
Microwave Materials and Applications, 2 Volume Set
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VOLUME I
List of Contributors xv
Series Preface xvii
Preface xix
1. Measurement of Microwave Dielectric Properties and Factors Affecting Them 1
M.T. Sebastian, M.A.S. Silva, and A.S.B. Sombra
1.1 Introduction 1
1.2 Permittivity (;;r) and quality factor (Q) 2
1.3 Measurement of Microwave Dielectric Properties 7
1.4 Methods of Measurement 8
1.5 Measurement of EMI Shielding Effectiveness 29
1.6 Terahertz and Millimeter Wave Measurements 31
1.7 Measurement of Dielectric Properties of Powder Samples 34
1.8 Estimation of Dielectric Loss by Spectroscopic Methods 35
1.9 Factors Affecting Dielectric Loss 39
1.10 Measurement of Temperature Coefficient of Resonant Frequency 41
1.11 Tuning of the Resonant Frequency 42
References 45
2. Modeling of Microwave Dielectric Properties of Composites 53
Marko Tuhkala, Merja Teirikangas, and Jari Juuti
2.1 Introduction 53
2.2 Connectivity 54
2.3 Electrostatic Theory 56
2.4 Mixing Equations 59
2.5 Effect of Porosity 71
2.6 Conclusion 77
References 77
3. Perovskites 81
K.P. Surendran and Rick Ubic
3.1 Introduction 81
3.2 Lattice Constant Prediction 83
3.3 Tolerance Factor 84
3.4 Octahedral Tilting 86
3.5 Simple Perovskites 87
3.6 Cation Ordering 89
3.7 Cation Deficient Perovskites 133
3.8 Summary 135
References 136
4. High Permittivity Materials 149
Rick Ubic, G. Subodh, and M.T. Sebastian
4.1 Introduction 149
4.2 The BaO-Ln2O3-TiO2 System 149
4.3 The Effect of Processing Parameters on Electrical Properties 162
4.4 Titania 164
4.5 Sr1-3x/2CexTiO3 Ceramics 166
4.6 Pbn(Nb1-xTax)O5+n 174
4.7 (Pb1-xCax)(Fe1/2B1/2)O3 [B = Nb, Ta] 185
4.8 Ag(Nb1-xTax)O3 187
4.9 Summary 190
References 190
5. Millimeter-Wave Materials 203
Hitoshi Ohsato
5.1 Introduction: New Frontiers of Millimeter-Wave Dielectrics 203
5.2 Dielectric Properties for Millimeter Wave 207
5.3 Candidates of Millimeter-Wave Dielectrics 209
5.4 Specialized Study 212
Acknowledgments 259
References 259
6. Other Important Materials 267
M.T. Sebastian and R.C. Pullar
6.1 Spinel 267
6.2 Li2ATi3O8 (A = Mg, Zn) Ceramics 280
6.3 Li2Zn3Ti4O12 289
6.4 Apatites 290
6.5 Alumina 303
6.6 Zirconium Tin Titanate 306
6.7 Dielectric Materials in the BaO-TiO2 System 314
6.8 Columbite Niobates (M2+Nb2O6) 318
Acknowledgments 327
References 328
7. Microwave Dielectric Properties of Glasses and Bulk Glass Ceramics 345
Martin Letz
7.1 Glasses 345
7.2 Bulk Glass Ceramics 349
References 353
8. High Temperature Cofired Ceramic (HTCC), Low Temperature Cofired Ceramic (LTCC), and Ultralow Temperature Cofired Ceramic (ULTCC) Materials 355
M.T. Sebastian and Heli Jantunen
8.1 High Temperature Cofired Ceramics (HTCC) 355
8.2 HTCC Alumina 357
8.3 Aluminium Nitride HTCC 359
8.4 ZrSiO4 361
8.5 Low Temperature Cofired Ceramics (LTCC) 366
8.6 Ultralow Temperature Cofired Ceramics (ULTCC) 395
8.7 Discussion and Conclusion 408
References 411
Index i1
VOLUME II
List of Contributors xv
Series Preface xvii
Preface xix
9. Voltage Tunable Microwave Dielectrics for Frequency and Phase Agile Devices 427
K. Sudheendran and K.C. James Raju
9.1 Introduction to Voltage Tunable Materials 427
9.2 Different Classes of Voltage Tunable Materials 428
9.3 Importance of Voltage Tunable Materials in Frequency and Phase Agile Devices 432
9.4 Growth Techniques for Voltage Tunable Thin Films on Various Substrates 434
9.5 Characterization techniques 437
9.6 High-Frequency Characterization 438
9.7 Design and Realization Aspects of Varactors Using Tunable Materials 449
9.8 Conclusions 454
Acknowledgment 454
References 454
10. Dielectric Inks 457
J. Varghese and M.T. Sebastian
10.1 Introduction 457
10.2 Methodology 461
10.3 Dielectric Inks and Their Properties 462
10.4 Polymer-Based Dielectric Inks, Properties and Applications 473
10.5 Commercially Available Dielectric Inks, Properties and Applications 475
10.6 Conclusion 475
Acknowledgment 477
References 477
11. Polymer-Ceramic Composites for Microwave Applications 481
R. Ratheesh and M.T. Sebastian
11.1 Introduction: Microwave Substrates 481
11.2 Types of Polymer-Ceramic Composites 483
11.3 Thermoplastic Matrix and Composites 485
11.4 PTFE/Ceramic Composites 489
11.5 Polyethylene-Ceramic Composites 502
11.6 Polystyrene-Ceramic Composites 507
11.7 Epoxy-Ceramic Composites 510
11.8 Liquid Crystal Polymer (LCP) 513
11.9 Thermal Conductivity 514
11.10 Polymer Nanoceramic Composites 518
11.11 Ultrawideband Antenna Design Using Copper Cladded Ceramic-Filled PTFE Substrates 521
11.12 Conclusion 526
References 527
12. Rubber-Ceramic Composites 537
M.T. Sebastian and L.K. Namitha
12.1 Introduction 537
12.2 Silicone Rubber 539
12.3 Butyl Rubber (BR) 553
12.4 Fabrication of Flexible Microstrip Antenna 567
12.5 Conclusions 570
References 570
13. Designing of Materials for EMI Shielding Applications 575
Swati Varshney and S.K. Dhawan
13.1 Electromagnetic Shielding and Microwave Absorption Mechanism 577
13.2 Shielding Effectiveness (SE) 577
13.3 Measurement of Shielding Effectiveness 578
13.4 Electromagnetic Shielding Materials 581
13.5 New Insight into Designing of Materials for Microwave Shielding 583
13.6 Nanostructured Graphene/Fe3O4 Incorporated Polyaniline for EMI Shielding 584
13.7 Designing of Polypyrrole-;;-Fe2O3 Nanocomposite Wave Absorber 586
13.8 Designing of Conducting Polymer Composite by Incorporating Ferrofluid 590
13.9 Designing of Polypyrrole-Aqueous Ferrofluid (PFF) Nanocomposite Microwave Absorber 593
13.10 Conclusions 596
Acknowledgments 598
References 598
14. Microwave Ferrites and Applications 603
Vincent G. Harris
14.1 Introduction 603
14.2 Structure, chemistry, magnetism, and gyromagnetic properties 604
14.3 Ferrite Materials Processing for Microwave Applications 611
14.4 Semiconductor Integration of Ferrite Thin and Thick Films for MIC Development 620
14.5 Ferrite-Based Microwave Device Development 628
14.6 Outlook 642
References 643
15. Applications of Microwave Dielectrics 653
Heike Bartsch, Alexander Schulz, Jens M¿uller, Alexander Ebert, Steffen Spira, Frank Wollenschl¿ager, and Matthias Hein
15.1 General Requirements for Microwave Applications 653
15.2 LTCC Microwave Components and Materials 654
15.3 LTCC Application Examples 666
References 676
16. Applications of Dielectric Resonators 683
P. Mohanan and S. Mridula
16.1 Introduction 683
16.2 Dielectric Resonator Antenna (DRA) 684
16.3 Applications of Dielectric Resonator in Microwave Oscillators 698
16.4 Application of Dielectric Resonators in Microwave Filters 703
References 710
Appendix: List of Low-Loss Ceramic Dielectric Materials and Their Properties 715
M.T. Sebastian
Index i1
Preface
A large number of papers continue to be published in the area of microwave materials and applications; however, there have hitherto been no books in the open literature that treat the different types of microwave materials, such as low-loss dielectric ceramics, glass ceramics, polymer- and elastomer-based composites, cofired ceramics, electromagnetic interference (EMI) shielding materials, tunable dielectrics, dielectric inks, or microwave ferrites. Our purpose here is to provide a comprehensive and self-consistent volume whereby the aforementioned lack of a reference book in the open literature can be remedied.
Microwave dielectric materials play a key role in global society, with a wide range of applications straddling terrestrial and satellite communications, including Internet of Things (IoT), software radio, GPS, DBS TV, environmental monitoring via satellite, etc. The mobile phone is one of the most widely spread technologies on the planet. In many countries the number of mobile subscriptions exceeds the population. The IoT is posed to make an explosive growth in the near future. In this paradigm, many everyday objects will be networked via radio-frequency identification (RFID), printed electronics, and sensor network technologies. Fifth generation (5G) mobile networks or wireless systems represent the next major phase of mobile telecommunication standards beyond the current 4G/IMT-Advanced standards. In addition to providing greater speeds, 5G networks will also need to meet the needs of new uses, such as the IoT as well as broadcast-like services and lifeline communications for times of natural disaster. According to GSMA Intelligence, the revenue for mobile network operators from interconnected devices in the segments of automotive, health, utilities, and consumer electronics will be $1.3 trillion by 2020. The worldwide data volume in mobile communication systems doubles nearly every year. To address this challenge, higher frequency bands will be used for which broadband and multiband equipment is required. The new standard Long Term Evolution (LTE-A) and the standardization process for 5G mobile communications necessitates changes in the technology of antennas and filters. In order to meet the specifications of future systems, new designs and improved or new microwave dielectric components are required. The recent progress in the IoT, microwave telecommunications, satellite broadcasting, and intelligent transport systems (ITSs) has resulted in an increasing demand for low-loss dielectric materials, tunable dielectrics, microwave ferrites, and EMI shielding materials. Low-loss dielectric oxide ceramics have revolutionized the microwave wireless communication industry by reducing the size and cost of filter, oscillator, and antenna components in applications ranging from cellular phones to the IoT. Wireless communication technology demands materials with highly specialized properties. Recently the demand for materials with low sintering temperatures has increased not only to lower the energy cost of devices but also to integrate with polymers and silver-based electrodes. Several polymer-based (polymer-ceramic) composites have also recently been developed for wireless communication technology.
A dielectric resonator is an electromagnetic component that exhibits resonance for a narrow range of frequencies. The resonance is similar to that of a circular hollow metallic waveguide except that the boundary is defined by a large change in permittivity rather than by a conductor. Dielectric resonators (DRs) generally consist of a puck of ceramic that has a high permittivity and a low dissipation factor (tan d). The resonant frequency is determined by the overall physical dimensions of the puck, the permittivity of the material, and its immediate surroundings. The key properties required for a dielectric resonator are high quality factor (Q ~ 1/tan d), high relative permittivity (?r), and near-zero temperature coefficient of resonant frequency (tf). The first chapter describes the different techniques for measuring the microwave properties of materials. Chapter 2 discusses the modeling of relative permittivity of composites using different mixing rules. Developing dielectric resonator materials in which these three properties are simultaneously optimized is difficult. Low-permittivity ceramics are used for millimeter-wave communications and also as substrates for microwave integrated circuits. The medium permittivity ceramics with ?r in the range 25-50 are used for satellite communication and in cell phone base stations. High-?r materials are used in mobile phones where miniaturization of components is very important. For millimeter-wave applications, temperature-stable, low-permittivity, and high-Q (low-loss) substrates are required for high-speed signal transmission with minimum attenuation. Chapters 3 to 6 describes such materials.
The term dielectric resonator (DR) first appeared in 1939 when Richtmeyer showed that a suitably shaped dielectric piece can function as a microwave resonator; however, it took more than 20 years to generate further interest in DRs and to verify Richtmeyer's prediction experimentally. In the early 1960s Okaya and Barash rediscovered DRs while working on rutile single crystals. They measured the permittivity and Q of TiO2 single crystals at room temperature down to 50 K in the microwave frequency range using the commensurate transmission line technique. In the early 1960s Cohn and his co-workers performed extensive theoretical and experimental work on DRs. Rutile ceramics that had an isotropic permittivity of about 100 were used for their experiments, but TiO2 has a poor (+450 ppm/oC) resonant frequency stability that prevented its commercial exploitation. The first microwave filter using TiO2 ceramics was proposed by Cohen in 1968, but this filter was not useful for practical applications because of its high ?r and frequency instability with temperature. A real breakthrough in dielectric resonator ceramic technology occurred in the early 1970s when the first temperature-stable low-loss barium tetratitanate (BaTi4O9) ceramics were developed by the Raytheon Company. Later, barium nanotitanate (Ba2Ti9O20) with improved performance was reported by Bell Laboratories. The next breakthrough came from Japan when Murata Manufacturing Company produced (Zr, Sn)TiO4 ceramics. Commercial production of dielectric resonators started in the early 1980s.
In the last two decades there has been extensive progress in the development of terahertz (THz) technology. This progress has enabled a multitude of potential applications, be it communications, biomedical, imaging, security, quality control of food and agricultural products, matter and light control, or chemical agent detection - in every application it has emerged as one of the most promising areas of interest. The terahertz region of the electromagnetic spectrum, referring roughly to the frequencies from 100 GHz or 0.1 THz to 30 THz, is the bridge between the microwave and infrared spectral bands. The promise of THz radiation resides in its unique properties and characteristics: its non-ionizing nature; its submillimeter spatial resolution; its transmission through dielectric materials that are transparent to it; its interaction with water molecules, making it useful for certain medical diagnoses; its unique signature for molecular and rotational energy levels of many biological and chemical agents; and its potential for wireless communications. Although a large number of materials have been characterized in the microwave frequency range, relatively little attention has been paid to millimeter-wave or terahertz characterization of materials, possibly due to the relatively expensive facilities required. Chapter 5 discusses mm-wave material systems and applications of this technology.
Glasses have good thermal properties compared to polymers and better material homogeneity in comparison to ceramics, and hence they are considered for microwave applications; however, glasses in general have higher dielectric losses and a limited range of dielectric constants. Glass-ceramic composites have the advantage of an increased range of dielectric constants and reduced losses. They can be made with excellent homogeneity to produce sophisticated miniaturized microwave electronic devices. Chapter 7 discusses microwave dielectric properties of important glasses and glass-ceramics.
In the past, microwave devices have been traditionally machined from metal, and coaxial RF connections were made with metallic connectors, generally leading to expensive, heavy, and bulky packages. Moreover, today's electronic circuits for the automotive industry, entertainment electronics, and telecommunications have to handle a steadily increasing level of functionality whilst occupying the smallest volume possible. In the development of complex miniaturized circuits, flexible glass/ceramic or ceramic tapes with sintering aids made of high-temperature cofired ceramics (HTCCs), low-temperature cofired ceramics (LTCCs), and ultralow-temperature cofired ceramics (ULTCCs) play a decisive role as base materials. The choice of HTCC, LTCC, or ULTCC tapes is based on the electrode materials used and cofiring temperature. Cofired ceramics have become crucial in the development of various modules and substrates. In this technology, several thin layers of low-permittivity...
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