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1 Input-Output Formalism for Few-Photon Transport |
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1 | (24) |
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1 | (1) |
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1.2 Hamiltonian and Input-Output Formalism |
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2 | (3) |
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1.3 Quantum Causality Relation |
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5 | (3) |
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1.4 Connection to Scattering Theory |
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8 | (2) |
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1.5 Single-Photon Transport |
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10 | (2) |
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12 | (2) |
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1.7 Example: A Waveguide Coupled to a Kerr-Nonlinear Cavity |
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14 | (2) |
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1.8 Wavefunction Approach |
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16 | (3) |
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19 | (6) |
Appendix |
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20 | (2) |
References |
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22 | (23) |
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2 Quadrature-Squeezed Light from Emitters in Optical Nanostructures |
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25 | (22) |
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25 | (5) |
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2.1.1 Quadrature-Squeezed Light |
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27 | (1) |
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27 | (1) |
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2.1.3 Squeezed Light sources |
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28 | (2) |
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2.2 Theoretical Description |
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30 | (3) |
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2.2.1 Macroscopic Quantum Electrodynamics |
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30 | (1) |
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2.2.2 The Optical Bloch Equations |
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31 | (1) |
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2.2.3 Squeezed Resonance Fluorescence |
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32 | (1) |
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2.3 Quadrature Squeezing Assisted by Nanostructures |
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33 | (11) |
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2.3.1 A Single Emitter Coupled to a Nanostructure |
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33 | (7) |
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2.3.2 Cooperative Quadrature Squeezing |
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40 | (4) |
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2.4 Conclusions and Outlook |
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44 | (3) |
References |
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45 | (24) |
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3 Coupling of Quantum Emitters to Plasmonic Nanoguides |
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47 | (26) |
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47 | (1) |
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3.2 Theory of Coupling an Emitter to a Plasmonic Waveguide |
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48 | (8) |
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3.2.1 Modes in Plasmonic Waveguides |
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49 | (2) |
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51 | (5) |
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3.3 Experimental Demonstrations of Coupling a Quantum Emitter to Plasmonic Nanoguides |
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56 | (12) |
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56 | (4) |
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3.3.2 Coupling of Quantum Emitters to Plasmonic Waveguides |
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60 | (8) |
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3.4 Conclusion and Outlook |
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68 | (5) |
References |
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69 | (254) |
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4 Controlled Interaction of Single Nitrogen Vacancy Centers with Surface Plasmons |
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73 | (24) |
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73 | (1) |
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4.2 Scanning Probe Assembly |
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74 | (13) |
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4.2.1 Control of Emission Dynamics Through Plasmon Coupling |
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75 | (3) |
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4.2.2 Coupling of NV Centers to Propagating Surface Plasmons |
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78 | (9) |
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4.3 Optical Trapping as a Positioning Tool |
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87 | (6) |
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4.3.1 Experimental Platform to Optically Trap a Single NV Center |
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88 | (1) |
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4.3.2 Surface Plasmon Based Trapping |
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89 | (4) |
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4.4 Conclusions and Outlook |
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93 | (1) |
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94 | (3) |
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5 Hyperbolic Metamaterials for Single-Photon Sources and Nanolasers |
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97 | (24) |
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98 | (1) |
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5.2 Fundamentals of Hyperbolic Metamaterials |
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99 | (1) |
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5.3 Enhancement of Single-Photon Emission from Color Centers in Diamond |
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100 | (8) |
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5.3.1 Calculations of NV Emission Enhancement by HMM |
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103 | (1) |
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5.3.2 Experimental Demonstration of HMM Enhanced Single-Photon Emission |
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104 | (2) |
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5.3.3 Increasing Collection Efficiency by Outcoupling High-k Waves to Free Space |
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106 | (2) |
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5.4 Lasing Action with Nanorod Hyperbolic Metamaterials |
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108 | (7) |
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5.4.1 Purcell Effect Calculations for Dye Molecules on Nanorod Metamaterials |
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111 | (2) |
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5.4.2 Experimental Demonstration of Lasing with Nanorod Metamaterials |
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113 | (2) |
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115 | (1) |
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Appendix: Semi-analytical Calculations of the Purcell Factor and Normalized Collected Emission Power |
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115 | (2) |
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117 | (4) |
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6 Strong Coupling Between Organic Molecules and Plasmonic Nanostructures |
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121 | (30) |
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121 | (3) |
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6.2 Theoretical Background |
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124 | (5) |
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124 | (2) |
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6.2.2 Semi-Classical Approach |
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126 | (2) |
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6.2.3 Fully Quantum-Mechanical Approach |
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128 | (1) |
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6.3 Coupling of Organic Molecules with Plasmonic Structures |
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129 | (2) |
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6.4 Dynamics of Strong Coupling |
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131 | (3) |
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132 | (1) |
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133 | (1) |
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6.5 Surface Lattice Resonances |
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134 | (7) |
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6.5.1 Empty Lattice Approximation |
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135 | (2) |
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6.5.2 Lattice of Point Dipoles |
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137 | (3) |
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6.5.3 Band Gap Formation in SLR Dispersions |
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140 | (1) |
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6.6 Strong Coupling in Nanoparticle Arrays |
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141 | (6) |
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6.6.1 Spectral Transmittance Experiments |
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142 | (3) |
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6.6.2 Spatial Coherence of Strongly Coupled Hybrid Modes |
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145 | (2) |
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147 | (1) |
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148 | (3) |
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7 Polar it on Condensation in Organic Semiconductors |
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151 | (14) |
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Konstantinos S. Daskalakis |
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151 | (1) |
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7.2 What Is a Condensate? |
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152 | (1) |
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7.3 Planar Microcavity Structures |
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153 | (3) |
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156 | (2) |
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158 | (2) |
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160 | (2) |
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162 | (1) |
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163 | (2) |
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8 Plasmon Particle Array Lasers |
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165 | (26) |
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166 | (1) |
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8.2 Experiments on Plasmon Lattice Laser |
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167 | (4) |
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8.2.1 Samples and Experimental Methods |
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167 | (2) |
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8.2.2 Input-Output Curves, Thresholds and Fourier Space |
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169 | (2) |
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8.3 Theory of Plasmon Lattices Coupled to Stratified Media |
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171 | (10) |
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8.3.1 Two-Dimensional Periodic Arrays, Folded Dispersion, and the "Nearly Free-Photon" Approximation |
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172 | (1) |
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8.3.2 Surface Lattice Resonances |
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173 | (1) |
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8.3.3 Semi-analytical Approach: Polarizability and Lattice Sums |
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174 | (4) |
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8.3.4 Theoretical Model--Results |
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178 | (2) |
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8.3.5 Stop Gap and Band Crossing |
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180 | (1) |
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8.4 Open Questions for Periodic Plasmon Lasers |
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181 | (1) |
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8.5 Scattering, Aperiodic and Finite Lasers |
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182 | (3) |
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185 | (1) |
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Appendix A 1D Green's Function |
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185 | (1) |
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Appendix B Ewald Summation |
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186 | (2) |
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188 | (3) |
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9 Surface Plasmon Enhanced Schottky Detectors |
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191 | (20) |
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191 | (1) |
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9.2 SPPs and Photodetection Mechanisms |
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192 | (4) |
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196 | (3) |
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9.4 Nanoparticle and Nanoantenna Detectors |
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199 | (3) |
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202 | (5) |
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9.6 Summary and Prospects |
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207 | (1) |
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208 | (3) |
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10 Antenna-Coupled Tunnel Junctions |
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211 | (26) |
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211 | (2) |
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10.2 Theoretical Framework |
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213 | (7) |
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213 | (1) |
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10.2.2 Photon Emission: A Two-Step Process |
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213 | (1) |
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214 | (6) |
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10.3 Coupling Tunnel Junctions to Free Space |
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220 | (10) |
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10.3.1 Macroscopic Solid State Tunnel Devices |
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220 | (4) |
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10.3.2 Scanning Tunneling Microscope |
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224 | (1) |
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10.3.3 Antenna-Coupled Tunnel Junctions |
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225 | (5) |
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230 | (1) |
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230 | (3) |
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10.4.1 Ultrafast Photon/SPP Sources |
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230 | (1) |
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10.4.2 LDOS and Impedance Matching Optimization |
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230 | (2) |
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10.4.3 Beyond MIM Devices |
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232 | (1) |
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10.4.4 Resonant Tunneling |
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232 | (1) |
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10.4.5 Stimulated Emission |
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232 | (1) |
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10.4.6 Beyond Visible Light Emission |
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233 | (1) |
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233 | (1) |
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233 | (4) |
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11 Spontaneous Emission in Nonlocal Metamaterials with Spatial Dispersion |
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237 | (42) |
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238 | (2) |
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11.2 Nonlocal Effective Medium Theory |
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240 | (18) |
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11.2.1 Calculation of Ez and Hz |
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241 | (1) |
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11.2.2 Calculation of Er, Hr, Eφ, and |
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242 | (2) |
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11.2.3 Applying the Boundary Conditions at r = R |
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244 | (2) |
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11.2.4 Dispersion of the Longitudinal Mode |
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246 | (3) |
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11.2.5 Solutions at Oblique Angles |
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249 | (3) |
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11.2.6 Wave Profiles at Oblique Angles |
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252 | (1) |
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11.2.7 Simplified Approach to Nonlocal Effective Medium Theory |
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253 | (1) |
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11.2.8 Nonlocal Transfer Matrix Method |
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254 | (4) |
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11.3 Dipole Emission in Nonlocal Metamaterials |
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258 | (13) |
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11.3.1 Plane Wave Expansion of Green's Function in Homogeneous Material |
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261 | (4) |
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11.3.2 Spontaneous Decay Rates Near Planar Interfaces |
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265 | (2) |
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11.3.3 Emission in Lossless Metamaterials and Local Field Corrections |
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267 | (2) |
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11.3.4 Effects of Finite Material Absorption |
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269 | (1) |
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11.3.5 Non-Local Field Correction Approach |
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269 | (2) |
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11.4 Experimental Results on Collective Purcell Enhancement |
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271 | (3) |
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274 | (1) |
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274 | (5) |
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12 Nonlocal Response in Plasmonic Nanostructures |
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279 | (24) |
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279 | (2) |
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12.2 Linear-Response Theory |
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281 | (3) |
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12.3 Linear-Response Electrodynamics |
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284 | (1) |
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12.4 Hydrodynamic Drift-Diffusion Theory |
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285 | (3) |
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288 | (1) |
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12.6 Numerical Implementations |
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289 | (2) |
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12.7 Characteristic Material Parameters |
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291 | (1) |
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12.8 A Unifying Description of Monomers and Dimers |
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292 | (4) |
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12.9 The Origin of Diffusion: Insight from ab Initio studies |
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296 | (3) |
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12.10 Conclusions and Outlook |
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299 | (1) |
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300 | (3) |
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13 Landau Damping---The Ultimate Limit of Field Confinement and Enhancement in Plasmonic Structures |
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303 | (20) |
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303 | (2) |
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13.2 Spill Out and Nonlocality in the Hydrodynamic Model |
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305 | (1) |
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13.3 Landau Damping as the Cause of Nonlocality |
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306 | (5) |
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13.4 Limits of Confinement in Propagating SPP |
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311 | (3) |
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13.5 Landau (Surface Collision) Damping in Multipole Modes of Spherical Nanoparticles |
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314 | (3) |
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13.6 Impact of Landau (Surface Collision) Damping on Field Enhancement in Dimer |
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317 | (3) |
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320 | (1) |
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321 | (2) |
Index |
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323 | |