
FDTD Modeling of Metamaterials
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Content
- FDTD Modeling of Metamaterials: Theory and Applications
- Contents
- Preface
- Acknowledgments
- Chapter 1: Introduction
- 1.1 What Are Electromagnetic Metamaterials?
- 1.2 A Historical Overview of Electromagntic Metamaterials
- 1.2.1 Artificial Dielectrics
- 1.2.2 Artificial Magnetic Materials
- 1.2.3 Bianisotropic Composites
- 1.2.4 Double-Negative and Indefinite Media
- 1.2.5 Photonic and Electromagnetic Crystals
- 1.3 Numerical Modeling of Electromagnetic Metamaterials
- 1.4 Layout of the Book
- References
- Chapter 2: Fundamentals and Applications of Electromagnetic Bandgap Structures
- 2.1 Introduction
- 2.2 Bloch's Theorem and the Dispersion Diagram
- 2.2.1 Translational Symmetry
- 2.2.2 Bloch's Theorem and Periodic Boundary Condition (PBC)
- 2.2.3 Brillouin Zone
- 2.2.4 Dispersion Diagram and EBG
- 2.3 An Overview of Numerical Methods for Modeling EBG Structures
- 2.3.1 The Generalized Rayleigh's Identity Method and the Korringa-Kohn-Rostoker (KKR) Method
- 2.3.2 Plane-Wave Expansion Method
- 2.3.3 The Transfer-Matrix Method
- 2.3.4 The Finite-Difference Time-Domain (FDTD) Method
- 2.4 An Overview of EBG Applications
- 2.4.1 In-Phase Reflection
- 2.4.2 Suppression of Surface Waves
- 2.4.3 EBGs Operating in Defect Modes
- 2.4.4 Subwavelength Imaging from the Passband of the EBGs
- 2.5 Summary
- References
- Chapter 3: A Brief Introduction to the FDTD Method for Modeling Metamaterials
- 3.1 Introduction
- 3.2 Formulations of the Yee's FDTD Algorithm
- 3.2.1 Maxwell's Equations
- 3.2.2 Yee's Orthogonal Mesh
- 3.2.3 Time Domain Discretization: The Leapfrog Scheme and the CourantStability Condition (CFL Condition)
- 3.3 Other Spatial Domain Discretization Schemes
- 3.3.1 Subgridding Mesh
- 3.3.2 Nonorthogonal Mesh
- 3.3.3 Hybrid FDTD Meshes
- 3.4 Boundary Conditions
- 3.4.1 Mur's Absorbing Boundary Conditions (ABCs)
- 3.4.2 Perfect Matched Layers (PMLs)
- 3.4.3 Periodic Boundary Condition (PBC)
- 3.5 Bandgap Calculation
- 3.5.1 Source Excitation
- 3.5.2 Dispersion Diagram Calculation
- 3.5.3 Transmission and Reflection Coefficient Calculation
- 3.6 Summary
- References
- Chapter 4: FDTD Modeling of EBGs and Their Applications
- 4.1 Introduction
- 4.2 FDTD Modeling of Infinite Electromagnetic Bandgap Structures
- 4.2.1 Physical Model of EBG Structures
- 4.2.2 Mesh Generation and Simulation Parameters in FDTD Modeling
- 4.2.3 Simulation Results of Infinite EBGs Using the Conformal and Yee's FDTD
- 4.3 Conformal FDTD Modeling of (Semi-)Finite EBG Structures
- 4.3.1 FDTD Model and Simulation Results
- 4.4 Design and Modeling of Millimeter-Wave EBG Antennas
- 4.4.1 Introduction
- 4.4.2 Design and Modeling of Woodpile EBG
- 4.4.3 A Millimeter-Wave EBG Antenna Based on a Woodpile Structure
- 4.4.4 Experimental Results
- 4.5 Conclusions
- References
- Chapter 5: Left-Handed Metamaterials (LHMs)and Their Applications
- 5.1 Introduction
- 5.2 Effective Medium Theory and Left-Handed Metamaterials
- 5.2.1 A Composite Medium of Metallic Wires and Split Ring Resonators
- 5.2.2 Isotropic Three-Dimensional Left-Handed Metamaterials
- 5.2.3 Left-Handed Metamaterials Using Simple Short Wire Pairs
- 5.3 Applications of Left-Handed Metamaterials
- 5.3.1 Imaging by a Perfect LHM Lens
- 5.3.2 Transmission Line Structures of Left-Handed Metamaterials
- 5.3.3 Directive Electromagnetic Scattering by an Infinite Conducting CylinderCoated with LHMs
- 5.3.4 Negative Index Materials (NIM) for Selective Angular Separation ofMicrowave by Polarization
- References
- Chapter 6: Numerical Modeling of Left-Handed Material (LHM) Using a Dispersive FDTD Method
- 6.1 Introduction
- 6.2 The Effective Medium of Left-Handed Materials (LHMs)
- 6.3 Modeling of Left-Handed Metamaterials Using a Dispersive FDTD Method
- 6.3.1 Two-Dimensional Dispersive FDTD with Auxiliary Differential Equations(ADEs)
- 6.3.2 Phase Compensation Through Layered LHM Structures
- 6.3.3 Conjugate Dielectric and Metamaterial Slab as Radomes
- 6.3.4 Numerical Results
- 6.4 Conclusions
- References
- Chapter 7: FDTD Modeling and Figure-of-Merit(FOM) Analysis of Practical Metamaterials
- 7.1 Introduction
- 7.2 EM Response of the Infinite, Doubly Periodic DNG Slab with Plane Wave Illumination
- 7.2.1 Model Description of the Array Comprising of Split-Ring Resonators and Wires
- 7.2.2 Scattering Parameters Measurements Obtained from the PBC/FDTD Code
- 7.2.3 Phase Data Inside the DNG Slab
- 7.3 Retrieval of Effective Material Constitutive Parameters Using the Inversion Approach
- 7.3.1 Review of the Inversion Approach
- 7.3.2 Retrieval of the Effective Material Parameters from the Numerical S-Parameters Obtained from FDTD Simulations of Metamaterials
- 7.3.3 Summary of the Difficulties Encountered Using the Inversion Approachfor Effective Medium Characterization
- 7.4 EM Response of a Finite Artificial-DNG Slab with Localized Beam Illumination
- 7.4.1 Slab with Localized Beam Illumination
- 7.4.2 FDTD Model
- 7.4.3 Total Transmission and Reflection Power UnderGaussian Beam Illumination
- 7.4.4 EM Response of the Artificial-DNG Slab at Normal Incidence with Ey Polarization
- 7.4.5 EM Response of the Artificial-DNG Slab at Oblique TMz IncidenceComing from (q = 150?, f = 90?) with Hx Polarization
- 7.4.6 EM Response of the Artificial-DNG Slab at Oblique TEz Incidence Comingfromq = 150?, f = 0? with Ey Polarization
- 7.4.7 EM Response of a Finite Artificial-DNG Slab Excited by Small Dipole
- 7.5 Figure-of-Merit (FOM) Analysis
- 7.5.1 Loss and Bandwidth of Metamaterials with Different Electrical Sizes and Particle Densities
- 7.5.2 Figure-of-Merit Analysis by Numerical Experiments
- 7.6 Conclusions
- References
- Chapter 8: Accurate FDTD Modeling of a Perfect Lens
- 8.1 Introduction
- 8.2 Dispersive FDTD Modeling of LHMs with Spatial Averaging at the Boundaries
- 8.2.1 The (E, D, H, B) Scheme
- 8.2.2 The (E, J, H, M) Scheme
- 8.2.3 The Spatial Averaging Methods
- 8.3 Numerical Implementation
- 8.4 Effects of Material Parameters on the Accuracy of Numerical Simulation
- 8.5 Effects of Switching Time
- 8.6 Effects of Transverse Dimensions on Image Quality
- 8.7 Modeling of Subwavelength Imaging
- 8.8 Conclusions
- References
- Chapter 9: Spatially Dispersive FDTD Modelingof Wire Medium
- 9.1 Introduction
- 9.2 Spatial Dispersion in the Wire Medium
- 9.3 Spatially Dispersive FDTD Formulations
- 9.4 Stability and Numerical Dispersion Analysis
- 9.5 Perfectly Matched Layer for Wire Medium Slabs
- 9.6 Numerical Thickness of Wire Medium Slabs
- 9.7 Two-Dimensional FDTD Simulations
- 9.8 Three-Dimensional FDTD Simulations
- 9.9 Experimental Verifications
- 9.10 Internal Imaging by Wire Medium Slabs
- 9.11 Conclusions
- References
- Chapter 10: FDTD Modeling of Metamaterialsfor Optics
- 10.1 Introduction
- 10.2 Dispersive FDTD Modeling of Silver-Dielectric Layered Structuresfor Subwavelength Imaging
- 10.2.1 Introduction
- 10.2.2 FDTD Modeling of the Silver-Dielectric Layered Structure
- 10.2.3 Numerical Results and Discussions
- 10.3 A Metamaterial Scanning Near-Field Optical Microscope
- 10.3.1 Introduction
- 10.3.2 Theory
- 10.3.3 Simulation
- 10.4 FDTD Study of Guided Modes in Nanoplasmonic Waveguides
- 10.4.1 Conformal Dispersive FDTD Method Using Effective Permittivities (EPs)
- 10.5 FDTD Calculation of Dispersion Diagrams
- 10.5.1 Wave Propagation in Plasmonic Waveguides Formed by Finite Numberof Elements
- 10.6 FDTD Modeling of Electromagnetic Cloaking Structures
- 10.6.1 Dispersive FDTD Modeling of the Cloaking Structure
- 10.6.2 Numerical Results and Discussion
- References
- Chapter 11: Overviews and Final Remarks
- 11.1 Introduction
- 11.2 Overview of Advantages and Disadvantages of the FDTDMethod in Modeling Metamaterials
- 11.3 Overview of Metamaterial Applications and Final Remarks
- 11.3.1 Small Antennas Enclosed by an ENG Shell
- 11.3.2 Focusing and Superlensing Effects
- 11.3.3 Performance Enhancement of Planar Antennas
- 11.3.4 Electromagnetic Cloaks
- References
- List of Abbreviations
- About the Authors
- Index
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