Preface |
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ix | |
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1 | (6) |
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2 Distributions and Derivatives in the Sense of Distribution |
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7 | (42) |
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2.1 Functions and Distributions |
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7 | (2) |
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2.2 Test Functions. The Space C0∞ |
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9 | (5) |
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14 | (2) |
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16 | (5) |
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2.5 Some Simple Operations in D' |
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21 | (5) |
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2.5.1 Multiplication by a Real Number or a Function |
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21 | (1) |
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2.5.2 Translation and Rescaling |
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21 | (1) |
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2.5.3 Derivation of a Distribution |
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22 | (4) |
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2.6 Order of a Distribution |
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26 | (5) |
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2.7 The Support of a Distribution |
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31 | (2) |
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33 | (16) |
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2.8.1 Distributions on Multidimensional Spaces |
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33 | (5) |
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2.8.2 Vector-Valued Distributions |
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38 | (11) |
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3 Maxwell Equations in the Sense of Distribution |
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49 | (18) |
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3.1 Maxwell Equations Reduced into the Vacuum |
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49 | (5) |
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3.1.1 Some Simple Examples |
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53 | (1) |
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3.2 Universal Boundary Conditions and Compatibility Relations |
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54 | (5) |
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3.2.1 An Example. Discontinuities on a Combined Sheet |
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57 | (2) |
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3.3 The Concept of Material Sheet |
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59 | (3) |
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3.4 The Case of Monochromatic Fields |
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62 | (5) |
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3.4.1 Discontinuities on the Interface Between Two Simple Media that Are at Rest |
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64 | (3) |
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4 Boundary Conditions on Material Sheets at Rest |
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67 | (42) |
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4.1 Universal Boundary Conditions and Compatibility Relations for a Fixed Material Sheet |
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67 | (2) |
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69 | (1) |
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4.3 Some Particular Cases |
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70 | (39) |
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4.3.1 Planar Material Sheet Between Two Simple Media |
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70 | (21) |
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4.3.2 Cylindrically or Spherically Curved Material Sheet Located Between Two Simple Media |
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91 | (2) |
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4.3.3 Conical Material Sheet Located Between Two Simple Media |
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93 | (16) |
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5 Discontinuities on a Moving Sheet |
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109 | (40) |
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5.1 Special Theory of Relativity |
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110 | (10) |
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5.1.1 The Field Created by a Uniformly Moving Point Charge |
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112 | (2) |
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5.1.2 The Expressions of the Field in a Reference System Attached to the Charged Particle |
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114 | (1) |
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5.1.3 Lorentz Transformation Formulas |
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115 | (3) |
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5.1.4 Transformation of the Electromagnetic Field |
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118 | (2) |
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5.2 Discontinuities on a Uniformly Moving Surface |
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120 | (18) |
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5.2.1 Transformation of the Universal Boundary Conditions |
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123 | (3) |
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5.2.2 Transformation of the Compatibility Relations |
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126 | (1) |
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5.2.3 Some Simple Examples |
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126 | (12) |
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5.3 Discontinuities on a Nonuniformly Moving Sheet |
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138 | (11) |
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5.3.1 Boundary Conditions on a Plane that Moves in a Direction Normal to Itself |
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139 | (4) |
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5.3.2 Boundary Conditions on the Interface of Two Simple Media |
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143 | (6) |
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6 Edge Singularities on Material Wedges Bounded by Plane Boundaries |
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149 | (30) |
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149 | (4) |
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6.2 Singularities at the Edges of Material Wedges |
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153 | (1) |
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6.3 The Wedge with Penetrable Boundaries |
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154 | (20) |
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156 | (15) |
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171 | (3) |
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6.4 The Wedge with Impenetrable Boundaries |
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174 | (1) |
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6.5 Examples. Application to Half-Planes |
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175 | (1) |
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6.6 Edge Conditions for the Induced Surface Currents |
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176 | (3) |
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7 Tip Singularities at the Apex of a Material Cone |
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179 | (30) |
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179 | (6) |
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7.2 Algebraic Singularities of an H-Type Field |
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185 | (6) |
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7.2.1 Contribution of the Energy Restriction |
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185 | (1) |
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7.2.2 Contribution of the Boundary Conditions |
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186 | (5) |
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7.3 Algebraic Singularities of an E-Type Field |
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191 | (2) |
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7.4 The Case of Impenetrable Cones |
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193 | (2) |
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7.5 Confluence and Logarithmic Singularities |
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195 | (2) |
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7.6 Application to some Widely used Actual Boundary Conditions |
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197 | (3) |
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7.7 Numerical Solutions of the Transcendental Equations Satisfied by the Minimal Index |
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200 | (9) |
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7.7.1 The Case of Very Sharp Tip |
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200 | (1) |
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7.7.2 The Case of Real-Valued Minimal ν |
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201 | (2) |
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7.7.3 A Function-Theoretic Method to Determine Numerically the Minimal ν |
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203 | (6) |
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8 Temporal Discontinuities |
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209 | (6) |
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8.1 Universal Initial Conditions |
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209 | (2) |
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8.2 Linear Mediums in the Generalized Sense |
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211 | (1) |
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8.3 An Illustrative Example |
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212 | (3) |
References |
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215 | (4) |
Index |
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219 | |
IEEE Press Series on Electromagnetic Wave Theory |
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