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xviii | |
Preface |
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xx | |
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1 | (23) |
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The classical dynamics of geometry |
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1 | (6) |
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7 | (4) |
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Beyond classical gravity: perturbative strings |
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11 | (4) |
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Beyond perturbative strings: branes |
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15 | (4) |
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The quantum dynamics of geometry |
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19 | (1) |
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Things to do in the meantime |
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20 | (2) |
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22 | (2) |
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24 | (46) |
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Motion of classical point particles |
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24 | (3) |
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24 | (2) |
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26 | (1) |
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Classical bosonic strings |
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27 | (13) |
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27 | (2) |
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29 | (1) |
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String equations of motion |
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30 | (1) |
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Further aspects of the two dimensional perspective |
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31 | (4) |
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35 | (1) |
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35 | (2) |
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37 | (1) |
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Conformal invariance as a residual symmetry |
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37 | (1) |
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Some Hamiltonian dynamics |
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38 | (2) |
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Quantised bosonic strings |
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40 | (7) |
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The constraints and physical states |
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41 | (1) |
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The intercept and critical dimensions |
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42 | (3) |
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A glance at more sophisticated techniques |
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45 | (2) |
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The sphere, the plane and the vertex operator |
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47 | (4) |
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48 | (3) |
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51 | (1) |
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52 | (4) |
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52 | (2) |
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Unoriented closed strings |
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54 | (1) |
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55 | (1) |
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Strings in curved backgrounds |
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56 | (5) |
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61 | (9) |
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Working with the local tangent frames |
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61 | (2) |
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63 | (2) |
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Coordinate vs. orthonormal bases |
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65 | (2) |
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The Lorentz group as a gauge group |
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67 | (1) |
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Fermions in curved spacetime |
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68 | (1) |
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Comparison to differential geometry |
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68 | (2) |
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A closer look at the world-sheet |
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70 | (24) |
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70 | (10) |
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70 | (3) |
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The special case of two dimensions |
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73 | (1) |
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74 | (1) |
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The operator product expansion |
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75 | (1) |
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The stress tensor and the Virasoro algebra |
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76 | (4) |
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Revisiting the relativistic string |
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80 | (5) |
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Fixing the conformal gauge |
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85 | (2) |
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85 | (1) |
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86 | (1) |
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The closed string partition function |
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87 | (7) |
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Strings on circles and T-duality |
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94 | (35) |
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Fields and strings on a circle |
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94 | (5) |
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The Kaluza--Klein reduction |
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95 | (1) |
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Closed strings on a circle |
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96 | (3) |
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T-duality for closed strings |
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99 | (1) |
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A special radius: enhanced gauge symmetry |
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100 | (3) |
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The circle partition function |
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103 | (1) |
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Toriodal compactifications |
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104 | (4) |
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More on enhanced gauge symmetry |
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108 | (5) |
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108 | (3) |
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The classical Lie algebras |
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111 | (2) |
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Physical realisations with vertex operators |
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113 | (1) |
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Another special radius: bosonisation |
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113 | (4) |
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String theory on an orbifold |
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117 | (2) |
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T-duality for open strings: D-branes |
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119 | (4) |
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Chan--Paton factors and Wilson lines |
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121 | (2) |
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D-brane collective coordinates |
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123 | (2) |
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T-duality for unoriented strings: orientifolds |
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125 | (4) |
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Background fields and world-volume actions |
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129 | (12) |
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T-duality in background fields |
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129 | (2) |
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A first look at the D-brane world-volume action |
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131 | (4) |
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World-volume actions from tilted D-branes |
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133 | (2) |
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The Dirac--Born--Infeld action |
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135 | (1) |
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136 | (1) |
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136 | (2) |
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D-branes and gauge theory |
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138 | (1) |
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BPS lumps on the world-volume |
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138 | (3) |
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D-brane tension and boundary states |
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141 | (14) |
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142 | (6) |
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An open string partition function |
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142 | (3) |
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A background field computation |
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145 | (3) |
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148 | (2) |
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Another open string partition function |
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148 | (2) |
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The boundary state formalism |
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150 | (5) |
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155 | (37) |
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The three basic superstring theories |
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155 | (14) |
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Open superstrings: type I |
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155 | (5) |
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Closed superstrings: type II |
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160 | (5) |
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Type I from type IIB, the prototype orientifold |
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165 | (1) |
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The Green--Schwarz mechanism |
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166 | (3) |
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The two basic heterotic string theories |
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169 | (5) |
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SO(32) and E8 x E8 from self-dual lattices |
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171 | (1) |
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172 | (2) |
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The ten dimensional supergravities |
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174 | (2) |
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Heterotic toroidal compactifications |
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176 | (2) |
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Superstring toroidal compactification |
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178 | (1) |
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A superstring orbifold: discovering the K3 manifold |
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179 | (13) |
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180 | (3) |
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Another miraculous anomaly cancellation |
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183 | (1) |
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184 | (1) |
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185 | (4) |
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189 | (2) |
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191 | (1) |
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Supersymmetric strings and T-duality |
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192 | (13) |
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T-duality of supersymmetric strings |
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192 | (3) |
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T-duality of type II superstrings |
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192 | (1) |
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T-duality of type I superstrings |
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193 | (1) |
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T-duality for the heterotic strings |
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194 | (1) |
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195 | (2) |
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The D-brane charge and tension |
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197 | (3) |
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The orientifold charge and tension |
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200 | (1) |
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Type I from type IIB, revisited |
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201 | (1) |
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Dirac charge quantisation |
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201 | (1) |
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202 | (3) |
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World-volume curvature couplings |
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205 | (19) |
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Tilted D-branes and branes within branes |
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205 | (1) |
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Anomalous gauge couplings |
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206 | (4) |
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Characteristic classes and invariant polynomials |
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210 | (6) |
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Anomalous curvature couplings |
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216 | (2) |
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218 | (2) |
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220 | (1) |
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Further non-Abelian extensions |
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221 | (1) |
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Further curvature couplings |
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222 | (2) |
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224 | (25) |
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A look at black holes in four dimensions |
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224 | (14) |
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A brief study of the Einstein--Maxwell system |
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224 | (1) |
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Basic properties of Schwarzschild |
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225 | (3) |
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Basic properties of Reissner--Nordstrom |
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228 | (1) |
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Extremality, supersymmetry, and the BPS condition |
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228 | (4) |
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Multiple black holes and multicentre solutions |
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232 | (1) |
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Near horizon geometry and an infinite throat |
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233 | (1) |
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Cosmological constant; de Sitter and anti-de Sitter |
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233 | (1) |
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de-Sitter spacetime and the sphere |
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234 | (1) |
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Anti-de Sitter in various coordinate systems |
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235 | (1) |
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Anti-de Sitter as a hyperbolic slice |
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236 | (1) |
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Revisiting the extremal solution |
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237 | (1) |
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238 | (5) |
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A family of `p-brane' solutions |
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238 | (1) |
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The boost form of solution |
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239 | (1) |
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The extremal limit and coincident D-branes |
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240 | (3) |
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Probing p-brane geometry with Dp-branes |
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243 | (3) |
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Thought experiment: building p with Dp |
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243 | (1) |
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Effective Lagrangian from the world-volume action |
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244 | (1) |
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245 | (1) |
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T-duality and supergravity solutions |
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246 | (3) |
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246 | (2) |
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248 | (1) |
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Multiple D-branes and bound states |
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249 | (12) |
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Dp and Dp' from boundary conditions |
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249 | (3) |
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The BPS bound for the Dp--Dp' system |
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252 | (2) |
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Bound states of fundamental strings and D-strings |
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254 | (1) |
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The three-string junction |
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255 | (3) |
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Aspects of D-brane bound states |
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258 | (3) |
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258 | (1) |
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258 | (1) |
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259 | (1) |
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260 | (1) |
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260 | (1) |
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Strong coupling and string duality |
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261 | (21) |
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Type IIB/type IIB duality |
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261 | (3) |
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D1-brane collective coordinates |
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261 | (2) |
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263 | (1) |
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SO(32) Type I/heterotic duality |
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264 | (1) |
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D1-brane collective coordinates |
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264 | (1) |
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Dual branes from 10D string-string duality |
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265 | (6) |
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The heterotic NS-fivebrane |
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267 | (1) |
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The type IIA and type IIB NS5-brane |
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268 | (3) |
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Type IIA/M-theory duality |
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271 | (2) |
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A closer look at D0-branes |
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271 | (1) |
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Eleven dimensional supergravity |
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271 | (2) |
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E8 x E8 heterotic string/M-theory duality |
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273 | (3) |
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276 | (2) |
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276 | (1) |
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From D-branes and NS5-branes to M-branes and back |
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277 | (1) |
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278 | (4) |
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Type II strings on T5 and E6(6) |
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278 | (1) |
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U-duality and bound states |
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279 | (3) |
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282 | (40) |
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D-branes as probes of ALE spaces |
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282 | (9) |
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Basic setup and a quiver gauge theory |
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282 | (3) |
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The moduli space of vacua |
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285 | (1) |
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ALE space as metric on moduli space |
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286 | (3) |
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D-branes and the hyper-Kahler quotient |
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289 | (2) |
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Fractional D-branes and wrapped D-branes |
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291 | (3) |
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291 | (1) |
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292 | (2) |
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Wrapped, fractional and stretched branes |
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294 | (6) |
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NS5-branes from ALE spaces |
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295 | (1) |
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Dual realisations of quivers |
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296 | (4) |
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300 | (6) |
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Seeing the instanton with a probe |
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301 | (4) |
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305 | (1) |
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306 | (8) |
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Adjoint Higgs and monopoles |
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309 | (2) |
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BPS monopole solution from Nahm data |
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311 | (3) |
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The D-brane dielectric effect |
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314 | (8) |
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Non-Abelian world-volume interactions |
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314 | (2) |
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Stable fuzzy spherical D-branes |
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316 | (2) |
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Stable smooth spherical D-branes |
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318 | (4) |
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K3 orientifolds and compactification |
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322 | (23) |
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ZN orientifolds and Chan--Paton factors |
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322 | (2) |
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Loops and tadpoles for ALE ZM singularities |
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324 | (9) |
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One-loop diagrams and tadpoles |
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324 | (1) |
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Computing the one-loop diagrams |
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325 | (5) |
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330 | (3) |
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Solving the tadpole equations |
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333 | (3) |
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333 | (1) |
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334 | (2) |
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336 | (3) |
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339 | (2) |
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Anomalies for N = 1 in six dimensions |
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341 | (4) |
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345 | (22) |
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345 | (1) |
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Probing six-branes: Kaluza--Klein monopoles and M-theory |
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346 | (2) |
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The moduli space of 3D supersymmetric gauge theory |
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348 | (4) |
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Wrapped branes and the enhancon mechanism |
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352 | (8) |
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353 | (1) |
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354 | (2) |
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Probing with a wrapped D6-brane |
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356 | (4) |
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The consistency of excision in supergravity |
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360 | (2) |
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The moduli space of pure glue in 3D |
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362 | (5) |
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Multi-monopole moduli space |
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363 | (4) |
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367 | (42) |
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The type IIB string and F-theory |
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367 | (27) |
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368 | (1) |
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369 | (2) |
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371 | (2) |
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The self-duality of D3-branes |
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373 | (2) |
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375 | (1) |
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376 | (3) |
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379 | (4) |
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F-theory, and a dual heterotic description |
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383 | (1) |
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384 | (2) |
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Enhanced gauge symmetry and singularities of K3 |
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386 | (1) |
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F-theory at constant coupling |
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387 | (5) |
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The moduli space of N = 2 SU (N) with Nf = 4 |
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392 | (2) |
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M-theory origins of F-theory |
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394 | (6) |
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M-branes and odd D-branes |
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396 | (3) |
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M-theory on K3 and heterotic on T3 |
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399 | (1) |
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Type IIA on K3 and heterotic on T4 |
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400 | (1) |
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400 | (9) |
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Another look at D0-branes |
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401 | (1) |
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The infinite momentum frame |
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402 | (2) |
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404 | (5) |
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409 | (31) |
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Black hole thermodynamics |
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409 | (5) |
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The path integral and the Euclidean calculus |
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409 | (2) |
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The semiclassical approximation |
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411 | (1) |
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The temperature of black holes |
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412 | (2) |
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The Euclidean action calculus |
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414 | (4) |
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The action for Schwarzschild |
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414 | (2) |
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The action for Reissner--Nordstrom |
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416 | (1) |
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The laws of thermodynamics |
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417 | (1) |
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D = 5 Reissner--Nordstrom black holes |
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418 | (11) |
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420 | (5) |
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Microscopic entropy and a 2D field theory |
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425 | (2) |
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Non-extremality and a 2D dilute gas limit |
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427 | (2) |
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429 | (3) |
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432 | (8) |
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432 | (1) |
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433 | (1) |
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Probing the black hole with branes |
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434 | (3) |
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The enhancon and the second law |
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437 | (3) |
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D-branes, gravity and gauge theory |
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440 | (27) |
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The AdS/CFT correspondence |
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441 | (11) |
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Branes and the decoupling limit |
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441 | (2) |
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Sphere reduction and gauged supergravity |
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443 | (3) |
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Extracts from the dictionary |
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446 | (3) |
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The action, counterterms, and the stress tensor |
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449 | (3) |
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The correspondence at finite temperature |
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452 | (3) |
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Limits of the non-extremal D3-brane |
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452 | (1) |
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The AdS--Schwarzschild black hole in global coordinates |
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453 | (2) |
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The correspondence with a chemical potential |
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455 | (9) |
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Spinning D3-branes and charged AdS black holes |
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455 | (4) |
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The AdS--Reissner--Nordstrom black hole |
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459 | (1) |
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Thermodynamic phase structure |
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459 | (5) |
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The holographic principle |
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464 | (3) |
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The holographic renormalisation group |
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467 | (37) |
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Renormalisation group flows from gravity |
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467 | (5) |
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A BPS domain wall and supersymmetry |
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469 | (3) |
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Flowing on the Coulomb branch |
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472 | (8) |
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A five dimensional solution |
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472 | (3) |
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A ten dimensional solution |
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475 | (1) |
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475 | (3) |
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478 | (2) |
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An N = 1 gauge dual RG flow |
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480 | (14) |
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The five dimensional solution |
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482 | (4) |
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The ten dimensional solution |
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486 | (1) |
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487 | (1) |
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488 | (1) |
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Kahler structure of the Coulomb branch |
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489 | (5) |
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An N = 2 gauge dual RG flow and the enhancon |
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494 | (8) |
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The five dimensional solution |
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494 | (4) |
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The ten dimensional solution |
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498 | (1) |
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499 | (1) |
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500 | (2) |
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502 | (2) |
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504 | (6) |
References |
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510 | (19) |
Index |
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529 | |