About Motivation and Luck |
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xi | |
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1 | (6) |
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The Stamler Approach: A Brief Historical Overview of the Original Idea |
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1 | (6) |
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7 | (24) |
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The Generalized Metric Dirac Operator |
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7 | (3) |
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Scalar Product in Laplace-Beltrami Form |
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10 | (5) |
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Example: Schwarzschild Metric |
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15 | (1) |
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Transition to the Metric Schrodinger or Covariant Schrodinger Equation |
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16 | (2) |
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18 | (2) |
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Example: The Classical Dirac Equation in the Minkowski Space-Time and Its Extension to Arbitrary Coordinates |
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20 | (4) |
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The Connection to the Einstein Field Equations |
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24 | (1) |
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Summing Up the Recipe: The Forward Derivation |
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25 | (1) |
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Summing Up the Recipe: The Backward Derivation |
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26 | (1) |
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27 | (2) |
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Example: Eigenvalue Solutions for Simple Fields with K(fm) = F(fm)* fm=P*mfm |
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29 | (2) |
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3 The ID Quantum Oscillator in the Metric Picture |
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31 | (24) |
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The Classical Harmonic Quantum Oscillator within the Metric Picture or the Theory of Everything |
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32 | (9) |
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Gaussian-Like Metric Approach |
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41 | (3) |
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44 | (1) |
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Question of Quantizing the Solution |
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45 | (5) |
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50 | (2) |
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Conclusions to the "Einstein Oscillator" |
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52 | (3) |
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4 The Quantized Schwarzschild Metric |
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55 | (12) |
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The Quantization of Time in the Vicinity of a Schwarzschild Object |
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57 | (1) |
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The Quantization of Mass for a Schwarzschild Object |
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58 | (1) |
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The Level Underneath (see also [ 16] or Section "The ID Quantum Oscillator in the Metric Picture") |
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59 | (1) |
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Investigations in Connection with the Speed of Light within the Level Underneath |
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60 | (2) |
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Discussion with Respect to rs(nr)/t(nt) = Clevel2 |
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62 | (1) |
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Discussion with Respect to rend(nr, nt)/t[ nr, nt = Clevel2 |
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63 | (1) |
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How to Evaluate the Speed of Light of the Level Underneath? |
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64 | (1) |
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Conclusions to Quantized Schwarzschild |
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65 | (2) |
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5 Matter-Antimatter Asymmetry |
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67 | (2) |
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Application to Dirac-Schwarzschild Particles at Rest |
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67 | (2) |
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6 Generalization of "The Recipe": From h to the Planck Tensor |
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69 | (30) |
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Generalization to Non-diagonal Metrics |
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69 | (4) |
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Generalization of the "Clever Zero" |
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73 | (1) |
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The Generalized "Vectorial Dirac Root" |
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73 | (4) |
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Examples for Other "Vectorial Dirac Roots" |
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77 | (4) |
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Simple square root with shear component with Ξ(X) = X2 |
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77 | (1) |
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Simple square root with shear component with Ξ(X) = X2 with virtual parameters Ei of various orders of "virtuality" |
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77 | (1) |
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Simple cubic root Ξ(X) = X3 |
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78 | (1) |
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Simple cubic root Ξ(X) = X3 with virtual parameter c |
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79 | (1) |
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Simple quartic root Ξ(X) = X4 |
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79 | (1) |
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Simple quartic root Ξ(X) = X4 with virtual parameter c |
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80 | (1) |
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Extension/Generalization to Arbitrary Functional Approaches for K(fn) |
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81 | (1) |
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81 | (1) |
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Extension/Generalization to Arbitrary Derivative Approaches: The Generalized Gradient of fn |
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82 | (1) |
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Extension/Generalization to Higher-Order Planck Tensors |
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83 | (1) |
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Summing Up the Generalized Recipe: The Forward Derivation |
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84 | (1) |
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Summing Up the Generalized Recipe: The Backward Derivation |
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85 | (1) |
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Backward Example: The Higgs Field Revisited (Extended Consideration from [ 15]) |
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86 | (8) |
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Forward Example: The Harmonic Oscillator and Eigenvalue Solutions for Simple Fields with k(fm) = F(fm)*fm = p*mfm Revisited (Extended Consideration from [ 10]) |
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94 | (3) |
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Conclusions to "Generalization of the Recipe" |
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97 | (2) |
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7 About Fermat's Last Theorem |
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99 | (4) |
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99 | (1) |
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100 | (1) |
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100 | (1) |
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101 | (2) |
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8 Dirac Quantization of the Kerr Metric |
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103 | (12) |
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The Generalized Metric Dirac Operator for a Kerr Object "at Rest" |
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103 | (3) |
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Further Results and Trials |
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106 | (3) |
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The Spatial Appearance of the Leptons |
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109 | (2) |
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Conclusions to the Quantized Schwarzschild and Kerr Objects |
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111 | (4) |
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115 | (34) |
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115 | (4) |
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119 | (2) |
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The Other Way to Fulfill the Maxwell Equations with Plane Waves |
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121 | (1) |
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122 | (1) |
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Spatial Extension of the Solution and the Localized Photon |
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123 | (5) |
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Localizing the Photon Forces It to Evolve Spin |
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128 | (2) |
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Option A Leading to Magnetic Charges |
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130 | (1) |
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Option B Leading to Magnetic Displacement Current Density |
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131 | (1) |
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Option C Finding the Correct Metric, a Yet Unsolved Problem |
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132 | (5) |
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Suspicion about Connections to Compactified Coordinates |
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137 | (3) |
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The Alternative Interpretation Using Real and Imaginary Part |
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140 | (3) |
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Further Illustrations and a Few Words about the Absence of Magnetic Monopoles in Our Observable Universe |
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143 | (3) |
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The Total Spatial Displacement for the Photon |
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146 | (2) |
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Conclusions to the Photon |
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148 | (1) |
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10 How the Quantum Theory Already Resides in the Einstein-Hilbert Action |
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149 | (46) |
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Theory: The Discarded Term |
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149 | (8) |
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157 | (2) |
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The Harmonic Quantum Oscillator in ID in the Metric Picture |
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159 | (5) |
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The Three-Dimensional Case |
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164 | (6) |
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Connection with the Technique of the "Intelligent Zero" of a Line Element |
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170 | (2) |
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Theory: The Conjecture 8Rap = Matter & Energy and the Extended-Einstein Field Equations |
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172 | (1) |
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Most Symmetric and Isotropic Virtual Matter Solutions in 2D, 3D, and 4D |
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173 | (1) |
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Four Most Simple Solutions for the Whole Thing in 4D: The Matter and Antimatter Asymmetry and Why Time is Different |
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174 | (2) |
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176 | (1) |
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Intermediate Result: The n-Dimensional Case |
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176 | (1) |
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177 | (1) |
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An Adapted Schwarzschild Solution |
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178 | (3) |
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Eigenequations Derived from δRαβ for Shear-Free Metrics |
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181 | (6) |
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182 | (2) |
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184 | (1) |
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185 | (2) |
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187 | (1) |
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187 | (5) |
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187 | (1) |
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188 | (1) |
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189 | (1) |
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Summing the Last Section Up |
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189 | (3) |
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Example: Symmetry of Revolution |
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192 | (3) |
References |
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195 | (4) |
Index |
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199 | |