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1 Strongly Interacting Matter in Magnetic Fields: A Guide to This Volume |
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1 | (12) |
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1 | (1) |
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1.2 Chiral Magnetic Effect and Anomaly-Induced Transport |
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2 | (3) |
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1.3 Phase Structure in a Magnetic Field |
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5 | (8) |
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1.3.1 Phases of QCD in a Magnetic Field |
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5 | (3) |
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1.3.2 Condensed Matter Systems in a Magnetic Field via AdS/CFT |
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8 | (3) |
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11 | (2) |
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2 Magnetic Catalysis: A Review |
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13 | (38) |
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13 | (2) |
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2.2 The Essence of Magnetic Catalysis |
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15 | (14) |
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2.2.1 Dimensional Reduction in a Magnetic Field |
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15 | (4) |
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2.2.2 Magnetic Catalysis in 2 + 1 Dimensions |
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19 | (3) |
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2.2.3 Magnetic Catalysis in 3 + 1 Dimensions |
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22 | (1) |
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2.2.4 Symmetry Breaking as Bound State Problem |
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23 | (3) |
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2.2.5 Analogy with Superconductivity |
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26 | (1) |
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2.2.6 Bound States in Lower Dimensions |
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27 | (2) |
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2.3 Magnetic Catalysis in Gauge Theories |
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29 | (8) |
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2.3.1 Magnetic Catalysis in QED |
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29 | (2) |
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2.3.2 Magnetic Catalysis in QCD |
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31 | (2) |
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2.3.3 Magnetic Catalysis in Graphene |
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33 | (4) |
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37 | (14) |
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Appendix Fermion Propagator in a Magnetic Field |
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38 | (3) |
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41 | (10) |
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3 Inverse Magnetic Catalysis in Field Theory and Gauge-Gravity Duality |
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51 | (36) |
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51 | (3) |
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3.2 Chiral Phase Transition in the Nambu-Jona-Lasinio Model |
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54 | (13) |
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3.2.1 Chiral Symmetry Breaking Without External Fields |
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55 | (4) |
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3.2.2 Chiral Symmetry Breaking in the Presence of a Magnetic Field |
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59 | (8) |
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3.3 Chiral Phase Transition in the Sakai-Sugimoto Model |
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67 | (15) |
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3.3.1 Introducing the Model |
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67 | (4) |
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3.3.2 Equations of Motion and Axial Current |
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71 | (2) |
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3.3.3 Semianalytic Solution to the Equations of Motion |
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73 | (2) |
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3.3.4 Broken Chiral Symmetry |
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75 | (1) |
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76 | (2) |
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3.3.6 Chiral Phase Transition |
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78 | (4) |
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82 | (5) |
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83 | (4) |
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4 Quark Matter in a Strong Magnetic Background |
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87 | (34) |
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87 | (2) |
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4.2 The PNJL Model with a Magnetic Background |
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89 | (4) |
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4.2.1 The One-Loop Quark Propagator |
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90 | (2) |
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4.2.2 The One-Loop Thermodynamic Potential |
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92 | (1) |
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93 | (7) |
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4.3.1 Condensates and Dressed Polyakov Loop |
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94 | (3) |
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4.3.2 Entanglement of NJL Coupling and Polyakov Loop |
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97 | (3) |
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4.4 Phase Diagram in the eB-T Plane |
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100 | (2) |
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4.4.1 Comparison with Other Computations |
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101 | (1) |
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4.5 Polarization of the Quark Condensate |
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102 | (12) |
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4.5.1 Non-renormalized Quark-Meson Model Results |
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105 | (4) |
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4.5.2 Results Within the Renormalized QM Model |
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109 | (5) |
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114 | (7) |
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116 | (5) |
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5 Thermal Chiral and Deconfining Transitions in the Presence of a Magnetic Background |
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121 | (22) |
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121 | (2) |
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5.2 Modified Dispersion Relations and Integral Measures |
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123 | (2) |
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5.3 PLSMq Effective Model and the Splitting of the Chiral and Deconfining Transition Lines |
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125 | (6) |
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5.4 Magbag--The Thermal MIT Bag Model in the Presence of a Magnetic Background |
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131 | (4) |
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135 | (2) |
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5.6 Conclusions and Perspectives |
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137 | (6) |
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138 | (5) |
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6 Electromagnetic Superconductivity of Vacuum Induced by Strong Magnetic Field |
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143 | (38) |
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143 | (1) |
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6.2 Conventional Superconductivity, Vacuum Superconductivity and Schwinger Pair Creation: Differences and Similarities |
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144 | (9) |
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6.2.1 Conventional Superconductivity via Formation of Cooper Pairs |
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144 | (2) |
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6.2.2 Vacuum Superconductivity |
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146 | (7) |
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6.3 Ground State of Vacuum Superconductor |
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153 | (24) |
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6.3.1 Energetic Favorability of the Superconducting State |
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153 | (2) |
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6.3.2 Approaches: Ginzburg-Landau vs Bardeen-Cooper-Schrieffer |
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155 | (1) |
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6.3.3 Example: Ginzburg-Landau Model |
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156 | (5) |
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6.3.4 Superconductivity of Vacuum in Strong Magnetic Field |
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161 | (11) |
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6.3.5 Superconductivity of Vacuum in Nambu-Jona-Lasinio Model |
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172 | (5) |
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177 | (4) |
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178 | (3) |
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7 Lattice QCD Simulations in External Background Fields |
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181 | (28) |
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181 | (2) |
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7.2 Background Fields on the Lattice |
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183 | (7) |
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7.2.1 Electromagnetic Fields |
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183 | (6) |
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7.2.2 Chromomagnetic Background Fields |
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189 | (1) |
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7.3 Vacuum Properties in Background Fields: Magnetic Catalysis |
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190 | (4) |
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7.4 QCD Phase Diagram in External Fields |
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194 | (7) |
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7.4.1 Deconfinement Transition in a Strong Magnetic Background |
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195 | (4) |
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7.4.2 Deconfinement Transition in a Chromomagnetic Background |
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199 | (2) |
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7.5 More on Gauge Field Modifications in External Electromagnetic Fields |
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201 | (4) |
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205 | (4) |
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206 | (3) |
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8 P-Odd Fluctuations in Heavy Ion Collisions. Deformed QCD as a Toy Model |
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209 | (32) |
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8.1 Introduction and Motivation |
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209 | (2) |
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8.2 Quantum Anomalies. Effective Lagrangian Approach |
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211 | (5) |
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8.2.1 Charge Separation Effect (CSE) |
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211 | (1) |
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8.2.2 Chiral Magnetic Effect (CME) |
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212 | (1) |
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8.2.3 Chiral Vortical Effect (CVE) |
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213 | (3) |
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8.3 Long Range Order as Seen on the Lattice |
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216 | (2) |
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218 | (4) |
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8.4.1 Formulation of the Theory |
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218 | (1) |
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8.4.2 Infrared Description |
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219 | (3) |
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8.5 Domain Walls in Deformed QCD |
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222 | (5) |
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8.5.1 Domain Wall Solution |
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223 | (2) |
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8.5.2 Double Layer Structure |
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225 | (2) |
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8.6 DW in the Presence of Matter Field |
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227 | (4) |
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8.7 CSE, CME, CVE and Related Topological Phenomena in Deformed QCD |
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231 | (4) |
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8.8 Conclusion and Future Directions |
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235 | (6) |
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237 | (2) |
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239 | (2) |
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9 Views of the Chiral Magnetic Effect |
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241 | (20) |
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9.1 Introduction--Discovery of the Chiral Magnetic Effect |
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241 | (4) |
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9.2 Chiral Separation Effect |
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245 | (4) |
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9.3 What Is the Chiral Chemical Potential? |
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249 | (2) |
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251 | (5) |
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256 | (5) |
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257 | (4) |
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10 The Chiral Magnetic Effect and Axial Anomalies |
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261 | (34) |
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10.1 Dirac Operators, Dimensional Reduction and Axial Anomalies |
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261 | (9) |
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10.1.1 Lowest Landau Level Projection |
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261 | (2) |
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10.1.2 Schur Decomposition of Dirac Propagator |
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263 | (2) |
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10.1.3 Currents and Anomalies in the Lowest Landau Level Projection |
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265 | (2) |
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10.1.4 Chiral Magnetic Effect and the Schwinger Effect |
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267 | (1) |
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10.1.5 Maxwell-Chern-Simons Theory and the Schwinger Model |
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268 | (2) |
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10.2 Chiral Magnetic Spiral |
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270 | (6) |
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10.2.1 Basic Setup and Dimensional Reduction |
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271 | (2) |
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10.2.2 Life in Two-Dimensions |
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273 | (3) |
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10.3 Fermions in an Instanton and Magnetic Field Background |
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276 | (14) |
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10.3.1 Euclidean Dirac Operator |
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277 | (2) |
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10.3.2 Magnetic Field Background |
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279 | (1) |
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10.3.3 Instanton Background |
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280 | (1) |
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10.3.4 Combined Instanton and Magnetic Field Background |
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281 | (2) |
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10.3.5 Large Instanton Limit: Covariantly Constant SU(2) Instanton and Constant Abelian Magnetic Field |
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283 | (2) |
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10.3.6 Dirac Spectrum in the Strong Magnetic Field Limit |
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285 | (2) |
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10.3.7 Physical Picture: Competition Between Spin and Chirality Projection |
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287 | (1) |
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10.3.8 Matrix Elements and Dipole Moments |
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287 | (3) |
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290 | (5) |
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291 | (4) |
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11 Chiral Magnetic Effect in Hydrodynamic Approximation |
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295 | (36) |
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295 | (6) |
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11.2 Non-renormalization Theorems |
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301 | (13) |
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11.2.1 Non-renormalization Theorems in Thermodynamic Approach |
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301 | (3) |
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11.2.2 Non-renormalization Theorems in Geometric Approach |
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304 | (4) |
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11.2.3 Non-renormalization Theorems in Diagrammatic Approach |
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308 | (3) |
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11.2.4 Non-renormalization Theorems in Effective Field Theories |
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311 | (3) |
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11.2.5 Concluding Remarks |
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314 | (1) |
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11.3 Hydrodynamic Chiral Effects as Quantum Phenomena |
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314 | (9) |
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11.3.1 Non-dissipative Currents |
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314 | (2) |
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11.3.2 Low-Dimensional Defects |
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316 | (1) |
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11.3.3 Relativistic Superfluidity |
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317 | (3) |
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320 | (2) |
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11.3.5 Concluding Remarks |
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322 | (1) |
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323 | (8) |
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327 | (4) |
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12 Remarks on Decay of Defects with Internal Degrees of Freedom |
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331 | (10) |
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331 | (1) |
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12.2 Decay of Axion-Like Domain Walls in D = 3 + 1 Theories |
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332 | (3) |
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12.3 Decays of Mesonic Walls |
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335 | (2) |
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12.3.1 Decay of π0 Domain Walls |
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335 | (1) |
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12.3.2 Wall Decay in QCD at High Density |
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336 | (1) |
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12.4 Nonabelian String Decay |
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337 | (1) |
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338 | (3) |
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339 | (2) |
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13 A Chiral Magnetic Effect from AdS/CFT with Flavor |
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341 | (36) |
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341 | (4) |
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13.2 The Theory in Question |
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345 | (4) |
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13.3 Chiral Magnetic Effect from Spinning Probe Branes |
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349 | (17) |
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13.3.1 Solutions at Zero Temperature |
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356 | (6) |
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13.3.2 Solutions at Finite Temperature |
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362 | (4) |
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13.4 Loss Rates of Axial Charge and of Energy |
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366 | (4) |
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13.5 Summary and Discussion |
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370 | (7) |
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373 | (4) |
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14 Lattice Studies of Magnetic Phenomena in Heavy-Ion Collisions |
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377 | (10) |
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377 | (1) |
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14.2 Chiral Magnetic Effect |
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378 | (4) |
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14.3 Induced Conductivity and Abnormal Dilepton Yield |
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382 | (2) |
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384 | (3) |
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384 | (3) |
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15 Chiral Magnetic Effect on the Lattice |
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387 | (12) |
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387 | (1) |
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15.2 Basics of the Lattice Simulation |
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388 | (2) |
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15.3 Lattice Simulation with a Topological Background |
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390 | (3) |
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15.4 Lattice Simulation with a Chiral Chemical Potential |
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393 | (3) |
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396 | (3) |
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397 | (2) |
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16 Magnetism in Dense Quark Matter |
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399 | (34) |
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399 | (1) |
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16.2 Magnetic Fields in Compact Stars |
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399 | (2) |
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16.3 Magnetism in Spin-Zero Color Superconductivity |
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401 | (1) |
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16.4 The Magnetic CFL Phase |
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402 | (6) |
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16.5 Magnetoelectric Effect in Cold-Dense Matter |
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408 | (5) |
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16.6 Paramagnetism in Color Superconductivity |
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413 | (3) |
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16.7 Magnetic Phases in CFL Matter |
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416 | (1) |
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16.8 Equation of State of the MCFL Phase |
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417 | (7) |
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16.8.1 Covariant Structure of the Energy-Momentum Tensor in a Magnetized System |
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419 | (2) |
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16.8.2 MCFL Thermodynamic Potential |
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421 | (1) |
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16.8.3 EoS in a Magnetic Field |
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422 | (2) |
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16.9 Astrophysical Implications |
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424 | (9) |
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16.9.1 Low-Energy Physics |
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424 | (2) |
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16.9.2 Boosting Stellar Magnetic Fields via an Internal Mechanism |
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426 | (1) |
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16.9.3 Stability of Magnetized Quark Stars |
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427 | (2) |
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429 | (4) |
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17 Anomalous Transport from Kubo Formulae |
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433 | (36) |
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433 | (3) |
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17.2 Anomalies and Hydrodynamics |
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436 | (14) |
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436 | (4) |
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17.2.2 Chemical Potentials for Anomalous Symmetries |
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440 | (7) |
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17.2.3 Contributions to the Kubo Formulae |
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447 | (3) |
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450 | (7) |
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17.3.1 Chiral Vortical Conductivity |
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451 | (3) |
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17.3.2 Chiral Magnetic Conductivity |
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454 | (1) |
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17.3.3 Conductivities for the Energy Flux |
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455 | (1) |
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17.3.4 Summary and Specialization to the Group U(1)v x U(1)A |
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456 | (1) |
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457 | (7) |
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17.4.1 Notation and Holographic Anomalies |
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457 | (2) |
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17.4.2 Applying Kubo Formulae and Linear Response |
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459 | (5) |
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17.5 Conclusion and Outlook |
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464 | (5) |
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Appendix 1 Boundary Counterterms |
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465 | (1) |
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Appendix 2 Equations of Motion for the Shear Sector |
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466 | (1) |
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466 | (3) |
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18 Quantum Criticality via Magnetic Branes |
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469 | (34) |
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469 | (2) |
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18.2 Basic Gauge Theory Dynamics |
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471 | (2) |
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18.2.1 Effective Low Energy Degrees of Freedom |
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471 | (1) |
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472 | (1) |
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18.3 Holographic Dual Set-Up |
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473 | (2) |
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18.3.1 Field Equations and Structure of the Solutions |
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474 | (1) |
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18.3.2 Boundary Stress Tensor and Current |
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475 | (1) |
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18.4 The Purely Magnetic Brane: Zero Charge Density |
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475 | (7) |
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18.4.1 The Purely Magnetic Brane at T = 0 |
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475 | (1) |
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18.4.2 RG Flow and Thermodynamics |
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476 | (2) |
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18.4.3 Calculation of Current-Current Correlators at T = 0 |
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478 | (1) |
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18.4.4 Method of Overlapping Expansions |
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479 | (1) |
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18.4.5 Current Two-Point Correlators |
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480 | (1) |
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18.4.6 Maxwell-Chern-Simons Holography in AdS3 |
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480 | (1) |
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18.4.7 Effective Conformal Field Theory and Double-Trace Operators |
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481 | (1) |
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18.4.8 Stress Tensor Correlators and Emergent Virasoro Symmetry |
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482 | (1) |
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18.5 Holographic Dual Solutions for Non-zero Charge Density |
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482 | (10) |
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18.5.1 Reduced Field Equations |
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483 | (1) |
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18.5.2 Near-Horizon Schrodinger Geometry |
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484 | (1) |
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18.5.3 The Charged Magnetic Brane Solution |
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484 | (1) |
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18.5.4 Regularity of the Solutions |
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485 | (1) |
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18.5.5 Existence of a Critical Magnetic Field |
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486 | (1) |
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18.5.6 Low T Thermodynamics for B > Bc |
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487 | (1) |
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18.5.7 Low T Thermodynamics for B = Bc |
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488 | (1) |
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18.5.8 Scaling Function in the Quantum Critical Region |
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489 | (1) |
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18.5.9 Numerical Completion of the Holographic Phase Diagram |
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490 | (1) |
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18.5.10 Correlators at Non-zero Charge Density |
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491 | (1) |
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18.5.11 Comments on Stability |
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492 | (1) |
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18.6 Quantum Criticality in 2 + 1 Dimensions |
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492 | (5) |
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18.6.1 Field Equations and Structure of the Solutions |
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493 | (1) |
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18.6.2 Horizon and Asymptotic Data, Physical Quantities |
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494 | (1) |
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18.6.3 Flows Towards the Electric IR Fixed Point |
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495 | (1) |
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18.6.4 Flows Towards the Magnetic IR Fixed Point |
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495 | (1) |
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18.6.5 Flows Towards the Lifshitz IR Fixed Point |
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496 | (1) |
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18.6.6 The Full Phase Diagram |
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496 | (1) |
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18.7 Relation with Quantum Criticality in Condensed Matter |
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497 | (6) |
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18.7.1 Meta-Magnetic Transitions in Strontium Ruthenates |
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497 | (2) |
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18.7.2 Relation to Hertz-Millis Theory |
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499 | (1) |
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500 | (3) |
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19 Charge-Dependent Correlations in Relativistic Heavy Ion Collisions and the Chiral Magnetic Effect |
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503 | (34) |
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503 | (4) |
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19.1.1 The Chiral Magnetic Effect in Brief |
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504 | (1) |
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19.1.2 Hunting for the CME in Heavy Ion Collisions |
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505 | (2) |
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19.2 The Charge-Dependent Correlation Measurements |
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507 | (9) |
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19.2.1 General Considerations Concerning Azimuthal Correlation Measurements |
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508 | (3) |
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19.2.2 Measuring the Charge Separation Through Azimuthal Correlations |
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511 | (3) |
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19.2.3 The Qc1 Vector Analysis for Measuring the Charge Separation |
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514 | (2) |
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19.3 Interpretation of the Available Data |
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516 | (4) |
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19.4 Discussion of Various Background Contributions |
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520 | (13) |
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521 | (2) |
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19.4.2 Transverse Momentum Conservation |
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523 | (3) |
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526 | (2) |
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19.4.4 Local Charge Conservation |
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528 | (1) |
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19.4.5 Decomposition of Flow-Induced and Flow-Independent Contributions |
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529 | (3) |
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19.4.6 Suppression of Elliptic-Flow-Induced Correlations |
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532 | (1) |
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19.5 Summary and Conclusions |
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533 | (4) |
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534 | (3) |
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20 Holography, Fractionalization and Magnetic Fields |
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537 | (18) |
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20.1 Charged Ideal Fluid with a Magnetic Field |
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540 | (6) |
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20.1.1 Gravity Background |
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540 | (3) |
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20.1.2 Density of States for (3 + 1)-Dimensional Fermions in a Magnetic Field |
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543 | (2) |
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20.1.3 Action Calculation |
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545 | (1) |
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20.2 The Role of the Dilaton |
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546 | (3) |
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20.3 Solutions with Stars |
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549 | (2) |
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20.3.1 Mesonic Phase: Star in the Infra-Red |
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549 | (1) |
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20.3.2 Partially Fractionalized Phases: Star Outside Horizon |
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550 | (1) |
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551 | (4) |
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552 | (3) |
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21 Holographic Description of Strongly Correlated Electrons in External Magnetic Fields |
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555 | (36) |
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555 | (4) |
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21.2 Holographic Fermions in a Dyonic Black Hole |
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559 | (5) |
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559 | (3) |
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21.2.2 Holographic Fermions |
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562 | (2) |
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21.3 Magnetic Fields and Conformal Invariance |
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564 | (2) |
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21.3.1 The Near-Horizon Limit and Dirac Equation in AdS2 |
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564 | (2) |
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566 | (6) |
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21.4.1 Relating to the ARPES Measurements |
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566 | (2) |
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21.4.2 Magnetic Crossover and Disappearance of the Quasiparticles |
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568 | (1) |
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569 | (3) |
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21.5 Fermi Level Structure at Zero Temperature |
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572 | (8) |
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21.5.1 Dirac Equation with m = 0 |
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572 | (3) |
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21.5.2 Magnetic Effects on the Fermi Momentum and Fermi Velocity |
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575 | (5) |
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21.6 Hall and Longitudinal Conductivities |
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580 | (6) |
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21.6.1 Integer Quantum Hall Effect |
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|
581 | (4) |
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21.6.2 Fractional Quantum Hall Effect |
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585 | (1) |
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586 | (5) |
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588 | (3) |
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22 A Review of Magnetic Phenomena in Probe-Brane Holographic Matter |
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591 | |
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591 | (2) |
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593 | (8) |
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22.2.1 Brane Construction |
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593 | (3) |
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22.2.2 Finite Temperature |
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596 | (1) |
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22.2.3 Magnetic Catalysis |
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597 | (2) |
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599 | (2) |
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22.3 The D4-D8-(Sakai-Sugimoto) Model |
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601 | (13) |
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601 | (3) |
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22.3.2 Finite Density and Background Fields |
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604 | (2) |
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22.3.3 Magnetic Catalysis of Chiral Symmetry Breaking |
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606 | (1) |
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22.3.4 Anomalous Currents |
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607 | (2) |
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22.3.5 The Pion Gradient Phase |
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609 | (3) |
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22.3.6 Magnetic Phase Transition |
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612 | (2) |
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614 | |
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614 | (2) |
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22.4.2 Finite Density and Background Fields |
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616 | (2) |
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22.4.3 Quantum Hall States |
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618 | (1) |
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619 | (2) |
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621 | |