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1 | (8) |
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1 | (1) |
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About the Content of the Book |
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2 | (1) |
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3 | (6) |
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Part I Classical Description of the Interaction of Light with Matter |
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The Linear Dielectric Susceptibility |
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9 | (12) |
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9 | (1) |
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The Dielectric Susceptibility |
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10 | (2) |
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12 | (3) |
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15 | (1) |
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Example: Orientation Polarization and Debye's Equations |
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15 | (6) |
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The Classical Treatment of Free and Bound Charge Carriers |
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21 | (16) |
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21 | (5) |
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Derivation of Drude's Formula |
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21 | (3) |
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Extended Detail: Another Evaluation of Drude's Formula |
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24 | (2) |
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The Oscillator Model for Bound Charge Carriers |
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26 | (9) |
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26 | (1) |
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27 | (3) |
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The Clausius-Mossotti and Lorentz-Lorenz-Equations |
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30 | (5) |
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Probing Matter in Different Spectral Regions |
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35 | (2) |
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Derivations from the Oscillator Model |
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37 | (24) |
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37 | (1) |
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Extended Detail: Homogeneous and Inhomogeneous Line Broadening Mechanisms |
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38 | (3) |
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Oscillators with More Than One Degree of Freedom |
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41 | (1) |
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Sellmeier's and Cauchy's Formulae |
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42 | (3) |
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Optical Properties of Mixtures |
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45 | (16) |
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Motivation and Example from Practice |
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45 | (4) |
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Extended Detail: The Maxwell Garnett, Bruggeman, and Lorentz--Lorenz Mixing Models |
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49 | (4) |
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Extended Detail: Remarks on Surface Plasmons |
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53 | (3) |
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Extended Detail: The Effect of Pores |
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56 | (5) |
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The Kramers--Kronig Relations |
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61 | (10) |
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Derivation of the Kramers Kronig Relations |
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61 | (3) |
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64 | (2) |
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66 | (5) |
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66 | (1) |
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67 | (4) |
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Part II Interface Reflection and Interference Phenomena in Thin Film Systems |
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71 | (30) |
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Transmission, Reflection, Absorption, and Scattering |
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71 | (5) |
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71 | (2) |
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73 | (2) |
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Remarks on the Absorbance Concept |
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75 | (1) |
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The Effect of Planar Interfaces: Fresnel's Formulae |
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76 | (8) |
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Total Reflection of Light |
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84 | (3) |
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Conditions of Total Reflection |
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84 | (1) |
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85 | (1) |
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Attenuated Total Reflection ATR |
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86 | (1) |
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87 | (9) |
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87 | (4) |
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Extended Detail: Propagating Surface Plasmons |
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91 | (5) |
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Extended Detail: Anisotropic Materials |
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96 | (5) |
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Interface Reflection Between an Isotropic and an Anisotropic Material |
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96 | (3) |
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Giant Birefringent Optics |
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99 | (2) |
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Thick Slabs and Thin Films |
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101 | (24) |
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Transmittance and Reflectance of a Thick Slab |
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101 | (3) |
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Thick Slabs and Thin Films |
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104 | (3) |
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107 | (3) |
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110 | (15) |
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110 | (2) |
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112 | (1) |
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113 | (2) |
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115 | (1) |
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A Single Thin Film on a Thick Substrate |
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116 | (4) |
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Extended Detail: A Few More Words on Reverse Search Procedures |
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120 | (5) |
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Extended Details: Gradient Index Films and Multilayers |
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125 | (16) |
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125 | (9) |
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125 | (1) |
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126 | (2) |
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128 | (1) |
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Calculation of Transmittance and Reflectance |
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129 | (5) |
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134 | (7) |
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The Characteristic Matrix |
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134 | (3) |
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Characteristic Matrix of a Single Homogeneous Film |
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137 | (1) |
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Characteristic Matrix of a Film Stack |
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137 | (1) |
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Calculation of Transmittance and Reflectance |
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138 | (3) |
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141 | (22) |
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Quarterwave Stacks and Derived Systems |
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141 | (4) |
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Extended Detail: Remarks on Resonant Grating Waveguide Structures |
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145 | (6) |
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145 | (1) |
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Propagating Modes and Grating Period |
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146 | (1) |
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Energy Exchange Between the Propagating Modes |
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147 | (1) |
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Analytical Film Thickness Estimation for a GWS |
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148 | (2) |
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150 | (1) |
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151 | (12) |
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151 | (2) |
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153 | (4) |
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157 | (6) |
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Part III Semiclassical Description of the Interaction of Light with Matter |
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163 | (24) |
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163 | (1) |
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Phenomenological Description |
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163 | (2) |
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165 | (2) |
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Extended Detail: Perturbation Theory of Quantum Transitions |
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167 | (5) |
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Extended Detail: Planck's Formula |
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172 | (4) |
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172 | (1) |
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173 | (1) |
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173 | (3) |
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Extended Detail: Expressions for Einstein Coefficients in the Dipole Approximation |
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176 | (4) |
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180 | (7) |
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Population Inversion and Light Amplification |
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180 | (1) |
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181 | (6) |
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Semiclassical Treatment of the Dielectric Function |
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187 | (12) |
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187 | (1) |
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Extended Detail: Calculation of the Dielectric Function by Means of the Density Matrix |
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188 | (11) |
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188 | (2) |
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Introduction of the Density Matrix |
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190 | (5) |
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Semiclassical Calculation of the Polarizability |
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195 | (4) |
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199 | (32) |
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Formal Treatment of the Dielectric Function of Crystals (Direct Transitions) |
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199 | (5) |
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204 | (4) |
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208 | (3) |
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211 | (7) |
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211 | (3) |
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214 | (4) |
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Resume from Chapters 10--12 |
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218 | (13) |
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218 | (4) |
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222 | (9) |
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Part IV Basics of Nonlinear Optics |
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Some Basic Effects of Nonlinear Optics |
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231 | (24) |
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Nonlinear Susceptibilities: Phenomenological Approach |
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231 | (11) |
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231 | (2) |
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Formal Treatment and Simple Second Order Nonlinear Optical Effects |
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233 | (7) |
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240 | (2) |
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Calculation Scheme for Nonlinear Optical Susceptibilities |
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242 | (10) |
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Macroscopic Susceptibilities and Microscopic Hyperpolarizabilities |
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242 | (1) |
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Density Matrix Approach for Calculating Optical Hyperpolarizabilities |
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243 | (5) |
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248 | (4) |
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252 | (3) |
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252 | (1) |
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253 | (2) |
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255 | (6) |
| Bibliography |
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261 | (10) |
| Index |
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271 | |