 Compression of compact DRAs 80

4.4 Performances comparison between Two-Segment and

Rect-angular DRAs 80

5.1 Parameters of DRA with single band-notch 84

5.2 Dimensions of UWB DRA with dual band-notch 93

5.3 Performances comparison between Single and Dual

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LIST OF FIGURES

FIGURE NO. TITLE PAGE

2.1 Geometry of Lodge’s biconical antennas (1898). 9 2.2 Carter’s improved match biconical antenna configuration

(1939). 9

2.3 Lindenblad’s coaxial horn antenna configuration (1941). 9 2.4 Brillouin’s coaxial horn antenna configuration (1948). 10 2.5 Geometry of Stohrs ellipsoidal monople antenna (1968). 10

2.6 Geometry of Gibson’s vivaldi antenna (1979). 10

2.7 Various types of UWB antennas (a) planar monopole antenna, (b) printed monopole antenna, (c) printed wide-slot antenna,

and (d) dielectric resonator antenna. 11

2.8 Various shapes of dielectric resonator. 12

2.9 Hemispherical DRA excited by coaxial probe. 14

2.10 Geometry of the cylindrical DRA. 15

2.11 Geometry of the Rectangular DRA. 16

2.12 Electric and Magnetic Fields inside the Rectangular DRA for the T EX

δ11Mode. 18

2.13 Microstrip feed line mechanism (a) side coupling and (b)

direct coupling. 19

2.14 Probe coupling the DRA (a) RDRA (b) CDRA. 20

2.15 Coaxial probe feed. 22

2.16 Various shape of CPW for coupling to DRAs. 22

2.17 Dielectric image guide (DIG) for coupling to DRA. 25 2.18 Aperture coupling technique (a) various aperture slots (b)

embedded slot in the ground plane. 26

2.19 Prototype of inverted cup-shaped HDRA. 28

2.20 Schematic diagrams of Z-shaped DRA. 29

2.21 Geometry of dielectric ring resonator excited by L-shaped

microstrip feed line . 32

2.22 Photograph of the RDRA. 33

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2.24 Photograph of MSDRA with a single insert. 35 2.25 Geometry of the HDRA with a parasitic patch, excited by

aperture-coupled. 36

2.26 Geometry of the staked CDRA, excited by coaxial probe. 39 2.27 Cross section of the embedded DRA and top view of the

narrow slot board. 40

2.28 Geometry of DR-loaded monopole antenna. 41

2.29 Geometry of DR-loaded microstrip patch antenna. 41 2.30 Geometry of the UWB DRA with dual band rejections. 44 2.31 Geometry of the UWB DRA with band rejection using hybrid

technique. 44

2.32 Configuration of the UWB DRA reconfigurable band

rejection. 45

2.33 Prototype of the UWB DRA excited by elliptical patch with

dual band notched characteristics. 46

2.34 Geometry of the UWB DRA excited by microstrip feed line

with dual band notched characteristics. 46

2.35 Configuration of the UWB DRA with band rejection

characteristics. 47

2.36 Geometry of the UWB DRA with band rejection

characteris-tics. 48

2.37 Geometry of the band-notched UWB rectangular DRA. 48 2.38 Geometry of UWB DR-loaded monopole antenna with band

rejection. 49

3.1 The flowchart of research methodology. 55

3.2 Chamber room (a) antenna under testing (b) reference

antenna (c) schematic diagram. 60

4.1 Geometry of proposed DRA. 65

4.2 Effect of ground plane length Lgon reflection coefficient. 66

4.3 Simulated radiation efficiency of proposed DRA excited by

two different feed lines. 66

4.4 Effect of changing dimension Lcon reflection coefficient. 67

4.5 Effect of changing dimension Ldon reflection coefficient. 68

4.6 Photograph of the proposed DRA. 68

4.7 Measured and simulated reflection coefficient of proposed

DRA. 69

4.8 Simulated radiation efficiency and measured gain of proposed

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4.9 Measured and simulated radiation patterns. H-plane (right) and E-plane (left) at (a) 3.5 GHz, (b) 6 GHz, and (c) 8.5 GHz. Red and blue are measured and simulated results,

respectively. 71

4.10 Geometry of proposed RDRA: (a) front, (b) back, (c) side

view. 73

4.11 Effect of microstrip feed line width W2 on reflection

coefficient. 74

4.12 Reflection coefficient of proposed antenna; the antenna without DR and inserted and planar RDRA with and without

parasitic strip. 75

4.13 Reflection coefficient for various length of L4. 75

4.14 Reflection coefficient for various values of εd. 76

4.15 Prototype of the fabricated proposed RDRA. 77

4.16 Measured and simulated Reflection coefficient of proposed

RDRA. 77

4.17 Simulated radiation efficiency and gain of proposed RDRA. 78 4.18 Measured and simulated radiation patterns. H(xz)-plane (left)

and E(yz)-plane (right) at (a) 4 GHz, (b) 7 GHz, and (c) 10 GHz. Blue and red are measured and simulated results (dB),

respectively. 79

5.1 Geometry of inserted DRA without modified structure: (a)

front, (b) back, (c) side view. 83

5.2 Schematic diagram of DRA: (a) back view of planar DRA, (b) back view of inserted DRA with modified structure, (c)

side view of planar DRA. 83

5.3 Reflection coefficient for planar DRA with and without L-shaped strip and inserted DRA with and without metallic

sheet. 85

5.4 Reflection coefficient for various L6. 86

5.5 Reflection coefficient for various W6. 86

5.6 Reflection coefficient for various L4. 87

5.7 Current distribution at notched frequency (5.8 GHz) (a) front

view (b) back view. 87

5.8 Reflection coefficient for various length of Ln. 88

5.9 Prototype of the fabricated proposed DRA. 89

5.10 Measured and simulated reflection coefficient of proposed

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5.11 Simulated radiation efficiency and measured gain of proposed

DRA. 90

5.12 Measured and simulated radiation patterns. H(xz)-plane (right) and E(yz)-plane (left) at (a) 4 GHz, (b) 6.5 GHz, (c) 8 GHz and (d) 10.5 GHz. Blue and red are measured and

simulated results (dB), respectively. 91

5.13 Geometry of the proposed DRA; (a) front view, (b) back view,

(c) 3D view. 94

5.14 Evolution of the proposed UWB DRA with dual band rejections; (a) planar RDRA (front view), (b) inserted DRA with Stub. (c) inserted DRA with Inverted T-shaped on the back plane, (d) inserted DRA with inverted T-shaped on the back plane and slot on the ground plane, (e) planar RDRA

(3D view), and (f) proposed DRA (3D view). 95 5.15 Simulated reflection coefficient for planar and inserted RDRA

and modified DRA with and without stub. 96

5.16 Simulated reflection coefficient for various stub lengths (Lb)

with 1.4 mm stub width. 97

5.17 Simulated reflection coefficient for various stub widths (Wb)

with 11.5 mm stub length. 98

5.18 Simulated reflection coefficient for various lengths of Lt. 98

5.19 Simulated reflection coefficient for various lengths of Ls. 99

5.20 Simulated reflection coefficient for inserted DRA with stub

and inverted T-shaped strip, separately. 100 5.21 Simulated reflection coefficient for various lengths of Lb. 101

5.22 Simulated reflection coefficient for various lengths of Lt. 101

5.23 Current distribution at two notched frequencies (a) 3.45 GHz (b) 3.45 GHz (all transparent), (c) 5.52 GHz, (d) 5.4 GHz (all

transparent). 102

5.24 Prototype of the fabricated proposed DRA. 103

5.25 Measured and simulated reflection coefficient of proposed

DRA. 103

5.26 Simulated radiation efficiency and measured gain of proposed

DRA. 104

5.27 Measured far-field radiation patterns; H(xz)-plane (left) and E(yz)-plane (right) at (a) 3.1 GHz, (b) 6.5 GHz, and (c) 9.5 GHz. Red and blue are simulated and measured results (dB),

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LIST OF ABBREVIATIONS

AR – Axial Ratio

BW – Bandwidth

CDR – Cylindrical Dielectric Resonator

CDRA – Cylindrical Dielectric Resonator Antenna CRP – Circular Ring Patch

CPW – Co-Planar Waveguide

CST – Computer Simulation Software

dB – decibel

dBi – decibel (isotropic) DIG – Dielectric Image Guide

DR – Dielectric Resonator

DRA – Dielectric Resonator Antenna DWM – Dielectric Waveguide Model EDC – Effective Dielectric Constant

EM – Electromagnetic

ESCSRR – Elliptic Single Complementary Split-Ring Resonator FCC – Federal Communication Commission

FDTD – Finite Difference Time Domain FEM – Finite Element Method

FSS – Frequency Selective Surface

GHz – Giga Hertz

HCLR – Hollow-Cross-Loop Resonator HDR – Hemispherical Dielectric Resonator

HDRA – Hemispherical Dielectric Resonator Antenna HFSS – High Frequency Structural Simulator

Hz – Hertz

IDCLLR – Interdigital Capacitance Loading Loop Resonator IEEE – Institute of Electrical and Electronic Engineers

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mm – Millimeter

MoM – Method of Moment

MSDRA – Multi-Segment Dielectric Resonator Antenna MWM – Magnetic Waveguide Model

PCB – Printed Circuit Boards PIN – Positive-Intrinsic-Negative Q factor – Quality factor

RDR – Rectangular Dielectric Resonator

RDRA – Rectangular Dielectric Resonator Antenna

RF – Radio Frequency

RL – Return Loss

RSRR – Rectangular Split-Ring Resonator

SIR-DGS – Stepped Impedance Resonator-Defected Ground Structure SRR – Split-Ring Resonator

TE – Transverse Electric

TLM – Transmission Line Matrix

TM – Transverse Magnetic

TSDRA – Two-Segment Dielectric Resonator Antenna

UWB – Ultra-wideband

VSWR – Voltage Standing Wave Ratio

WiMAX – Worldwide Interoperability for Microwave Access WLAN – Wireless Local Area Network

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LIST OF SYMBOLS

fc – Center frequency

ε – Dielectric constant

εef f – Effective permittivity

E − plane – Electric plane

δ – Fraction of a half-of-field cycle variation

G – Gain of antenna

H − plane – Magnetic plane

≥ – More than

fn – Notched frequency

φ – Phi angle

λ – Wavelength

λn – wavelength at the notched resonant frequency

π – pi Γ – Reflection coefficient f0 – Resonant frequency c – Speed of light θ – Theta angle –

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LIST OF APPENDICES

APPENDIX TITLE PAGE

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INTRODUCTION

1.1 Background of the Study

The Ultra-Wideband (UWB) systems have developed intensely in the past two decades which are implemented for both academic and industrial communities of telecommunication applications. These antennas generally strive to be compatible the Federal Communications Commission (FCC) which support an impedance bandwidth of 7.5 GHz, i.e. from 3.1 GHz to 10.6 GHz in 2002 [1]. There are several advantages of UWB communications compare to other technologies which make them excellent candidate to present a further eloquent solution for wireless broadband applications as follow [2–6].

First of all, the UWB systems can obtain an immense capacity of several Gbps with a short range of 1 to 10 meters due to proportion of channel capacity to bandwidth. Secondly, the UWB facilitates an extremely reliable communication and secure solution due to possessing a spectral density in low power level, noise-like, which causes slightly electromagnetic interference with longer-range existing narrow-band systems. Thirdly, in UWB systems, a sufficient spatial resolution is achieved by applying a short duration impulse. This characteristic is used in target imaging to provide a potential capability to distinct targets from background clutter. Fourthly, since the UWB signals have short duration pulse waveforms, no multi-path cancellation will occurred because of passing the direct multi-path signal through the system before attaining the reflected path signal. Lastly, UWB systems compared to conventional radio systems have an intrinsic capability for integration in low

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complexity, low power, and low cost due to propagating without the requirement of an additional RF components which providing considerably short time domain pulse.

On the other hands, dielectric resonators (DRs) have been applied in the microwave circuits design such as oscillators and filters due to their high Q-factor characteristic. Moreover, it is found that the DRs with low dielectric constant can be used in antenna design as radiating element because of their low radiating Q-factor [7]. In the last two decades, dielectric resonator antennas (DRAs) have received agreeable consideration for UWB antennas due to remarkable characteristics such as different excitation mechanisms [8–11], high radiation efficiency [12], nearly constant gain [13, 14], and compact antenna size [15, 16]. The DRAs compared to microstrip patch antennas (MPAs)have wider impedance bandwidth because of having very small dielectric losses and lack of conductor losses, and also higher efficiency and less radiation pattern distortions due to lack of existing surface wave phenomena. In addition, DRAs compared with printed antenna provide small size ate expense of thickness due to decreasing the maximum path length in a certain direction to other directions.

1.2 Problem Statement

Based on investigation on ultra-wideband DR antenna, the researchers encountered some difficulties. One of the main challenges is obtaining wide impedance bandwidth more than around 91% with high radiation efficiency more than 90% while sustaining compact size. For example, the DRA impedance bandwidth is mostly below 10% for a single-mode excitation, which is not sufficient for UWB applications. On the other hands, existing electromagnetic interference of some narrow bands system such as wireless local area network (WLAN) and worldwide interoperability for microwave access (WiMAX) is a serious problem for UWB application systems. Some design techniques have been developed for the band rejection UWB DRA antenna. However, most of these approaches suffer from increasing size of antenna and lack of the

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flexibility and separately of each band rejection with control the width of the band-notch across the stop-band.

1.3 Research Objective

The objectives of this work focus on simulate and fabricate of a novel UWB DRA which are :

i. Design of compact UWB DRA with high radiation efficiency while sustaining wide bandwidth over whole desired frequencies.

ii. Design of UWB DRA with sufficient band rejection for existing electromagnetic interference of nearby wireless communication systems such as WiMAX (3.3-3.8 GHz) and WLAN (5.15-5.825 GHz).

1.4 Scopes of Project

This work focuses on the design of the UWB DRA which operates within the frequency range from 3.1 GHz to 10.6 GHz. The development of the UWB DRA is comprised by avoiding the electromagnetic interference of nearby narrow band systems such as the worldwide interoperability for microwave access (WiMAX) system operating at 3.3-3.8 GHz and wireless local area network (WLAN) system operating at 5.15-5.85 GHz.

The rectangular DR with dielectric constant less than 15 is used to achieve wide impedance bandwidth. The compact UWB DRAs is simulated and verified by CST and HFSS in terms of return loss, gain, efficiency, and radiation pattern to improve its performance. A parametric study of the different design of UWB DRAs was carried out. The UWB DRA is optimized and fabricated with good agreement between the measured results with simulated results.

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1.5 Contribution of the Research

For this work, four contributions are introduced which include:

i. Design of a new compact two-segment Z-shaped DRA with different permittivity excited by a U-shaped feed-line for ultra-wideband application that the combination mechanism of the U-shaped feed-line and two-segments DR (TSDR) characteristics provide firm omnidirectional radiation pattern and high radiation efficiency with compact size while sustaining wide impedance bandwidth.

ii. Design of a new simple compact rectangular dielectric resonator antenna (RDRA) for ultra-wideband application that by applying a combination of simple parasitic strip connected to the ground plane, microstrip feed line and inserted RDR characteristic, a compact antenna size with a wide impedance bandwidth, high radiation efficiency, nearly constant gain and consistent omnidirectional radiation pattern over desired frequency range are achieved. iii. Design of a new compact DRA with band rejection of 5.71-6.32 GHz (upper

WLAN band) using a modified metallic sheet for ultra-wideband application that the combination mechanism of L-Shape strip connected to the ground plane, proper position of microstrip feed line, inserted DR characteristic, and metallic sheet underneath DR provide a wide impedance bandwidth and compact antenna with consistent omnidirectional radiation pattern.

iv. Design of a new compact UWB DRA with dual band rejection of 3.22-4.06 GHz (WiMAX) and 4.84-5.96 GHz (WLAN) that by intently implementing a combination mechanism of two inserted identical DRs, U-shaped excitation performance, stub, inverted T-shaped parasitic strip, and slot in the ground plane, ultra wideband characteristic with efficient dual band-notched and miniature size of about 0.124λ × 0.31λ × 0.062λ at 3.1 GHz are achieved simultaneously.

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1.6 Signification of the Research

Dielectric resonator antennas would be chosen by more system engineers when designing their wireless products due to possessing their considerable characteristics, flexibility in design and easily available commercially at very low cost. Therefore, DRAs have proved themselves to be ideal candidates for UWB antenna applications such as local and personal area networks (LAN/PAN), roadside info-station, short range radios and military communications.

1.7 Thesis Outlines

This thesis is organized in six chapters, which each chapter will describe on the different aspects of the work. The outlines of the dissertation for each 6 chapter are organized as follows.

Chapter 1 introduces an introduction of UWB system and a brief history about the dielectric resonator antenna and also makes some view about the problem statements, objective, and scope of this work.

Chapter 2 describes most prevalently used shapes of DRA and focuses on surveys of coupling mechanisms, bandwidth enhancement techniques, and compact techniques of DRAs through the literature to obtain some idea and achieve proper design.

Chapter 3 focuses on the methodology of project and steps of design. Moreover, the steps of the fabrication process and measurement procedure are illustrated.

Chapter 4 depicts simulated and measured results of an ultra-wideband dielectric resonator antenna design. Discussions about comparisons between simulated and measured result through the diagram are illustrated.

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Chapter 5 demonstrates a design of ultra-wideband dielectric resonator antenna with WiMAX/WLAN band rejections. Parametric studies and discussions with experimental results are illustrated.

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