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1 | (14) |
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1.1 Electron Waves at the Nanoscale |
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1 | (2) |
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1.2 Open Quantum Billiards |
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3 | (2) |
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1.3 Taming Wave Propagation in the Deep Quantum Regime |
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5 | (2) |
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1.4 The Necessity of Efficient Computational Techniques |
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7 | (1) |
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8 | (7) |
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9 | (6) |
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2 Electrons in Low-Dimensional Mesoscopic Systems |
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15 | (22) |
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2.1 Two-Dimensional Electron Systems |
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15 | (6) |
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2.1.1 Band Structure and Effective Mass |
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15 | (2) |
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2.1.2 Heterojunctions and Band Engineering |
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17 | (2) |
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2.1.3 Modulation Doping and Band Diagram |
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19 | (2) |
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2.2 Coherent Transport Devices |
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21 | (6) |
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2.2.1 Shaping the 2D Electron System |
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21 | (2) |
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2.2.2 Mesoscopic Length Scales |
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23 | (2) |
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2.2.3 Approximations to the Hamiltonian |
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25 | (2) |
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2.3 Magnetoelectric Subbands and Transport Channels |
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27 | (5) |
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32 | (5) |
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34 | (3) |
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3 Coherent Electronic Transport: Landauer-Buttiker Formalism |
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37 | (22) |
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37 | (2) |
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3.2 Scattering Matrix and Transmission Function |
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39 | (8) |
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39 | (1) |
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3.2.2 Transmission Amplitudes and Coefficients |
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40 | (3) |
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3.2.3 Connected Scatterers |
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43 | (3) |
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3.2.4 Two-Terminal System |
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46 | (1) |
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3.3 Two-Terminal Landauer Formula |
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47 | (6) |
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3.3.1 General Case of Coherent Transport |
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47 | (3) |
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3.3.2 Linear Response Regime |
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50 | (2) |
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3.3.3 Transmission as Conductance |
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52 | (1) |
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3.4 Multiterminal Conductance |
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53 | (6) |
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3.4.1 Current from Scattering States |
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54 | (1) |
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55 | (1) |
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3.4.3 Current and (Fictitious) Voltage Probes |
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56 | (1) |
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57 | (2) |
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4 Stationary Scattering in Planar Confining Geometries |
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59 | (44) |
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59 | (2) |
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4.2 Greenian Formulation of Scattering |
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61 | (16) |
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61 | (5) |
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4.2.2 Scattering Matrix from Greenian |
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66 | (6) |
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4.2.3 Elements of Formal Scattering Theory |
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72 | (5) |
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4.3 Non-Hermitian Approach to Scattering |
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77 | (13) |
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4.3.1 Decomposition of Configuration Space |
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77 | (2) |
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4.3.2 Effective Scattering Hamiltonian for Finite System |
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79 | (6) |
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4.3.3 Connection to Electronic Transport |
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85 | (5) |
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4.4 Multi-state Interference Effects |
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90 | (13) |
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91 | (4) |
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4.4.2 Aharonov-Bohm Oscillations |
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95 | (3) |
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98 | (5) |
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5 Computational Quantum Transport in Multiterminal and Multiply Connected Structures |
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103 | (46) |
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5.1 Computational Schemes for Quantum Transport |
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103 | (2) |
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5.2 From Operators to Matrices |
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105 | (7) |
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5.2.1 Grid Discretization and Tight-Binding Hamiltonian |
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105 | (6) |
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5.2.2 Dispersion Relation |
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111 | (1) |
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5.3 Scattering via Spatial Decomposition |
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112 | (11) |
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5.3.1 Truncation of the Hamiltonian |
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113 | (4) |
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5.3.2 Open System Propagator |
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117 | (6) |
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5.4 Computation of the Propagator |
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123 | (7) |
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5.4.1 Block-Partitioning of the Hamiltonian |
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123 | (2) |
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5.4.2 Standard Recursive Green Function Method |
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125 | (1) |
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5.4.3 Reordered Block-Gaussian Elimination Scheme |
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126 | (4) |
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5.5 Extended Recursive Green Function Method for Multiterminal, Multiply Connected Structures |
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130 | (8) |
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5.5.1 Modular Partitioning |
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131 | (2) |
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133 | (2) |
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135 | (2) |
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5.5.4 Computational Efficiency and Considerations |
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137 | (1) |
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5.6 Transport Through Multiterminal and Multiply Connected Billiard Systems |
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138 | (11) |
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5.6.1 Single Three-Terminal Elliptic Billiard |
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138 | (4) |
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5.6.2 Transmission and Localization Patterns in a Looped Multiterminal Structure |
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142 | (4) |
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146 | (3) |
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6 Magnetoconductance Switching by Phase Modulation in Arrays of Oval Quantum Billiards |
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149 | (24) |
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6.1 System Setup, Approximations and Computational approach |
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149 | (3) |
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6.2 Single Oval Billiard: Transmission Suppression from Selective Eigenstate Interference |
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152 | (6) |
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6.3 Quantum Dot Array: Composite Resonant States and Magnetically Controlled Transmission Bands |
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158 | (5) |
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6.4 Conductance Switching |
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163 | (4) |
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6.5 The Impact of Impurities |
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167 | (2) |
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6.6 Summary and Conclusions |
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169 | (4) |
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170 | (3) |
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7 Current Control in Soft-Wall Electron Billiards: Energy-Persistent Scattering in the Deep Quantum Regime |
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173 | (20) |
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7.1 Persistent Switching Via Geometric Rescaling at Low Energies |
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173 | (3) |
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7.2 Decoupling of Resonances and Controllable Finite-Temperature Conductance |
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176 | (3) |
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7.3 Closed Billiard Eigenspectrum |
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179 | (3) |
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7.4 Switching Between Collimated and Backscattered Wave Propagation |
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182 | (3) |
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7.5 Conductance Switching in Soft-Wall Billiard Arrays |
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185 | (2) |
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7.6 Billiard Geometry and Soft-Wall Potential Variations |
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187 | (2) |
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7.7 Summary and Conclusions |
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189 | (4) |
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190 | (3) |
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8 Directional Magnetotransport Control in Multiterminal Focusing Quantum Billiards |
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193 | (26) |
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8.1 From Two-terminal to Multiterminal Conductance Control: Directional Coupling by Wave Guiding and Focusing |
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194 | (2) |
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8.2 Setup and Computational Approach |
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196 | (2) |
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8.3 Symmetries of the Transmission Coefficients |
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198 | (2) |
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8.4 Transmission Spectra at Zero Magnetic Field |
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200 | (2) |
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8.5 Geometry Dependent Mean Transmission |
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202 | (5) |
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8.6 Transmission in a Magnetic Field |
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207 | (5) |
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212 | (2) |
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214 | (2) |
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8.9 Summary and Conclusions |
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216 | (3) |
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217 | (2) |
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9 Summary, Conclusions, and Perspectives |
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219 | (6) |
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223 | (2) |
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A Green Functions of Leads |
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225 | (6) |
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A.1 Green Function of an Infinite Quasi-1D Wire |
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225 | (2) |
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A.2 Interface Green Function of a Semi-Infinite Quasi-1D Wire |
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227 | (4) |
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B Block-Matrix Inversion and Schur Complement |
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231 | (6) |
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B.1 Inversion by Block-Gaussian Elimination |
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231 | (3) |
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B.2 Application to Block-Partitioned Lattice Hamiltonian |
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234 | (3) |
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C Inter- and Intra-Connection of Modules |
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237 | (6) |
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C.1 Inter-Connection Between Two Modules |
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237 | (3) |
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C.2 Intra-Connection of a Module |
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240 | (3) |
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D Gauge Transformation of the Greenian |
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243 | (4) |
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D.1 Gauge Transformation of the Green Function Between Two Different Axial Gauges |
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243 | (1) |
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D.2 Gauge Transformation for the Inter-Connection of Two Modules |
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244 | (3) |
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247 | (2) |
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248 | (1) |
Index |
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249 | |