About the Authors |
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xvii | |
Preface |
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xix | |
Acknowledgments |
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xxiii | |
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1 Maxwell's Equations, Constitutive Relations, Wave Equation, and Polarization |
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1 | (51) |
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1.1 Introductory Comments |
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1 | (4) |
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5 | (5) |
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1.3 Constitutive Relations |
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10 | (5) |
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1.4 Frequency Domain Fields |
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15 | (4) |
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1.5 Kramers-Kronig Relationship |
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19 | (2) |
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1.6 Vector and Scalar Wave Equations |
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21 | (2) |
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1.6.1 Vector Wave Equations for EM Fields |
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21 | (1) |
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1.6.2 Scalar Wave Equations for EM Fields |
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22 | (1) |
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1.7 Separable Solutions of the Source-Free Wave Equation in Rectangular Coordinates and for Isotropic Homogeneous Media. Plane Waves |
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23 | (6) |
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1.8 Polarization of Plane Waves, Poincare Sphere, and Stokes Parameters |
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29 | (11) |
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1.8.1 Polarization States |
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29 | (3) |
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1.8.2 General Elliptical Polarization |
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32 | (4) |
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1.8.3 Decomposition of a Polarization State into Circularly Polarized Components |
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36 | (1) |
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1.8.4 Poincare Sphere for Describing Polarization States |
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37 | (3) |
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1.9 Phase and Group Velocity |
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40 | (4) |
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1.10 Separable Solutions of the Source-Free Wave Equation in Cylindrical and Spherical Coordinates and for Isotropic Homogeneous Media |
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44 | (7) |
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1.10.1 Source-Free Cylindrical Wave Solutions |
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44 | (4) |
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1.10.2 Source-Free Spherical Wave Solutions |
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48 | (3) |
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51 | (1) |
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2 EM Boundary and Radiation Conditions |
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52 | (35) |
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2.1 EM Field Behavior Across a Boundary Surface |
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52 | (8) |
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2.2 Radiation Boundary Condition |
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60 | (3) |
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2.3 Boundary Conditions at a Moving Interface |
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63 | (21) |
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2.3.1 Nonrelativistic Moving Boundary Conditions |
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63 | (3) |
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2.3.2 Derivation of the Nonrelativistic Field Transformations |
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66 | (3) |
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2.3.3 EM Field Transformations Based on the Special Theory of Relativity |
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69 | (15) |
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2.4 Constitutive Relations for a Moving Medium |
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84 | (1) |
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85 | (2) |
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3 Plane Wave Propagation in Planar Layered Media |
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87 | (57) |
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87 | (1) |
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3.2 Plane Wave Reflection from a Planar Boundary Between Two Different Media |
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87 | (25) |
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3.2.1 Perpendicular Polarization Case |
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88 | (5) |
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3.2.2 Parallel Polarization Case |
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93 | (4) |
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97 | (3) |
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100 | (4) |
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3.2.5 Plane Wave Incident on a Lossy Half Space |
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104 | (6) |
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3.2.6 Doppler Shift for Wave Reflection from a Moving Mirror |
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110 | (2) |
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3.3 Reflection and Transmission of a Plane Wave Incident on a Planar Stratified Isotropic Medium Using a Transmission Matrix Approach |
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112 | (7) |
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3.4 Plane Waves in Anisotropic Homogeneous Media |
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119 | (16) |
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3.5 State Space Formulation for Waves in Planar Anisotropic Layered Media |
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135 | (8) |
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3.5.1 Development of State Space Based Field Equations |
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135 | (4) |
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3.5.2 Reflection and Transmission of Plane Waves at the Interface Between Two Anisotropic Half Spaces |
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139 | (3) |
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3.5.3 Transmission Type Matrix Analysis of Plane Waves in Multilayered Anisotropic Media |
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142 | (1) |
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143 | (1) |
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4 Plane Wave Spectral Representation for EM Fields |
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144 | (12) |
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144 | (1) |
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144 | (11) |
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155 | (1) |
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5 Electromagnetic Potentials and Fields of Sources in Unbounded Regions |
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156 | (55) |
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5.1 Introduction to Vector and Scalar Potentials |
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156 | (4) |
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5.2 Construction of the Solution for A |
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160 | (5) |
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5.3 Calculation of Fields from Potentials |
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165 | (11) |
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5.4 Time Dependent Potentials for Sources and Fields in Unbounded Regions |
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176 | (9) |
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5.5 Potentials and Fields of a Moving Point Charge |
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185 | (7) |
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192 | (3) |
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5.7 Direct Calculation of Fields of Sources in Unbounded Regions Using a Dyadic Green's Function |
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195 | (14) |
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5.7.1 Fields of Sources in Unbounded, Isotropic, Homogeneous Media in Terms of a Closed Form Representation of Green's Dyadic, G0 |
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195 | (2) |
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5.7.2 On the Singular Nature of G0(r\r') for Observation Points Within the Source Region |
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197 | (4) |
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5.7.3 Representation of the Green's Dyadic G0 in Terms of an Integral in the Wavenumber (k) Space |
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201 | (7) |
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5.7.4 Electromagnetic Radiation by a Source in a General Bianisotropic Medium Using a Green's Dyadic Ga in k-Space |
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208 | (1) |
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209 | (2) |
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6 Electromagnetic Field Theorems and Related Topics |
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211 | (103) |
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6.1 Conservation of Charge |
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211 | (1) |
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6.2 Conservation of Power |
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212 | (6) |
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6.3 Conservation of Momentum |
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218 | (7) |
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225 | (10) |
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235 | (7) |
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6.6 Reciprocity Theorems and Conservation of Reactions |
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242 | (9) |
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6.6.1 The Lorentz Reciprocity Theorem |
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243 | (6) |
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6.6.2 Reciprocity Theorem for Bianisotropic Media |
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249 | (2) |
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251 | (3) |
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254 | (4) |
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258 | (20) |
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6.9.1 Volume Equivalence Theorem for EM Scattering |
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258 | (2) |
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6.9.2 A Surface Equivalence Theorem for EM Scattering |
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260 | (10) |
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6.9.3 A Surface Equivalence Theorem for Antennas |
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270 | (8) |
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278 | (4) |
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6.11 Antenna Equivalent Circuit |
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282 | (1) |
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6.12 The Receiving Antenna Problem |
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282 | (5) |
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6.13 Expressions for Antenna Mutual Coupling Based on Generalized Reciprocity Theorems |
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287 | (10) |
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6.13.1 Circuit Form of the Reciprocity Theorem for Antenna Mutual Coupling |
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287 | (5) |
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6.13.2 A Mixed Circuit Field Form of a Generalized Reciprocity Theorem for Antenna Mutual Coupling |
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292 | (2) |
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6.13.3 A Mutual Admittance Expression for Slot Antennas |
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294 | (2) |
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6.13.4 Antenna Mutual Coupling, Reaction Concept, and Antenna Measurements |
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296 | (1) |
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6.14 Relation Between Antenna and Scattering Problems |
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297 | (11) |
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6.14.1 Exterior Radiation by a Slot Aperture Antenna Configuration |
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297 | (2) |
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6.14.2 Exterior Radiation by a Monopole Antenna Configuration |
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299 | (9) |
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308 | (1) |
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6.16 Antenna Directive Gain |
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309 | (2) |
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6.17 Field Decomposition Theorem |
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311 | (2) |
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313 | (1) |
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7 Modal Techniques for the Analysis of Guided Waves, Resonant Cavities, and Periodic Structures |
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314 | (139) |
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7.1 On Modal Analysis of Some Guided Wave Problems |
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314 | (1) |
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7.2 Classification of Modal Fields in Uniform Guiding Structures |
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314 | (11) |
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315 | (10) |
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325 | (3) |
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328 | (2) |
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7.5 Modal Expansions in Closed Uniform Waveguides |
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330 | (7) |
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331 | (1) |
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332 | (2) |
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7.5.3 Orthogonality of Modes in Closed Perfectly Conducting Uniform Waveguides |
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334 | (3) |
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7.6 Effect of Losses in Closed Guided Wave Structures |
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337 | (1) |
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7.7 Source Excited Uniform Closed Perfectly Conducting Waveguides |
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338 | (4) |
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7.8 An Analysis of Some Closed Metallic Waveguides |
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342 | (41) |
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7.8.1 Modes in a Parallel Plate Waveguide |
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342 | (8) |
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7.8.2 Modes in a Rectangular Waveguide |
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350 | (8) |
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7.8.3 Modes in a Circular Waveguide |
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358 | (6) |
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364 | (2) |
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7.8.5 Obstacles and Discontinuities in Waveguides |
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366 | (13) |
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7.8.6 Modal Propagation Past a Slot in a Waveguide |
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379 | (4) |
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7.9 Closed and Open Waveguides Containing Penetrable Materials and Coatings |
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383 | (17) |
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7.9.1 Material-Loaded Closed PEC Waveguide |
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384 | (4) |
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7.9.2 Material Slab Waveguide |
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388 | (7) |
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7.9.3 Grounded Material Slab Waveguide |
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395 | (1) |
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395 | (3) |
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7.9.5 Circular Cylindrical Optical Fiber Waveguides |
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398 | (2) |
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7.10 Modal Analysis of Resonators |
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400 | (9) |
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7.10.1 Rectangular Waveguide Cavity Resonator |
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402 | (4) |
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7.10.2 Circular Waveguide Cavity Resonator |
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406 | (2) |
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7.10.3 Dielectric Resonators |
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408 | (1) |
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7.11 Excitation of Resonant Cavities |
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409 | (2) |
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7.12 Modal Analysis of Periodic Arrays |
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411 | (11) |
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7.12.1 Floquet Modal Analysis of an Infinite Planar Periodic Array of Electric Current Sources |
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412 | (7) |
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7.12.2 Floquet Modal Analysis of an Infinite Planar Periodic Array of Current Sources Configured in a Skewed Grid |
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419 | (3) |
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7.13 Higher-Order Floquet Modes and Associated Grating Lobe Circle Diagrams for Infinite Planar Periodic Arrays |
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422 | (3) |
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7.13.1 Grating Lobe Circle Diagrams |
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422 | (3) |
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7.14 On Waves Guided and Radiated by Periodic Structures |
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425 | (5) |
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7.15 Scattering by a Planar Periodic Array |
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430 | (7) |
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7.15.1 Analysis of the EM Plane Wave Scattering by an Infinite Periodic Slot Array in a Planar PEC Screen |
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432 | (5) |
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7.16 Finite 1-D and 2-D Periodic Array of Sources |
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437 | (14) |
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7.16.1 Analysis of Finite 1-D Periodic Arrays for the Case of Uniform Source Distribution and Far Zone Observation |
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437 | (7) |
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7.16.2 Analysis of Finite 2-D Periodic Arrays for the Case of Uniform Distribution and Far Zone Observation |
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444 | (2) |
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7.16.3 Floquet Modal Representation for Near and Far Fields of 1-D Nonuniform Finite Periodic Array Distributions |
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446 | (3) |
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7.16.4 Floquet Modal Representation for Near and Far Fields of 2-D Nonuniform Planar Periodic Finite Array Distributions |
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449 | (2) |
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451 | (2) |
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8 Green's Functions for the Analysis of One-Dimensional Source-Excited Wave Problems |
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453 | (69) |
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8.1 Introduction to the Sturm-Liouville Form of Differential Equation for 1-D Wave Problems |
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453 | (3) |
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8.2 Formulation of the Solution to the Sturm-Liouville Problem via the 1-D Green's Function Approach |
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456 | (7) |
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8.3 Conditions Under Which the Green's Function Is Symmetric |
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463 | (1) |
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8.4 Construction of the Green's Function G(x\x') |
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464 | (2) |
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8.4.1 General Procedure to Obtain G(x\x') |
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464 | (2) |
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8.5 Alternative Simplified Construction of G(x\x') Valid for the Symmetric Case |
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466 | (17) |
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8.6 On the Existence and Uniqueness of G(x\x') |
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483 | (1) |
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8.7 Eigenfunction Expansion Representation for G(x\x') |
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483 | (5) |
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8.8 Delta Function Completeness Relation and the Construction of Eigenfunctions from G(x\x') = U(x<)T(x>)/W |
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488 | (31) |
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8.9 Explicit Representation of G(x\x') Using Step Functions |
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519 | (1) |
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520 | (2) |
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9 Applications of One-Dimensional Green's Function Approach for the Analysis of Single and Coupled Set of EM Source Excited Transmission Lines |
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522 | (32) |
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522 | (1) |
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9.2 Analytical Formulation for a Single Transmission Line Made Up of Two Conductors |
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522 | (3) |
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9.3 Wave Solution for the Two Conductor Lines When There Are No Impressed Sources Distributed Anywhere Within the Line |
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525 | (2) |
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9.4 Wave Solution for the Case of Impressed Sources Placed Anywhere on a Two Conductor Line |
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527 | (14) |
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9.5 Excitation of a Two Conductor Transmission Line by an Externally Incident Electromagnetic Wave |
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541 | (2) |
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9.6 A Matrix Green's Function Approach for Analyzing a Set of Coupled Transmission Lines |
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543 | (3) |
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9.7 Solution to the Special Case of Two Coupled Lines (N = 2) with Homogeneous Dirichlet or Neumann End Conditions |
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546 | (5) |
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9.8 Development of the Multiport Impedance Matrix for a Set of Coupled Transmission Lines |
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551 | (1) |
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9.9 Coupled Transmission Line Problems with Voltage Sources and Load Impedances at the End Terminals |
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552 | (1) |
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553 | (1) |
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10 Green's Functions for the Analysis of Two- and Three-Dimensional Source-Excited Scalar and EM Vector Wave Problems |
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554 | (116) |
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554 | (1) |
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10.2 General Formulation for Source-Excited 3-D Separable Scalar Wave Problems Using Green's Functions |
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555 | (11) |
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10.3 General Procedure for Construction of Scalar 2-D and 3-D Green's Function in Rectangular Coordinates |
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566 | (3) |
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10.4 General Procedure for Construction of Scalar 2-D and 3-D Green's Functions in Cylindrical Coordinates |
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569 | (3) |
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10.5 General Procedure for Construction of Scalar 3-D Green's Functions in Spherical Coordinates |
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572 | (3) |
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10.6 General Formulation for Source-Excited 3-D Separable EM Vector Wave Problems Using Dyadic Green's Functions |
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575 | (8) |
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10.7 Some Specific Green's Functions for 2-D Problems |
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583 | (40) |
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10.7.1 Fields of a Uniform Electric Line Source |
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583 | (7) |
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10.7.2 Fields of an Infinite Periodic Array of Electric Line Sources |
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590 | (1) |
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10.7.3 Line Source-Excited PEC Circular Cylinder Green's Function |
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591 | (5) |
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10.7.4 A Cylindrical Wave Series Expansion for H0(2)(k\ρ - ρ'\) |
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596 | (2) |
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10.7.5 Line Source Excitation of a PEC Wedge |
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598 | (4) |
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10.7.6 Line Source Excitation of a PEC Parallel Plate Waveguide |
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602 | (4) |
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10.7.7 The Fields of a Line Dipole Source |
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606 | (2) |
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10.7.8 Fields of a Magnetic Line Source on an Infinite Planar Impedance Surface |
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608 | (4) |
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10.7.9 Fields of a Magnetic Line Dipole Source on an Infinite Planar Impedance Surface |
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612 | (2) |
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10.7.10 Circumferentially Propagating Surface Fields of a Line Source Excited Impedance Circular Cylinder |
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614 | (3) |
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10.7.11 Analysis of Circumferentially Propagating Waves for a Line Dipole Source-Excited Impedance Circular Cylinder |
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617 | (2) |
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10.7.12 Fields of a Traveling Wave Line Source |
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619 | (1) |
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10.7.13 Traveling Wave Line Source Excitation of a PEC Wedge and a PEC Cylinder |
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620 | (3) |
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10.8 Examples of Some Alternative Representations of Green's Functions for Scalar 3-D Point Source-Excited Cylinders, Wedges and Spheres |
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623 | (29) |
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10.8.1 3-D Scalar Point Source-Excited Circular Cylinder Green's Function |
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623 | (7) |
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10.8.2 3-D Scalar Point Source Excitation of a Wedge |
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630 | (2) |
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10.8.3 Angularly and Radially Propagating 3-D Scalar Point Source Green's Function for a Sphere |
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632 | (8) |
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10.8.4 Kontorovich--Lebedev Transform and MacDonald Based Approaches for Constructing an Angularly Propagating 3-D Point Source Scalar Wedge Green's Function |
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640 | (7) |
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10.8.5 Analysis of the Fields of a Vertical Electric or Magnetic Current Point Source on a PEC Sphere |
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647 | (5) |
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10.9 General Procedure for Construction of EM Dyadic Green's Functions for Source-Excited Separable Canonical Problems via Scalar Green's Functions |
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652 | (13) |
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10.9.1 Summary of Procedure to Obtain the EM Fields of Arbitrarily Oriented Point Sources Exciting Canonical Separable Configurations |
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653 | (12) |
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10.10 Completeness of the Eigenfunction Expansion of the Dyadic Green's Function at the Source Point |
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665 | (4) |
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669 | (1) |
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11 Method of Factorization and the Wiener--Hopf Technique for Analyzing Two-Part EM Wave Problems |
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670 | (27) |
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11.1 The Wiener--Hopf Procedure |
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670 | (12) |
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11.2 The Dual Integral Equation Approach |
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682 | (9) |
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691 | (5) |
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696 | (1) |
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12 Integral Equation-Based Methods for the Numerical Solution of Nonseparable EM Radiation and Scattering Problems |
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697 | (45) |
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697 | (1) |
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12.2 Boundary Integral Equations |
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697 | (8) |
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12.2.1 The Electric Field Integral Equation (EFIE) |
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699 | (1) |
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12.2.2 The Magnetic Field Integral Equation (MFIE) |
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700 | (1) |
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12.2.3 Combined Field and Combined Source Integral Equations |
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701 | (1) |
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12.2.4 Impedance Boundary Condition |
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702 | (1) |
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12.2.5 Boundary Integral Equation for a Homogeneous Material Volume |
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703 | (2) |
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12.3 Volume Integral Equations |
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705 | (1) |
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12.4 The Numerical Solution of Integral Equations |
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706 | (14) |
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12.4.1 The Minimum Square-Error Method |
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706 | (2) |
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12.4.2 The Method of Moments (MoM) |
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708 | (2) |
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12.4.3 Simplification of the MoM Impedance Matrix Integrals |
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710 | (3) |
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12.4.4 Expansion and Testing Functions |
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713 | (5) |
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12.4.5 Low-Frequency Break-Down |
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718 | (2) |
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12.5 Iterative Solution of Large MoM Matrices |
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720 | (12) |
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12.5.1 Fast Iterative Solution of MoM Matrix Equations |
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721 | (4) |
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12.5.2 The Fast Multipole Method (FMM) |
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725 | (5) |
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12.5.3 Multilevel FMM and Fast Fourier Transform FMM |
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730 | (2) |
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12.6 Antenna Modeling with the Method of Moments |
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732 | (2) |
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12.7 Aperture Coupling with the Method of Moments |
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734 | (2) |
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12.8 Physical Optics Methods |
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736 | (4) |
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12.8.1 Physical Optics for a PEC Surface |
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736 | (2) |
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12.8.2 Iterative Physical Optics |
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738 | (2) |
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740 | (2) |
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13 Introduction to Characteristic Modes |
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742 | (10) |
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742 | (1) |
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13.2 Characteristic Modes from the EFIE for a Conducting Surface |
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743 | (3) |
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13.2.1 Electric Field Integral Equation and Radiation Operator |
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743 | (1) |
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13.2.2 Eigenfunctions of the Electric Field Radiation Operator |
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743 | (2) |
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13.2.3 Characteristic Modes from the EFIE Impedance Matrix |
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745 | (1) |
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13.3 Computation of Characteristic Modes |
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746 | (2) |
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13.4 Solution of the EFIE Using Characteristic Modes |
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748 | (1) |
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13.5 Tracking Characteristic Modes with Frequency |
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749 | (1) |
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13.6 Antenna Excitation Using Characteristic Modes |
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749 | (1) |
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750 | (2) |
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14 Asymptotic Evaluation of Radiation and Diffraction Type Integrals for High Frequencies |
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752 | (66) |
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752 | (1) |
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14.2 Steepest Descent Techniques for the Asymptotic Evaluation of Radiation Integrals |
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752 | (39) |
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14.2.1 Topology of the Exponent in the Integrand Containing a First-Order Saddle Point |
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753 | (3) |
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14.2.2 Asymptotic Evaluation of Integrals Containing a First-Order Saddle Point in Its Integrand Which Is Free of Singularities |
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756 | (4) |
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14.2.3 Asymptotic Evaluation of Integrals Containing a Higher-Order Saddle Point in Its Integrand Which Is Free of Singularities |
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760 | (3) |
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14.2.4 Pauli--Clemmow Method (PCM) for the Asymptotic Evaluation of Integrals Containing a First-Order Saddle Point Near a Simple Pole Singularity |
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763 | (10) |
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14.2.5 Van der Waerden Method (VWM) for the Asymptotic Evaluation of Integrals Containing a First-Order Saddle Point Near a Simple Pole Singularity |
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773 | (2) |
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14.2.6 Relationship Between PCM and VWM Leading to a Generalized PCM (or GPC) Solution |
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775 | (2) |
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14.2.7 An Extension of PCM for Asymptotic Evaluation of an Integral Containing a First-Order Saddle Point and a Nearby Double Pole |
|
|
777 | (2) |
|
14.2.8 An Extension of PCM for Asymptotic Evaluation of an Integral Containing a First-Order Saddle Point and Two Nearby First-Order Poles |
|
|
779 | (4) |
|
14.2.9 An Extension of VWM for Asymptotic Evaluation of an Integral Containing a First-Order Saddle Point and a Nearby Double Pole |
|
|
783 | (1) |
|
14.2.10 Nonuniform Asymptotic Evaluation of an Integral Containing a Saddle Point and a Branch Point |
|
|
784 | (5) |
|
14.2.11 Uniform Asymptotic Evaluation of an Integral Containing a Saddle Point and a Nearby Branch Point |
|
|
789 | (2) |
|
14.3 Asymptotic Evaluation of Integrals with End Points |
|
|
791 | (3) |
|
14.3.1 Watson's Lemma for Integrals |
|
|
792 | (1) |
|
14.3.2 Generalized Watson's Lemma for Integrals |
|
|
792 | (1) |
|
14.3.3 Integration by Parts for Asymptotic Evaluation of a Class of Integrals |
|
|
792 | (2) |
|
14.4 Asymptotic Evaluation of Radiation Integrals Based on the Stationary Phase Method |
|
|
794 | (22) |
|
14.4.1 Stationary Phase Evaluation of 1-D Infinite Integrals |
|
|
794 | (1) |
|
14.4.2 Nonuniform Stationary Phase Evaluation of 1-D Integrals with End Points |
|
|
795 | (1) |
|
14.4.3 Uniform Stationary Phase Evaluation of 1-D Integrals with a Nearby End Point |
|
|
796 | (5) |
|
14.4.4 Nonuniform Stationary Phase Evaluation of 2-D Infinite Integrals |
|
|
801 | (15) |
|
|
816 | (2) |
|
15 Physical and Geometrical Optics |
|
|
818 | (37) |
|
15.1 The Physical Optics (PO) Approximation for PEC Surfaces |
|
|
818 | (2) |
|
15.2 The Geometrical Optics (GO) Ray Field |
|
|
820 | (4) |
|
15.3 GO Transport Singularities |
|
|
824 | (4) |
|
15.4 Wavefronts, Stationary Phase, and GO |
|
|
828 | (4) |
|
15.5 GO Incident and Reflected Ray Fields |
|
|
832 | (8) |
|
15.6 Uniform GO Valid at Smooth Caustics |
|
|
840 | (14) |
|
|
854 | (1) |
|
16 Geometrical and Integral Theories of Diffraction |
|
|
855 | (96) |
|
16.1 Geometrical Theory of Diffraction and Its Uniform Version (UTD) |
|
|
855 | (6) |
|
16.2 UTD for an Edge in an Otherwise Smooth PEC Surface |
|
|
861 | (11) |
|
16.3 UTD Slope Diffraction for an Edge |
|
|
872 | (2) |
|
16.4 An Alternative Uniform Solution (the UAT) for Edge Diffraction |
|
|
874 | (1) |
|
16.5 UTD Solutions for Fields of Sources in the Presence of Smooth PEC Convex Surfaces |
|
|
874 | (39) |
|
16.5.1 UTD Analysis of the Scattering by a Smooth, Convex Surface |
|
|
876 | (9) |
|
16.5.2 UTD for the Radiation by Antennas on a Smooth, Convex Surface |
|
|
885 | (16) |
|
16.5.3 UTD Analysis of the Surface Fields of Antennas on a Smooth, Convex Surface |
|
|
901 | (12) |
|
|
913 | (2) |
|
16.7 UTD for Edge-Excited Surface Rays |
|
|
915 | (6) |
|
16.8 The Equivalent Line Current Method (ECM) |
|
|
921 | (5) |
|
16.8.1 Line Type ECM for Edge-Diffracted Ray Caustic Field Analysis |
|
|
922 | (4) |
|
16.9 Equivalent Line Current Method for Interior PEC Waveguide Problems |
|
|
926 | (7) |
|
|
927 | (5) |
|
|
932 | (1) |
|
16.10 The Physical Theory of Diffraction (PTD) |
|
|
933 | (7) |
|
16.10.1 PTD for Edged Bodies - A Canonical Edge Diffraction Problem in the PTD Development |
|
|
936 | (1) |
|
16.10.2 Details of PTD for 3-D Edged Bodies |
|
|
937 | (2) |
|
16.10.3 Reduction of PTD to 2-D Edged Bodies |
|
|
939 | (1) |
|
16.11 On the PTD for Aperture Problems |
|
|
940 | (1) |
|
16.12 Time-Domain Uniform Geometrical Theory of Diffraction (TD-UTD) |
|
|
940 | (5) |
|
16.12.1 Introductory Comments |
|
|
940 | (1) |
|
16.12.2 Analytic Time Transform (ATT) |
|
|
941 | (1) |
|
16.12.3 TD-UTD for a General PEC Curved Wedge |
|
|
942 | (3) |
|
|
945 | (6) |
|
17 Development of Asymptotic High-Frequency Solutions to Some Canonical Problems |
|
|
951 | (91) |
|
|
951 | (1) |
|
17.2 Development of UTD Solutions for Some Canonical Wedge Diffraction Problems |
|
|
951 | (23) |
|
17.2.1 Scalar 2-D Line Source Excitation of a Wedge |
|
|
952 | (6) |
|
17.2.2 Scalar Plane Wave Excitation of a Wedge |
|
|
958 | (2) |
|
17.2.3 Scalar Spherical Wave Excitation of a Wedge |
|
|
960 | (5) |
|
17.2.4 EM Plane Wave Excitation of a PEC Wedge |
|
|
965 | (3) |
|
17.2.5 EM Conical Wave Excitation of a PEC Wedge |
|
|
968 | (3) |
|
17.2.6 EM Spherical Wave Excitation of a PEC Wedge |
|
|
971 | (3) |
|
17.3 Canonical Problem of Slope Diffraction by a PEC Wedge |
|
|
974 | (4) |
|
17.4 Development of a UTD Solution for Scattering by a Canonical 2-D PEC Circular Cylinder and Its Generalization to a Convex Cylinder |
|
|
978 | (13) |
|
17.4.1 Field Analysis for the Shadowed Part of the Transition Region |
|
|
982 | (3) |
|
17.4.2 Field Analysis for the Illuminated Part of the Transition Region |
|
|
985 | (6) |
|
17.5 A Collective UTD for an Efficient Ray Analysis of the Radiation by Finite Conformal Phased Arrays on Infinite PEC Circular Cylinders |
|
|
991 | (13) |
|
17.5.1 Finite Axial Array on a Circular PEC Cylinder |
|
|
992 | (7) |
|
17.5.2 Finite Circumferential Array on a Circular PEC Cylinder |
|
|
999 | (5) |
|
17.6 Surface, Leaky, and Lateral Waves Associated with Planar Material Boundaries |
|
|
1004 | (28) |
|
|
1004 | (1) |
|
17.6.2 The EM Fields of a Magnetic Line Source on a Uniform Planar Impedance Surface |
|
|
1004 | (7) |
|
17.6.3 EM Surface and Leaky Wave Fields of a Uniform Line Source over a Planar Grounded Material Slab |
|
|
1011 | (8) |
|
17.6.4 An Analysis of the Lateral Wave Phenomena Arising in the Problem of a Vertical Electric Point Current Source over a Dielectric Half Space |
|
|
1019 | (13) |
|
17.7 Surface Wave Diffraction by a Planar, Two-Part Impedance Surface: Development of a Ray Solution |
|
|
1032 | (6) |
|
|
1033 | (3) |
|
|
1036 | (2) |
|
17.8 Ray Solutions for Special Cases of Discontinuities in Nonconducting or Penetrable Boundaries |
|
|
1038 | (1) |
|
|
1039 | (3) |
|
18 EM Beams and Some Applications |
|
|
1042 | (23) |
|
|
1042 | (1) |
|
18.2 Astigmatic Gaussian Beams |
|
|
1043 | (8) |
|
18.2.1 Paraxial Wave Equation Solutions |
|
|
1043 | (1) |
|
|
1044 | (3) |
|
18.2.3 3-D Astigmatic Gaussian Beams |
|
|
1047 | (1) |
|
18.2.4 3-D Gaussian Beam from a Gaussian Aperture Distribution |
|
|
1048 | (2) |
|
18.2.5 Reflection of Astigmatic Gaussian Beams (GBs) |
|
|
1050 | (1) |
|
18.3 Complex Source Beams and Relation to GBs |
|
|
1051 | (10) |
|
18.3.1 Introduction to Complex Source Beams (CSBs) |
|
|
1051 | (1) |
|
18.3.2 Complex Source Beam from Scalar Green's Function |
|
|
1051 | (3) |
|
18.3.3 Representation of Arbitrary EM Fields by a CSB Expansion |
|
|
1054 | (2) |
|
18.3.4 Edge Diffraction of an Incident CSB by a Curved Conducting Wedge |
|
|
1056 | (5) |
|
18.4 Pulsed Complex Source Beams in the Time Domain |
|
|
1061 | (2) |
|
|
1063 | (2) |
A Coordinate Systems, Vectors, and Dyadics |
|
1065 | (7) |
B The Total Time Derivative of a Time Varying Flux Density Integrated Over a Moving Surface |
|
1072 | (3) |
C The Delta Function |
|
1075 | (3) |
D Transverse Fields in Terms of Axial Field Components for TMZ and TEZ Waves Guided Along z |
|
1078 | (2) |
E Two Different Representations for Partial Poisson Sum Formulas and Their Equivalence |
|
1080 | (2) |
F Derivation of 1-D Green's Second Identity |
|
1082 | (1) |
G Green's Second Identity for 3-D Scalar, Vector, and Vector-Dyadic Wave Fields |
|
1083 | (3) |
H Formal Decomposition and Factorization Formulas |
|
1086 | (3) |
I On the Transition Function F(±Ka) |
|
1089 | (3) |
J On the Branch Cuts Commonly Encountered in the Evaluation of Spectral Wave Integrals |
|
1092 | (4) |
K On the Steepest Descent Path (SDP) for Spectral Wave Integrals |
|
1096 | (3) |
L Parameters Used in the Uniform GO Solution for the Lit and Shadow Sides of a Smooth Caustic |
|
1099 | (2) |
M Asymptotic Approximations of Hankel Functions for Large Argument and Various Orders |
|
1101 | (4) |
Index |
|
1105 | |