Preface |
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1 | (5) |
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5 | (18) |
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Scaling and Dimensional Analysis |
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5 | (2) |
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Power Laws in Statistical Physics |
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7 | (3) |
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Liquid Gas Critical Point |
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7 | (2) |
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9 | (2) |
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Superfluid Transition in 4He |
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11 | (1) |
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12 | (1) |
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Dynamic Critical Phenomena |
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13 | |
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10 | (4) |
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14 | (9) |
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20 | (3) |
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How Phase Transitions Occur In Principle |
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23 | (62) |
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Review of Statistical Mechanics |
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23 | (2) |
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25 | (4) |
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Thermodynamic Limit in a Charged System |
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26 | (1) |
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Thermodynamic Limit for Power Law Interactions |
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27 | (2) |
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Phase Boundaries and Phase Transitions |
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29 | (3) |
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Ambiguity in the Definition of Phase Boundary |
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29 | (1) |
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Types of Phase Transition |
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30 | (1) |
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Finite Size Effects and the Correlation Length |
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30 | (2) |
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32 | (1) |
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33 | (2) |
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Analytic Properties of the Ising Model |
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35 | (5) |
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38 | (1) |
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Convexity and the Free Energy Density |
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38 | (2) |
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Symmetry Properties of the Ising Model |
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40 | (3) |
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40 | (1) |
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41 | (2) |
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Existence of Phase Transitions |
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43 | (7) |
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Zero Temperature Phase Diagram |
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44 | (1) |
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Phase Diagram at Non-Zero Temperature: d = 1 |
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45 | (2) |
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Phase Diagram at Non-Zero Temperature: d = 2 |
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47 | (2) |
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Impossibility of Phase Transitions |
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49 | (1) |
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Spontaneous Symmetry Breaking |
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50 | (5) |
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52 | (2) |
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54 | (1) |
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55 | (16) |
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57 | (2) |
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Symmetry and Its Implications for Ergodicity Breaking |
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59 | (3) |
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Example of Replica Symmetry Breaking: Rubber |
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62 | (3) |
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Order Parameters and Overlaps in a Classical Spin Glass |
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65 | (3) |
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Replica Formalism for Constrained Systems |
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68 | (3) |
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71 | (3) |
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74 | (5) |
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Lattice Gas Thermodynamics from the Ising Model |
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75 | (2) |
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Derivation of Lattice Gas Model from the Configurational Sum |
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77 | (2) |
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Equivalence in Statistical Mechanics |
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79 | (1) |
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80 | (5) |
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History of the Thermodynamic Limit |
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80 | (1) |
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Do Quantum Effects Matter? |
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81 | (1) |
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82 | (3) |
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How Phase Transitions Occur in Practice |
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85 | (32) |
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85 | (3) |
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Free Boundary Conditions and H = 0 |
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86 | (1) |
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Periodic Boundary Conditios and H = 0 |
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86 | (1) |
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Recursion Method for H = 0 |
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87 | (1) |
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Effect of Boundary Conditions |
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88 | (1) |
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88 | (3) |
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91 | (1) |
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92 | (3) |
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95 | (6) |
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Zero Field: Ad Hoc Method |
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95 | (3) |
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Existence of Long Range Order |
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98 | (1) |
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99 | (2) |
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Low Temperature Expansion |
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101 | (3) |
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103 | (1) |
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103 | (1) |
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104 | (13) |
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105 | (3) |
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108 | (3) |
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How Good Is Mean Field Theory? |
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111 | (1) |
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112 | (5) |
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Critical Phenomena in Fluids |
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117 | (18) |
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117 | (2) |
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117 | (1) |
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118 | (1) |
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Landau's Symmetry Principle |
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119 | (1) |
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119 | (3) |
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Fluid at Constant Pressure |
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119 | (1) |
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Fluid at Constant Temperature |
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120 | (1) |
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Maxwell's Equal Area Rule |
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121 | (1) |
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Vicinity of the Critical Point |
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122 | (1) |
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123 | (5) |
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Determination of the Critical Point |
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123 | (1) |
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Law of Corresponding States |
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124 | (1) |
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125 | (3) |
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128 | (3) |
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Number Fluctuations and Compressibility |
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128 | (1) |
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Number Fluctuations and Correlations |
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129 | (1) |
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130 | (1) |
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Measurement of Critical Exponents |
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131 | (4) |
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Definition of Critical Exponents |
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131 | (1) |
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Determination of Critical Exponents |
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132 | (2) |
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134 | (1) |
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135 | (32) |
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136 | (2) |
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136 | (1) |
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137 | (1) |
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137 | (1) |
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Common Features of Mean Field Theories |
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138 | (1) |
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Phenomenological Landau Theory |
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139 | (4) |
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140 | (1) |
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141 | (2) |
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Continuous Phase Transitions |
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143 | (2) |
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Critical Exponents in Landau Theory |
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144 | (1) |
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145 | (2) |
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147 | (7) |
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147 | (2) |
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Interpretation of the Landau Free Energy |
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149 | (5) |
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154 | (13) |
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154 | (1) |
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Functional Integrals in Real and Fourier Space |
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154 | (2) |
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Functional Differentiation |
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156 | (1) |
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157 | (1) |
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Calculation of Two-Point Correlation Function |
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158 | (4) |
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162 | (1) |
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163 | (4) |
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Fluctuations and the Breakdown of Landau Theory |
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167 | (22) |
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Breakdown of Microscopic Landau Theory |
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167 | (2) |
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Fluctuations Away from the Critical Point |
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168 | (1) |
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Fluctuations Near the Critical Point |
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169 | (1) |
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Breakdown of Phenomenological Landau Theory |
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169 | (5) |
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Calculation of the Ginzburg Criterion |
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170 | (2) |
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Size of the Critical Region |
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172 | (2) |
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The Gaussian Approximation |
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174 | (7) |
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174 | (1) |
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175 | (1) |
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Infinite Number of Degrees of Freedom |
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176 | (3) |
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Two-Point Correlation Function Revisited |
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179 | (2) |
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181 | (8) |
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185 | (4) |
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189 | (12) |
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Dimensional Analysis of Landau Theory |
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189 | (4) |
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Dimensional Analysis and Critical Exponents |
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193 | (3) |
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Anomalous Dimensions and Asymtotics |
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196 | (1) |
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Renormalisation and Anomalous Dimensions |
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197 | (4) |
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199 | (2) |
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Scaling in Static, Dynamic and Non-Equilibrium Phenomena |
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201 | (28) |
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The Static Scaling Hypothesis |
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202 | (4) |
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204 | (1) |
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204 | (1) |
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The Zero-field Susceptibility |
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204 | (1) |
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The Critical Isotherm and a Scaling Law |
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205 | (1) |
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Other Forms of the Scalling Hypothesis |
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206 | (3) |
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Scaling Hypothesis for the Free Energy |
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206 | (1) |
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Scaling Hypothesis for the Correlation Function |
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206 | (1) |
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Scaling and the Correlation Length |
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207 | (2) |
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Dynamic Critical Phenomena |
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209 | (7) |
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Small Time-Dependent Fluctuations |
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209 | (2) |
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211 | (2) |
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Dynamic Scaling Hypothesis for Relaxation Times |
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213 | (1) |
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Dynamic Scaling Hypothesis for the Response Function |
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214 | (1) |
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Scaling of the Non-linear Response |
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214 | (2) |
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Scaling in the Approach to Equilibrium |
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216 | (10) |
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Growth of a Fluctuating Surface |
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217 | (2) |
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Spinodal Decomposition in Alloys and Block Copolymers |
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219 | (7) |
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226 | (3) |
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Appendix 8 The Fokker-Planck Equation |
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226 | (3) |
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The Renormalisation Group |
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229 | (58) |
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230 | (6) |
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230 | (4) |
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234 | (1) |
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235 | (1) |
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Basic Ideas of the Renormalisation Group |
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236 | (6) |
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Properties of Renormalisation Group Transformations |
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236 | (4) |
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The Origin of Singular Behaviour |
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240 | (2) |
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242 | (7) |
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Physical Significance of Fixed Points |
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242 | (1) |
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Local Behaviour of RG Flows Near a Fixed Point |
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243 | (3) |
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Global Properties of RG Flows |
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246 | (3) |
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249 | (7) |
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249 | (3) |
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Diagonal RG Transformation for Two Relevant Variables |
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252 | (2) |
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254 | (1) |
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Non-diagonal RG Transformations |
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255 | (1) |
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256 | (1) |
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RG for the Two Dimensional Ising Model |
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257 | (11) |
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Exact Calculation of Eigenvalues from Onsager's Solution |
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258 | (1) |
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Formal Representation of the Coarse-Grained Hamiltonian |
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259 | (1) |
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Perturbation Theory for the RG Recursion Relation |
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260 | (3) |
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Fixed Points and Critical Exponents |
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263 | (1) |
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264 | (1) |
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265 | (2) |
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267 | (1) |
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First Order Transitions and Non-Critical Properties |
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268 | (2) |
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RG for the Correlation Function |
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270 | (1) |
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271 | (7) |
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271 | (2) |
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Crossover Arising from Anisotropy |
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273 | (3) |
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Crossover and Disorder: the Harris Criterion |
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276 | (2) |
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278 | (1) |
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279 | (8) |
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283 | (4) |
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Anomalous Dimensions Far From Equilibrium |
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287 | (48) |
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287 | (2) |
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289 | (4) |
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Long Time Behaviour of the Diffusion Equation |
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289 | (1) |
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Dimensional Analysis of the Diffusion Equation |
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290 | (1) |
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Intermediate Asymptotics of the First Kind |
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291 | (2) |
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Anomalous Dimensions in Similarity Solutions |
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293 | (9) |
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The Modified Porous Medium Equation |
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293 | (3) |
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Dimensional Analysis for Barenblatt's Equation |
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296 | (2) |
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Similarity Solution with an Anomalous Dimension |
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298 | (3) |
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Intermediate Asymptotics of the Second Kind |
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301 | (1) |
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302 | (16) |
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Renormalisation and its Physical Interpretation |
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303 | (2) |
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Heuristic Calculation of the Anomalous Dimension α |
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305 | (1) |
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Renormalisation and Dimensional Analysis |
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306 | (3) |
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Removal of Divergences and the RG |
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309 | (4) |
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Assumption of Renormalisability |
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313 | (1) |
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Renormalisation and Physical Theory |
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314 | (2) |
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Renormalisation of the Modified Porous Medium Equation |
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316 | (2) |
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Perturbation Theory for Barenblatt's Equation |
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318 | (7) |
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318 | (1) |
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319 | (1) |
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320 | (1) |
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Isolation of the Divergence |
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320 | (2) |
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Perturbative Renormalisation |
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322 | (2) |
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Renormalised Perturbation Expansion |
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324 | (1) |
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Origin of Divergence of Perturbation Theory |
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325 | (1) |
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325 | (3) |
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Similarity Solutions as Fixed Points |
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326 | (2) |
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Universality in the Approach to Equilibrium |
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328 | (1) |
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328 | (7) |
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Appendix 10 Method of Characteristics |
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329 | (3) |
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332 | (3) |
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335 | (16) |
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Correlation in the Ordered Phase |
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336 | (9) |
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The Susceptibility Tensor |
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337 | (2) |
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Excitations for T < Tc: Goldstone's Theorem |
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339 | (4) |
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Emergence of Order Parameter Rigidity |
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343 | (1) |
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344 | (1) |
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344 | (1) |
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Kosterlitz-Thouless Transition |
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345 | (6) |
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345 | (1) |
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346 | (2) |
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348 | (2) |
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Universal Jump in the Stiffness |
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350 | (1) |
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Critical Phenomena Near Four Dimensions |
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351 | (38) |
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Basic Idea of the Epsilon Expansion |
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353 | (1) |
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RG for the Gaussian Model |
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354 | (7) |
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Integrating Out the Short Wavelength Degrees of Freedom |
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355 | (2) |
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Rescaling of Fields and Momenta |
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357 | (1) |
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Analysis of Recursion Relation |
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357 | (1) |
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358 | (1) |
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A Dangerous Irrelevant Variable in Landau Theory |
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359 | (2) |
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RG Beyond the Gaussian Approximation |
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361 | (9) |
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Setting Up Perturbation Theory |
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362 | (3) |
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Calculation of 〈V〉0: Strategy |
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365 | (1) |
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Correlation Functions of σl: Wick's Theorem |
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366 | (2) |
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368 | (2) |
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370 | (7) |
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370 | (3) |
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Feynman Diagrams for 〈V2〉0 - 〈V〉20 |
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373 | (3) |
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Elimination of Unnecessary Diagrams |
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376 | (1) |
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The RG Recursion Relations |
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377 | (7) |
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Feynman Diagrams for Small ε = 4 - d |
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378 | (2) |
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Recursion Relations to O(ε) |
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380 | (1) |
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Fixed Points to O(ε) |
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381 | (1) |
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382 | (2) |
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384 | (5) |
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Appendix 12 The Linked Cluster Theorem |
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385 | (1) |
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386 | (3) |
Index |
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389 | |