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Summary
Summary
This extensively revised and expanded third edition of the Artech House bestseller, Computational Electrodynamics: The Finite-Difference Time-Domain Method, offers engineers the most up-to-date and definitive resource on this critical method for solving Maxwell's equations. The method helps practitioners design antennas, wireless communications devices, high-speed digital and microwave circuits, and integrated optical devices with unsurpassed efficiency. There has been considerable advancement in FDTD computational technology over the past few years, and the third edition brings professionals the very latest details with entirely new chapters on important techniques, major updates on key topics, and new discussions on emerging areas such as nanophotonics. What's more, to supplement the third edition, the authors have created a Web site with solutions to problems, downloadable graphics and videos, and updates,
Author Notes
Allen Taflove is a professor of electrical and computer engineering at Northwestern University, Evanston, IL. He is also the author of Computational Electrodynamics: The Finite-Difference Time-Domain Method (Artech House 1995).
050
Table of Contents
Preface to the Second Edition | p. xvii |
Preface to the First Edition | p. xxi |
1 Electrodynamics Entering the 21st Century | p. 1 |
1.1 Introduction | p. 1 |
1.2 The Heritage of Military Defense Applications | p. 2 |
1.3 Frequency-Domain Solution Techniques | p. 3 |
1.4 Rise of Finite-Difference Time-Domain Methods | p. 3 |
1.5 History of FDTD Techniques for Maxwell's Equations | p. 5 |
1.6 Characteristics of FDTD and Related Space-Grid Time-Domain Techniques | p. 7 |
1.6.1 Classes of Algorithms | p. 7 |
1.6.2 Predictive Dynamic Range | p. 17 |
1.6.3 Scaling to Very Large Problem Sizes | p. 18 |
1.7 Examples of Applications (including Color Plate Section, pages 9-16) | p. 19 |
1.7.1 Radar-Guided Missile | p. 20 |
1.7.2 High-Speed Computer Circuit-Board Module | p. 21 |
1.7.3 Power-Distribution System for a High-Speed Computer Multichip Module | p. 22 |
1.7.4 Microwave Amplifier | p. 23 |
1.7.5 Cellular Telephone | p. 24 |
1.7.6 Optical Microdisk Resonator | p. 25 |
1.7.7 Photonic Bandgap Microcavity Laser | p. 27 |
1.7.8 Colliding Spatial Solitons | p. 28 |
1.8 Conclusions | p. 29 |
References | p. 30 |
2 The One-Dimensional Scalar Wave Equation | p. 35 |
2.1 Introduction | p. 35 |
2.2 Propagating-Wave Solutions | p. 35 |
2.3 Dispersion Relation | p. 36 |
2.4 Finite Differences | p. 38 |
2.5 Finite-Difference Approximation of the Scalar Wave Equation | p. 39 |
2.6 Numerical Dispersion Relation | p. 42 |
2.6.1 Case 1: Very Fine Sampling in Time and Space ([Delta]t [right arrow] 0, [Delta]x [right arrow] 0) | p. 43 |
2.6.2 Case 2: Magic Time-Step (c[Delta]t = [Delta]x) | p. 43 |
2.6.3 Case 3: Dispersive Wave Propagation | p. 44 |
2.6.4 Example of Calculation of Numerical Phase Velocity and Attenuation | p. 49 |
2.6.5 Examples of Calculations of Pulse Propagation | p. 51 |
2.7 Numerical Stability | p. 55 |
2.7.1 Complex-Frequency Analysis | p. 55 |
2.7.2 Examples of Calculations Involving Numerical Instability | p. 59 |
2.8 Summary | p. 61 |
Appendix 2A Order of Accuracy | p. 63 |
2A.1 Lax-Richtmyer Equivalence Theorem | p. 63 |
2A.2 Limitations | p. 64 |
References | p. 64 |
Bibliography on Stability of Finite-Difference Methods | p. 65 |
Problems | p. 65 |
3 Introduction to Maxwell's Equations and the Yee Algorithm | p. 67 |
3.1 Introduction | p. 67 |
3.2 Maxwell's Equations in Three Dimensions | p. 67 |
3.3 Reduction to Two Dimensions | p. 70 |
3.3.1 TM[subscript z] Mode | p. 71 |
3.3.2 TE[subscript z] Mode | p. 71 |
3.4 Reduction to One Dimension | p. 72 |
3.4.1 x-Directed, z-Polarized TEM Mode | p. 72 |
3.4.2 x-Directed, y-Polarized TEM Mode | p. 73 |
3.5 Equivalence to the Wave Equation in One Dimension | p. 74 |
3.6 The Yee Algorithm | p. 75 |
3.6.1 Basic Ideas | p. 75 |
3.6.2 Finite Differences and Notation | p. 77 |
3.6.3 Finite-Difference Expressions for Maxwell's Equations in Three Dimensions | p. 80 |
3.6.4 Space Region With a Continuous Variation of Material Properties | p. 85 |
3.6.5 Space Region With a Finite Number of Distinct Media | p. 87 |
3.6.6 Space Region With Nonpermeable Media | p. 89 |
3.6.7 Reduction to the Two-Dimensional TM[subscript z] and TE[subscript z] Modes | p. 91 |
3.6.8 Interpretation as Faraday's and Ampere's Laws in Integral Form | p. 93 |
3.6.9 Divergence-Free Nature | p. 96 |
3.7 Alternative Finite-Difference Grids | p. 98 |
3.7.1 Cartesian Grids | p. 99 |
3.7.2 Hexagonal Girds | p. 101 |
3.7.3 Tetradecahedron/Dual-Tetrahedron Mesh in Three Dimensions | p. 104 |
3.8 Summary | p. 105 |
References | p. 106 |
Problems | p. 106 |
4 Numerical Dispersion and Stability | p. 109 |
4.1 Introduction | p. 109 |
4.2 Derivation of the Numerical Dispersion Relation for Two-Dimensional Wave Propagation | p. 110 |
4.3 Extension to Three Dimensions | p. 112 |
4.4 Comparison With the Ideal Dispersion Case | p. 113 |
4.5 Anisotropy of the Numerical Phase Velocity | p. 114 |
4.5.1 Sample Values of Numerical Phase Velocity | p. 114 |
4.5.2 Intrinsic Grid Velocity Anisotropy | p. 120 |
4.6 Complex-Valued Numerical Wavenumbers | p. 124 |
4.6.1 Case 1: Numerical Wave Propagation Along the Principal Lattice Axes | p. 124 |
4.6.2 Case 2: Numerical Wave Propagation Along a Grid Diagonal | p. 127 |
4.6.3 Example of Calculation of Numerical Phase Velocity and Attenuation | p. 129 |
4.6.4 Example of Calculation of Wave Propagation | p. 131 |
4.7 Numerical Stability | p. 133 |
4.7.1 Complex-Frequency Analysis | p. 133 |
4.7.2 Example of a Numerically Unstable Two-Dimensional FDTD Model | p. 139 |
4.8 Generalized Stability Problem | p. 141 |
4.8.1 Boundary Conditions | p. 141 |
4.8.2 Variable and Unstructured Meshing | p. 142 |
4.8.3 Lossy, Dispersive, Nonlinear, and Gain Materials | p. 142 |
4.9 Modified Yee-Based Algorithms for Improved Numerical Dispersion | p. 142 |
4.9.1 Strategy 1: Center a Specific Numerical Phase-Velocity Curve About c | p. 143 |
4.9.2 Strategy 2: Use Fourth-Order-Accurate Spatial Differences | p. 143 |
4.9.3 Strategy 3: Use Hexagonal Grids | p. 152 |
4.9.4 Strategy 4: Use Discrete Fourier Transforms to Calculate the Spatial Derivatives | p. 156 |
4.10 Alternating-Direction-Implicit Time-Stepping Algorithm for Operation Beyond the Courant Limit | p. 160 |
4.10.1 Numerical Formulation of the Zheng/Chen/Zhang Algorithm | p. 162 |
4.10.2 Numerical Stability | p. 169 |
4.10.3 Numerical Dispersion | p. 171 |
4.10.4 Discussion | p. 171 |
4.11 Summary | p. 172 |
References | p. 172 |
Problems | p. 173 |
Projects | p. 174 |
5 Incident Wave Source Conditions | p. 175 |
5.1 Introduction | p. 175 |
5.2 Pointwise E and H Hard Sources in One Dimension | p. 176 |
5.3 Pointwise E and H Hard Sources in Two Dimensions | p. 178 |
5.3.1 Green's Function for the Scalar Wave Equation in Two Dimensions | p. 178 |
5.3.2 Obtaining Comparative FDTD Data | p. 179 |
5.3.3 Results for Effective Action Radius of a Hard-Sourced Field Component | p. 180 |
5.4 J and M Current Sources in Three Dimensions | p. 182 |
5.4.1 Sources and Charging | p. 183 |
5.4.2 Sinusoidal Sources | p. 184 |
5.4.3 Transient (Pulse) Sources | p. 185 |
5.4.4 Intrinsic Lattice Capacitance | p. 189 |
5.4.5 Intrinsic Lattice Inductance | p. 190 |
5.4.6 Impact Upon FDTD Simulations of Lumped-Element Capacitors and Inductors | p. 191 |
5.5 The Plane-Wave Source Condition | p. 193 |
5.6 The Total-Field/Scattered-Field Technique: Ideas and One-Dimensional Formulation | p. 194 |
5.6.1 Ideas | p. 194 |
5.6.2 One-Dimensional Formulation | p. 197 |
5.7 Two-Dimensional Formulation of the TF/SF Technique | p. 201 |
5.7.1 Consistency Conditions | p. 203 |
5.7.2 Calculation of the Incident Field | p. 207 |
5.7.3 Illustrative Example | p. 212 |
5.8 Three-Dimensional Formulation of the TF/SF Technique | p. 212 |
5.8.1 Consistency Conditions | p. 216 |
5.8.2 Calculation of the Incident Field | p. 221 |
5.9 Pure Scattered-Field Formulation | p. 224 |
5.9.1 Application to PEC Structures | p. 224 |
5.9.2 Application to Lossy Dielectric Structures | p. 225 |
5.9.3 Choice of Incident Plane-Wave Formulation | p. 227 |
5.10 Waveguide Source Conditions | p. 227 |
5.10.1 Pulsed Electric Field Modal Hard Source | p. 228 |
5.10.2 Total-Field/Reflected-Field Modal Formulation | p. 229 |
5.10.3 Resistive Source and Load Conditions | p. 230 |
5.11 Summary | p. 231 |
References | p. 232 |
Problems | p. 232 |
Projects | p. 232 |
6 Analytical Absorbing Boundary Conditions | p. 235 |
6.1 Introduction | p. 235 |
6.2 Bayliss-Turkel Radiation Operators | p. 237 |
6.2.1 Spherical Coordinates | p. 238 |
6.2.2 Cylindrical Coordinates | p. 241 |
6.3 Engquist-Majda One-Way Wave Equations | p. 244 |
6.3.1 One-Term and Two-Term Taylor Series Approximations | p. 245 |
6.3.2 Mur Finite-Difference Scheme | p. 248 |
6.3.3 Trefethen-Halpern Generalized and Higher Order ABCs | p. 251 |
6.3.4 Theoretical Reflection Coefficient Analysis | p. 253 |
6.3.5 Numerical Experiments | p. 256 |
6.4 Higdon Radiation Operators | p. 261 |
6.4.1 Formulation | p. 261 |
6.4.2 First Two Higdon Operators | p. 263 |
6.4.3 Discussion | p. 264 |
6.5 Liao Extrapolation in Space and Time | p. 265 |
6.5.1 Formulation | p. 265 |
6.5.2 Discussion | p. 267 |
6.6 Ramahi Complementary Operators | p. 269 |
6.6.1 Basic Idea | p. 269 |
6.6.2 Complementary Operators | p. 270 |
6.6.3 Effect of Multiple Wave Reflections | p. 271 |
6.6.4 Basis of the Concurrent Complementary Operator Method | p. 273 |
6.6.5 Illustrative FDTD Modeling Results Obtained Using the C-COM | p. 278 |
6.7 Summary | p. 281 |
References | p. 281 |
Problems | p. 282 |
7 Perfectly Matched Layer Absorbing Boundary Conditions | p. 285 |
7.1 Introduction | p. 285 |
7.2 Plane Wave Incident Upon a Lossy Half-Space | p. 286 |
7.3 Plane Wave Incident Upon Berenger's PML Medium | p. 288 |
7.3.1 Two-Dimensional TE[subscript z] Case | p. 289 |
7.3.2 Two-Dimensional TM[subscript z] Case | p. 293 |
7.3.3 Three-Dimensional Case | p. 294 |
7.4 Stretched-Coordinate Formulation of Berenger's PML | p. 295 |
7.5 An Anisotropic PML Absorbing Medium | p. 298 |
7.5.1 Perfectly Matched Uniaxial Medium | p. 298 |
7.5.2 Relationship to Berenger's Split-Field PML | p. 301 |
7.5.3 A Generalized Three-Dimensional Formulation | p. 302 |
7.5.4 Inhomogeneous Media | p. 304 |
7.6 Theoretical Performance of the PML | p. 305 |
7.6.1 The Continuous Space | p. 305 |
7.6.2 The Discrete Space | p. 305 |
7.7 Efficient Implementation of UPML in FDTD | p. 308 |
7.7.1 Derivation of the Finite-Difference Expressions | p. 308 |
7.7.2 Computer Implementation of the UPML | p. 311 |
7.8 Numerical Experiments With Berenger's Split-Field PML | p. 314 |
7.8.1 Outgoing Cylindrical Wave in a Two-Dimensional Open-Region Grid | p. 314 |
7.8.2 Outgoing Spherical Wave in a Three-Dimensional Open-Region Lattice | p. 316 |
7.8.3 Dispersive Wave Propagation in Metal Waveguides | p. 318 |
7.8.4 Dispersive and Multimode Wave Propagation in Dielectric Waveguides | p. 320 |
7.9 Numerical Experiments With UPML | p. 322 |
7.9.1 Current Source Radiating in an Unbounded Two-Dimensional Region | p. 322 |
7.9.2 Highly Elongated Domains | p. 327 |
7.9.3 Microstrip Transmission Line | p. 330 |
7.10 UPML Termination for Conductive Media | p. 332 |
7.10.1 Theory | p. 332 |
7.10.2 Numerical Example: Termination of a Conductive Half-Space Medium | p. 335 |
7.11 UPML Termination for Dispersive Media | p. 338 |
7.11.1 Theory | p. 338 |
7.11.2 Numerical Example: Reflection by a Lorentz Medium | p. 343 |
7.12 Summary and Conclusions | p. 343 |
References | p. 345 |
Projects | p. 347 |
8 Near-to-Far-Field Transformation | p. 349 |
8.1 Introduction | p. 349 |
8.2 Two-Dimensional Transformation, Phasor Domain | p. 350 |
8.2.1 Application of Green's Theorem | p. 351 |
8.2.2 Far-Field Limit | p. 352 |
8.2.3 Reduction to Standard Form | p. 354 |
8.3 Obtaining Phasor Quantities Via Discrete Fourier Transformation | p. 356 |
8.4 Surface Equivalence Theorem | p. 359 |
8.5 Extension to Three Dimensions, Phasor Domain | p. 361 |
8.6 Time-Domain Near-to-Far-Field Transformation | p. 366 |
8.7 Summary | p. 371 |
References | p. 372 |
Project | p. 372 |
9 Dispersive and Nonlinear Materials | p. 373 |
9.1 Introduction | p. 373 |
9.2 Types of Dispersions Considered | p. 374 |
9.2.1 Debye Media | p. 374 |
9.2.2 Lorentz Media | p. 375 |
9.3 Piecewise-Linear Recursive Convolution Method, Linear Material Case | p. 375 |
9.3.1 General Formulation of the Method | p. 375 |
9.3.2 Application to Debye Media | p. 378 |
9.3.3 Application to Lorentz Media | p. 379 |
9.3.4 Numerical Results | p. 380 |
9.4 Piecewise-Linear Recursive Convolution Method, Nonlinear Dispersive Material Case | p. 382 |
9.4.1 Governing Equations | p. 382 |
9.4.2 General Formulation of the Method | p. 384 |
9.4.3 FDTD Realization in One Dimension | p. 386 |
9.4.4 Numerical Results | p. 388 |
9.5 Auxiliary Differential Equation Method, Linear Material Case | p. 392 |
9.5.1 Formulation for Multiple Debye Poles | p. 392 |
9.5.2 Formulation for Multiple Lorentz Pole Pairs | p. 394 |
9.5.3 Numerical Results | p. 397 |
9.6 Auxiliary Differential Equation Method, Nonlinear Dispersive Material Case | p. 398 |
9.6.1 Formulation for Multiple Lorentz Pole Pairs, TM[subscript Z] Case | p. 398 |
9.6.2 Numerical Results for Temporal Solitons | p. 401 |
9.6.3 Numerical Results for Spatial Solitons | p. 404 |
9.7 Summary and Conclusions | p. 407 |
References | p. 408 |
Problems | p. 409 |
Projects | p. 410 |
10 Local Subcell Models of Fine Geometrical Features | p. 411 |
10.1 Introduction | p. 411 |
10.2 Basis of Contour-Path FDTD Modeling | p. 412 |
10.3 The Simplest Contour-Path Subcell Models | p. 413 |
10.3.1 Diagonal Split-Cell Model for PEC Surfaces | p. 413 |
10.3.2 Average Properties Model for Material Surfaces | p. 415 |
10.4 The Contour-Path Model of the Narrow Slot | p. 416 |
10.5 The Contour-Path Model of the Thin Wire | p. 420 |
10.6 Locally Conformal Models of Curved Surfaces | p. 424 |
10.6.1 Dey-Mittra Technique for PEC Structures | p. 424 |
10.6.2 Illustrative Results for PEC Structures | p. 427 |
10.6.3 Dey-Mittra Technique for Material Structures | p. 433 |
10.7 Maloney-Smith Technique for Thin Material Sheets | p. 434 |
10.7.1 Basis | p. 434 |
10.7.2 Illustrative Results | p. 438 |
10.8 Dispersive Surface Impedance | p. 442 |
10.8.1 Maloney-Smith Method | p. 442 |
10.8.2 Beggs Method | p. 449 |
10.8.3 Lee Method | p. 457 |
10.9 Relativistic Motion of PEC Boundaries | p. 461 |
10.9.1 Basis | p. 461 |
10.9.2 Illustrative Results | p. 465 |
10.10 Summary and Discussion | p. 468 |
References | p. 470 |
Bibliography | p. 471 |
Projects | p. 472 |
11 Nonorthogonal and Unstructured Grids | p. 473 |
11.1 Introduction | p. 473 |
11.2 Nonuniform Orthogonal Grids | p. 474 |
11.3 Locally Conformal Grids, Globally Orthogonal | p. 482 |
11.4 Global Curvilinear Coordinates | p. 484 |
11.4.1 Nonorthogonal Curvilinear FDTD Algorithm | p. 484 |
11.4.2 Stability Criterion | p. 490 |
11.5 Irregular Nonorthogonal Structured Grids | p. 493 |
11.6 Irregular Nonorthogonal Unstructured Grids | p. 500 |
11.6.1 Generalized Yee Algorithm | p. 500 |
11.6.2 Inhomogeneous Media | p. 506 |
11.6.3 Practical Implementation of the Generalized Yee Algorithm | p. 508 |
11.7 A Planar Generalized Yee Algorithm | p. 509 |
11.7.1 Time-Stepping Expressions | p. 510 |
11.7.2 Projection Operators | p. 511 |
11.7.3 Efficient Time-Stepping Implementation | p. 513 |
11.8 Examples of Passive-Circuit Modeling Using the Planar Generalized Yee Algorithm | p. 514 |
11.8.1 32-GHz Wilkinson Power Divider | p. 514 |
11.8.2 32-GHz Gysel Power Divider | p. 517 |
11.8.3 Signal Lines in an IBM Thermal Conduction Module | p. 518 |
11.9 Summary and Conclusions | p. 522 |
References | p. 523 |
Problems | p. 525 |
Projects | p. 527 |
12 Bodies of Revolution | p. 529 |
12.1 Introduction | p. 529 |
12.2 Field Expansion | p. 530 |
12.3 Difference Equations for Off-Axis Cells | p. 530 |
12.3.1 Ampere's Law Contour Path Integral to Calculate e[subscript r] | p. 532 |
12.3.2 Ampere's Law Contour Path Integral to Calculate e[subscript phi] | p. 534 |
12.3.3 Ampere's Law Contour Path Integral to Calculate e[subscript z] | p. 536 |
12.3.4 Difference Equations | p. 539 |
12.3.5 Surface-Conforming Contour Path Integrals | p. 542 |
12.4 Difference Equations for On-Axis Cells | p. 544 |
12.4.1 Ampere's Law Contour Path Integral to Calculate e[subscript z] on the z-Axis | p. 544 |
12.4.2 Ampere's Law Contour Path Integral to Calculate e[subscript phi] on the z-Axis | p. 546 |
12.4.3 Faraday's Law Calculation of h[subscript r] on the z-Axis | p. 548 |
12.5 Numerical Stability | p. 549 |
12.6 PML Absorbing Boundary Condition | p. 549 |
12.6.1 BOR-FDTD Background | p. 549 |
12.6.2 Extension of PML to the General BOR Case | p. 552 |
12.6.3 Examples | p. 558 |
12.7 Application to Particle Accelerator Physics | p. 560 |
12.7.1 Definitions and Concepts | p. 560 |
12.7.2 Examples | p. 563 |
12.8 Summary | p. 566 |
References | p. 566 |
Problems | p. 567 |
Projects | p. 568 |
13 Analysis of Periodic Structures | p. 569 |
13.1 Introduction | p. 569 |
13.2 Review of Scattering From Periodic Structures | p. 572 |
13.3 Direct Field Methods | p. 575 |
13.3.1 Normal Incidence Case | p. 575 |
13.3.2 Multiple Unit Cells for Oblique Incidence | p. 577 |
13.3.3 Sine-Cosine Method | p. 579 |
13.3.4 Angled-Update Method | p. 580 |
13.4 Introduction to the Field-Transformation Technique | p. 584 |
13.5 Multiple-Grid Approach | p. 589 |
13.5.1 Formulation | p. 589 |
13.5.2 Numerical Stability Analysis | p. 591 |
13.5.3 Numerical Dispersion Analysis | p. 592 |
13.5.4 Lossy Materials | p. 593 |
13.5.5 Lossy Screen Example | p. 595 |
13.6 Split-Field Method, Two Dimensions | p. 596 |
13.6.1 Formulation | p. 596 |
13.6.2 Numerical Stability Analysis | p. 598 |
13.6.3 Numerical Dispersion Analysis | p. 600 |
13.6.4 Lossy Materials | p. 601 |
13.6.5 Lossy Screen Example | p. 602 |
13.7 Split-Field Method, Three Dimensions | p. 603 |
13.7.1 Formulation | p. 603 |
13.7.2 Numerical Stability Analysis | p. 607 |
13.7.3 UPML Absorbing Boundary Condition | p. 610 |
13.8 Application of the Periodic FDTD Method | p. 614 |
13.8.1 Photonic Bandgap Structures | p. 614 |
13.8.2 Frequency-Selective Surfaces | p. 616 |
13.8.3 Antenna Arrays | p. 618 |
13.9 Summary and Conclusions | p. 623 |
Acknowledgments | p. 623 |
References | p. 623 |
Projects | p. 625 |
14 Modeling of Antennas | p. 627 |
14.1 Introduction | p. 627 |
14.2 Formulation of the Antenna Problem | p. 628 |
14.2.1 Transmitting Antenna | p. 628 |
14.2.2 Receiving Antenna | p. 630 |
14.2.3 Symmetry | p. 630 |
14.2.4 Excitation | p. 632 |
14.3 Antenna Feed Models | p. 634 |
14.3.1 Detailed Modeling of the Feed | p. 634 |
14.3.2 Simple Gap Feed Model for a Monopole Antenna | p. 636 |
14.3.3 Improved Simple Feed Model | p. 639 |
14.4 Near-to-Far-Field Transformations | p. 644 |
14.4.1 Use of Symmetry | p. 645 |
14.4.2 Time-Domain Near-to-Far-Field Transformation | p. 646 |
14.4.3 Frequency-Domain Near-Field to Far-Field Transformation | p. 648 |
14.5 Plane-Wave Source | p. 649 |
14.5.1 Effect of an Incremental Displacement of the Surface Currents | p. 649 |
14.5.2 Effect of an Incremental Time Shift | p. 651 |
14.5.3 Relation to Total-Field/Scattered-Field Lattice Zoning | p. 652 |
14.6 Case Study I: The Standard-Gain Horn | p. 653 |
14.7 Case Study II: The Vivaldi Slotline Array | p. 659 |
14.7.1 Background | p. 659 |
14.7.2 The Planar Element | p. 660 |
14.7.3 The Vivaldi Pair | p. 665 |
14.7.4 The Vivaldi Quad | p. 665 |
14.7.5 The Linear Phased Array | p. 668 |
14.7.6 Phased-Array Radiation Characteristics Indicated by the FDTD Modeling | p. 669 |
14.7.7 Active Impedance of the Phased Array | p. 669 |
14.8 Near-Field Simulations | p. 675 |
14.8.1 Generic 900-MHz Cellphone Handset in Free Space | p. 675 |
14.8.2 900-MHz Dipole Antenna Near a Layered Bone-Brain Half-Space | p. 676 |
14.8.3 840-MHz Dipole Antenna Near a Rectangular Brain Phantom | p. 678 |
14.8.4 900-MHz Infinitesimal Dipole Antenna Near a Spherical Brain Phantom | p. 680 |
14.8.5 1,900-MHz Half-Wavelength Dipole Near a Spherical Brain Phantom | p. 681 |
14.9 Selected Recent Applications | p. 682 |
14.9.1 Use of Photonic-Bandgap Materials | p. 682 |
14.9.2 Ground-Penetrating Radar | p. 682 |
14.9.3 Antenna-Radome Interaction | p. 687 |
14.9.4 Personal Wireless Communications Devices | p. 690 |
14.9.5 Biomedical Applications of Antennas | p. 696 |
14.10 Summary and Conclusions | p. 697 |
References | p. 697 |
Projects | p. 701 |
15 High-Speed Electronic Circuits With Active and Nonlinear Components | p. 703 |
15.1 Introduction | p. 703 |
15.2 Basic Circuit Parameters | p. 705 |
15.2.1 Transmission Line Parameters | p. 706 |
15.2.2 Impedance | p. 706 |
15.2.3 S Parameters | p. 707 |
15.3 Differential Capacitance Calculation | p. 708 |
15.4 Differential Inductance Calculation | p. 709 |
15.5 Lumped Inductance Due to a Discontinuity | p. 711 |
15.5.1 Flux / Current Definition | p. 711 |
15.5.2 Fitting Z([omega]) or S([omega]) to an Equivalent Circuit | p. 712 |
15.5.3 Discussion: Choice of Methods | p. 712 |
15.6 Inductance of Complex Power-Distribution Systems | p. 713 |
15.6.1 Method Description | p. 713 |
15.6.2 Example: Multiplane Meshed Printed-Circuit Board | p. 715 |
15.6.3 Discussion | p. 718 |
15.7 Parallel Coplanar Microstrips | p. 718 |
15.8 Multilayered Interconnect Modeling Example | p. 720 |
15.9 Digital Signal Processing and Spectrum Estimation | p. 721 |
15.9.1 Prony's Method | p. 721 |
15.9.2 Autoregressive Models | p. 725 |
15.9.3 Pade Approximation | p. 729 |
15.10 Modeling of Lumped Circuit Elements | p. 734 |
15.10.1 FDTD Formulation Extended to Circuit Elements | p. 734 |
15.10.2 The Resistor | p. 736 |
15.10.3 The Resistive Voltage Source | p. 737 |
15.10.4 The Capacitor | p. 737 |
15.10.5 The Inductor | p. 738 |
15.10.6 The Diode | p. 740 |
15.10.7 The Bipolar Junction Transistor | p. 741 |
15.11 Direct Linking of FDTD and SPICE | p. 743 |
15.11.1 Basic Idea | p. 745 |
15.11.2 Norton Equivalent Circuit "Looking Into" the FDTD Space Lattice | p. 745 |
15.11.3 Thevenin Equivalent Circuit "Looking Into" the FDTD Space Lattice | p. 748 |
15.12 Case Study: A 6-GHz MESFET Amplifier Model | p. 750 |
15.12.1 Large-Signal Model | p. 750 |
15.12.2 Amplifier Configuration | p. 753 |
15.12.3 Analysis of the Circuit Without the Packaging Structure | p. 754 |
15.12.4 Analysis of the Circuit With the Packaging Structure | p. 756 |
15.13 Summary and Conclusions | p. 759 |
Acknowledgements | p. 760 |
References | p. 761 |
Additional Bibliography | p. 763 |
Projects | p. 764 |
16 Microcavity Optical Resonators | p. 767 |
16.1 Introduction | p. 767 |
16.2 Issues Related to FDTD Modeling of Optical Structures | p. 768 |
16.2.1 Optical Waveguides | p. 768 |
16.2.2 Material Dispersion and Nonlinearities | p. 772 |
16.3 Macroscopic Modeling of Optical Gain Media | p. 772 |
16.3.1 Theory | p. 773 |
16.3.2 Validation Studies | p. 776 |
16.4 Application to Vertical-Cavity Surface-Emitting Lasers | p. 780 |
16.4.1 Passive Studies | p. 782 |
16.4.2 Active Studies | p. 784 |
16.5 Microcavities Based on Photonic Bandgap Structures, Quasi One-Dimensional Case | p. 788 |
16.6 Microcavities Based on Photonic Bandgap Structures, Two-Dimensional Case | p. 793 |
16.7 Microcavity Ring Resonators | p. 797 |
16.7.1 FDTD Modeling Considerations | p. 797 |
16.7.2 Coupling to Straight Waveguides | p. 800 |
16.7.3 Coupling to Curved Waveguides | p. 802 |
16.7.4 Elongated Ring Designs | p. 804 |
16.7.5 Resonances | p. 806 |
16.8 Microcavity Disk Resonators | p. 810 |
16.8.1 Resonance Behavior | p. 811 |
16.8.2 Suppression of Higher Order Radial Whispering-Gallery Modes | p. 815 |
16.8.3 Additional FDTD Modeling Studies | p. 819 |
16.9 Summary and Conclusions | p. 819 |
References | p. 822 |
Additional Bibliography | p. 825 |
Projects | p. 826 |
Acronyms | p. 827 |
About the Authors | p. 831 |
Index | p. 839 |