Preface |
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xv | |
A note on choice of metric |
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xviii | |
Text website |
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xx | |
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Part 1 Effective field theory: the Standard Model, supersymmetry, unification |
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1 | (136) |
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Before the Standard Model |
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3 | (6) |
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7 | (2) |
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9 | (20) |
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9 | (3) |
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Realizations of symmetry in quantum field theory |
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12 | (6) |
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The quantization of Yang-Mills theories |
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18 | (4) |
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The particles and fields of the Standard Model |
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22 | (3) |
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25 | (2) |
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27 | (2) |
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28 | (1) |
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28 | (1) |
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Phenomenology of the Standard Model |
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29 | (34) |
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29 | (3) |
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The quark and lepton mass matrices |
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32 | (2) |
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34 | (1) |
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The renormalization group |
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35 | (4) |
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Calculating the beta function |
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39 | (4) |
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The strong interactions and dimensional transmutation |
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43 | (1) |
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Confinement and lattice gauge theory |
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44 | (7) |
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Strong interaction processes at high momentum transfer |
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51 | (12) |
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59 | (2) |
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61 | (2) |
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The Standard Model as an effective field theory |
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63 | (12) |
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Lepton and baryon number violation |
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66 | (4) |
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Challenges for the Standard Model |
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70 | (1) |
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71 | (1) |
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Dark matter and dark energy |
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72 | (1) |
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Summary: successes and limitations of the Standard Model |
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73 | (2) |
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73 | (2) |
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Anomalies, instantons and the strong CP problem |
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75 | (32) |
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76 | (5) |
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81 | (8) |
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89 | (11) |
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100 | (2) |
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Possible solutions of the strong CP problem |
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102 | (5) |
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105 | (1) |
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106 | (1) |
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107 | (12) |
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Cancellation of anomalies |
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110 | (1) |
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Renormalization of couplings |
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110 | (1) |
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Breaking to SU(3) x SU(2) x U(1) |
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111 | (1) |
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112 | (1) |
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Charge quantization and magnetic monopoles |
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113 | (1) |
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114 | (1) |
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114 | (5) |
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117 | (1) |
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117 | (2) |
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Magnetic monopoles and solitons |
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119 | (12) |
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Solitons in 1 + 1 dimensions |
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120 | (2) |
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Solitons in 2 + 1 dimensions: strings or vortices |
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122 | (1) |
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122 | (2) |
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124 | (1) |
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Collective coordinates for the monopole solution |
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125 | (2) |
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The Witten effect: the electric charge in the presence of θ |
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127 | (1) |
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Electric-magnetic duality |
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128 | (3) |
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129 | (1) |
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129 | (2) |
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Technicolor: a first attempt to explain hierarchies |
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131 | (6) |
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QCD in a world without Higgs fields |
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132 | (1) |
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Fermion masses: extended technicolor |
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133 | (2) |
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Precision electroweak measurements |
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135 | (2) |
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136 | (1) |
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136 | (1) |
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137 | (166) |
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139 | (18) |
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The supersymmetry algebra and its representations |
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140 | (1) |
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140 | (4) |
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144 | (3) |
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The supersymmetry currents |
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147 | (1) |
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The ground-state energy in globally supersymmetric theories |
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148 | (1) |
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149 | (2) |
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Non-renormalization theorems |
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151 | (3) |
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Local supersymmetry: supergravity |
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154 | (3) |
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155 | (1) |
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155 | (2) |
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A first look at supersymmetry breaking |
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157 | (10) |
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Spontaneous supersymmetry breaking |
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157 | (3) |
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160 | (1) |
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Loop corrections and the vacuum degeneracy |
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161 | (1) |
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Explicit, soft supersymmetry breaking |
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162 | (1) |
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Supersymmetry breaking in supergravity models |
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163 | (4) |
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166 | (1) |
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166 | (1) |
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The Minimal Supersymmetric Standard Model |
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167 | (18) |
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Soft supersymmetry breaking in the MSSM |
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169 | (4) |
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173 | (2) |
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Why is one Higgs mass negative? |
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175 | (1) |
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Radiative corrections to the Higgs mass limit |
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176 | (1) |
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Embedding the MSSM in supergravity |
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177 | (1) |
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178 | (1) |
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Constraints on soft breakings |
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179 | (6) |
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183 | (1) |
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183 | (2) |
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Supersymmetric grand unification |
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185 | (6) |
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A supersymmetric grand unified model |
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185 | (1) |
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Coupling constant unification |
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186 | (2) |
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Dimension-five operators and proton decay |
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188 | (3) |
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189 | (1) |
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189 | (2) |
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191 | (18) |
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Criteria for supersymmetry breaking: the Witten index |
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192 | (1) |
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Gaugino condensation in pure gauge theories |
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193 | (1) |
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194 | (3) |
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Nf < N: a non-perturbative superpotential |
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197 | (3) |
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The superpotential in the case Nf < N -- 1 |
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200 | (1) |
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Nf = N -- 1: the instanton-generated superpotential |
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201 | (8) |
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208 | (1) |
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208 | (1) |
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Dynamical supersymmetry breaking |
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209 | (10) |
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Models of dynamical supersymmetry breaking |
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209 | (2) |
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Particle physics and dynamical supersymmetry breaking |
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211 | (8) |
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218 | (1) |
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218 | (1) |
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Theories with more than four conserved supercharges |
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219 | (14) |
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N = 2 theories: exact moduli spaces |
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219 | (2) |
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A still simpler theory: N = 4 Yang-Mills |
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221 | (2) |
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A deeper understanding of the BPS condition |
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223 | (2) |
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225 | (8) |
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230 | (1) |
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231 | (2) |
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More supersymmetric dynamics |
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233 | (10) |
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Conformally invariant field theories |
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233 | (2) |
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235 | (1) |
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236 | (4) |
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240 | (1) |
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241 | (2) |
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241 | (1) |
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242 | (1) |
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An introduction to general relativity |
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243 | (16) |
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Tensors in general relativity |
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244 | (5) |
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249 | (1) |
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250 | (2) |
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The Schwarzschild solution |
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252 | (2) |
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Features of the Schwarzschild metric |
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254 | (2) |
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Coupling spinors to gravity |
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256 | (3) |
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257 | (1) |
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257 | (2) |
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259 | (10) |
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A history of the universe |
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263 | (6) |
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268 | (1) |
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268 | (1) |
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Astroparticle physics and inflation |
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269 | (34) |
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272 | (8) |
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280 | (3) |
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The LSP as the dark matter |
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283 | (2) |
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285 | (2) |
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287 | (7) |
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Flat directions and baryogenesis |
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294 | (2) |
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Supersymmetry breaking in the early universe |
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296 | (1) |
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The fate of the condensate |
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297 | (3) |
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300 | (3) |
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301 | (1) |
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301 | (2) |
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303 | (178) |
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305 | (8) |
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The peculiar history of string theory |
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306 | (7) |
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311 | (2) |
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313 | (28) |
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The light cone gauge in string theory |
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315 | (3) |
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318 | (2) |
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320 | (2) |
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322 | (6) |
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Vertex operators and the S-matrix |
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328 | (6) |
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The S-matrix vs. the effective action |
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334 | (1) |
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335 | (6) |
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338 | (1) |
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338 | (3) |
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341 | (18) |
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341 | (2) |
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Quantization in the Ramond sector: the appearance of space-time fermions |
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343 | (1) |
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344 | (1) |
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World sheet supersymmetry |
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345 | (1) |
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The spectra of the superstrings |
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346 | (7) |
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Manifest space-time supersymmetry: the Green-Schwarz formalism |
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353 | (2) |
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355 | (4) |
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356 | (1) |
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356 | (3) |
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359 | (6) |
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360 | (1) |
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361 | (1) |
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Heterotic string interactions |
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361 | (2) |
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A non-supersymmetric heterotic string theory |
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363 | (2) |
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363 | (1) |
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364 | (1) |
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Effective actions in ten dimensions |
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365 | (8) |
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Coupling constants in string theory |
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368 | (5) |
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371 | (1) |
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371 | (2) |
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Compactification of string theory I. Tori and orbifolds |
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373 | (28) |
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Compactification in field theory: the Kaluza-Klein program |
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373 | (4) |
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377 | (3) |
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380 | (2) |
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Strings in background fields |
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382 | (4) |
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Bosonic formulation for the heterotic string |
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386 | (1) |
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387 | (8) |
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Effective actions in four dimensions for orbifold models |
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395 | (3) |
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Non-supersymmetric compactifications |
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398 | (3) |
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399 | (1) |
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400 | (1) |
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Compactification of string theory II. Calabi--Yau compactifications |
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401 | (28) |
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Mathematical preliminaries |
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401 | (5) |
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Calabi-Yau spaces: constructions |
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406 | (3) |
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The spectrum of Calabi--Yau compactifications |
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409 | (2) |
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World sheet description of Calabi--Yau compactification |
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411 | (3) |
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An example: the quintic in CP4 |
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414 | (2) |
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Calabi--Yau compactification of the heterotic string at weak coupling |
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416 | (13) |
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426 | (1) |
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427 | (2) |
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Dynamics of string theory at weak coupling |
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429 | (12) |
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Non-renormalization theorems |
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430 | (4) |
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434 | (4) |
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438 | (1) |
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Obstacles to a weakly coupled string phenomenology |
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439 | (2) |
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440 | (1) |
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Beyond weak coupling: non-perturbative string theory |
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441 | (26) |
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442 | (1) |
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Strings at strong coupling: duality |
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442 | (1) |
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443 | (4) |
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Branes from T-duality of Type I strings |
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447 | (4) |
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Strong-weak coupling dualities: the equivalence of different string theories |
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451 | (1) |
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Strong-weak coupling dualities: some evidence |
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452 | (6) |
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Strongly coupled heterotic string |
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458 | (2) |
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Non-perturbative formulations of string theory |
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460 | (7) |
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465 | (1) |
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466 | (1) |
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Large and warped extra dimensions |
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467 | (8) |
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Large extra dimensions: the ADD proposal |
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467 | (3) |
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Warped spaces: the Randall-Sundrum proposal |
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470 | (5) |
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473 | (1) |
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473 | (2) |
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Coda: where are we headed? |
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475 | (6) |
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479 | (2) |
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481 | (24) |
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Appendix A Two-component spinors |
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483 | (4) |
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Appendix B Goldstone's theorem and the pi mesons |
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487 | (4) |
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489 | (2) |
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Appendix C Some practice with the path integral in field theory |
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491 | (10) |
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491 | (1) |
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Finite-temperature field theory |
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492 | (3) |
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495 | (1) |
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Weak interactions at high temperature |
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496 | (1) |
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Electroweak baryon number violation |
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497 | (2) |
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499 | (1) |
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499 | (2) |
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Appendix D The beta function in supersymmetric Yang-Mills theory |
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501 | (4) |
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503 | (2) |
References |
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505 | (6) |
Index |
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511 | |