| Preface |
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xiii | |
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The Standard Model: 30 Years of Glory |
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1 | (50) |
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1 | (1) |
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2 | (20) |
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2 | (3) |
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Neutrino scattering results (1972-1974) |
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5 | (2) |
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7 | (1) |
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8 | (2) |
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10 | (5) |
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15 | (5) |
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20 | (2) |
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Weak interaction and quark and lepton families |
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22 | (21) |
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Neutral current discovery (1973-1974) |
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22 | (7) |
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Discovery of the W and Z bosons |
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29 | (2) |
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31 | (1) |
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The experimental apparatus |
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32 | (3) |
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A new quark: Charm (The 1974 ``November revolution'') |
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35 | (5) |
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The third family: the T lepton and b quark |
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40 | (1) |
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40 | (1) |
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41 | (2) |
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LEP and SLC: The ideal machines for Standard Model Studies |
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43 | (6) |
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44 | (3) |
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47 | (2) |
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49 | (2) |
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51 | (46) |
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51 | (1) |
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Small coupling, large logarithms and evolution |
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52 | (13) |
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Logarithm is not a function |
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53 | (1) |
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Puzzle of DIS and QCD partons |
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54 | (2) |
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56 | (2) |
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58 | (1) |
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Space-like parton evolution |
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58 | (1) |
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Time-like parton cascades |
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59 | (1) |
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Apparent and hidden in parton dynamics |
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60 | (2) |
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Fluctuation Time and Evolution Times: Coherence |
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62 | (2) |
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Vanishing of the forward inelastic diffraction |
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64 | (1) |
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Bremsstrahlung, coherence, conservation of current |
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65 | (15) |
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65 | (2) |
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67 | (1) |
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Soft radiation cross Section |
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68 | (1) |
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69 | (1) |
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Soft Photons don't carry quantum numbers |
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70 | (1) |
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Gribov Bremsstrahlung theorem |
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71 | (1) |
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Soft Gluons don't carry away no color |
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71 | (2) |
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Independent and coherent radiation |
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73 | (1) |
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The role of interference: strict angular ordering |
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74 | (1) |
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Angular ordering on the back of envelope |
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75 | (2) |
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Time delay and decoherence effects |
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77 | (3) |
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80 | (17) |
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QCD scattering and cross-channel radiation |
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80 | (4) |
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Conservation of color and QCD angular ordering |
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84 | (3) |
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Humpbacked plateau and LPHD |
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87 | (1) |
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Solving the DIS evolution |
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87 | (2) |
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89 | (2) |
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Coherent damping of the Landau singularity |
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91 | (1) |
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92 | (2) |
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94 | (1) |
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95 | (2) |
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Baryon Asymmetry of the Universe |
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97 | (46) |
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97 | (4) |
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Non-conservation of baryon number |
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101 | (9) |
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101 | (2) |
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Anomalous electroweak non-conservation of fermion quantum numbers |
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103 | (7) |
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110 | (1) |
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Grand unified baryogenesis |
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111 | (5) |
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Baryogenesis in decays of ultra-heavy particles |
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111 | (3) |
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Survival of primordial baryon asymmetry |
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114 | (2) |
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116 | (3) |
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119 | (15) |
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119 | (1) |
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Electroweak phase transition |
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120 | (2) |
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Electroweak sphalerons after the phase transition |
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122 | (2) |
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Sources of CP-violation in the EW theory and its extensions |
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124 | (1) |
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125 | (4) |
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Asymmetry from fermion-domain wall interactions |
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129 | (5) |
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134 | (9) |
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Introduction to Superstring Theory |
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143 | (46) |
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143 | (1) |
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Lecture 1: Overview and Motivation |
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144 | (10) |
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146 | (1) |
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Basic Ideas of String Theory |
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147 | (1) |
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A Brief History of String Theory |
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148 | (1) |
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149 | (1) |
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150 | (1) |
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The Second Superstring Revolution |
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151 | (1) |
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The Origins of Gauge Symmetry |
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152 | (1) |
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153 | (1) |
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Lecture 2: String Theory Basics |
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154 | (13) |
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World-Line Description of a Point Particle |
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155 | (1) |
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156 | (2) |
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158 | (2) |
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160 | (1) |
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161 | (3) |
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The Number of Physical States |
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164 | (1) |
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The Structure of String Perturbation Theory |
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165 | (1) |
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166 | (1) |
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167 | (9) |
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168 | (1) |
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169 | (2) |
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171 | (2) |
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173 | (1) |
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174 | (1) |
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175 | (1) |
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175 | (1) |
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Lecture 4: From Superstrings to M Theory |
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176 | (13) |
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178 | (2) |
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180 | (1) |
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Type IIB Superstring Theory |
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181 | (2) |
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The D3-Brane and N = 4 Gauge Theory |
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183 | (2) |
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185 | (4) |
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Neutrino Mass and Oscillations |
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189 | (62) |
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189 | (1) |
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Neutrinos in the Standard Model |
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190 | (7) |
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Direct Measurements of Neutrino Mass |
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197 | (5) |
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Motivating Neutrino Mass and Sterile Neutrinos in the Theory |
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202 | (3) |
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Neutrino Oscillation Formalism |
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205 | (6) |
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Experimental Signals for Oscillations |
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211 | (20) |
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The Solar Neutrino Deficit |
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211 | (5) |
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The Atmospheric Neutrino Deficit |
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216 | (7) |
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223 | (8) |
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Experiments Which Set Limits on Oscillations |
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231 | (5) |
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Limits on νμ ↔ νe oscillations |
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231 | (1) |
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Limits on νμ ↔ ντ oscillations |
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232 | (3) |
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Limits on νe ↔ ντ oscillations |
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235 | (1) |
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Theoretical Interpretation of the Data |
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236 | (2) |
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The Future (Near and Far) |
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238 | (8) |
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Future Tests of Solar Neutrino Oscillations |
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238 | (2) |
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Future Tests of Atmospheric Neutrino Oscillations |
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240 | (3) |
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Future Tests of the LSND Signal |
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243 | (2) |
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245 | (1) |
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246 | (5) |
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New Developments in Charged Particle Tracking |
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251 | (62) |
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251 | (1) |
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Experimental Environment - New Challenges |
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252 | (7) |
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e+e- B factories - Belle and BaBar |
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253 | (1) |
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Heavy Ion Physics - ALICE at the LHC |
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254 | (1) |
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Hadronic B factories - HERA-B |
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255 | (2) |
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The High Energy Frontier - ATLAS and CMS at the LHC |
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257 | (2) |
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Charged Particle Tracking with Gaseous Detectors |
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259 | (15) |
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Ionization of Gases by Charged Particles |
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259 | (1) |
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260 | (5) |
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265 | (6) |
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The Choice of the Gas Mixture |
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271 | (1) |
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Generic Gaseous Tracking Detectors |
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272 | (2) |
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Charged Particle Tracking with Semiconductor Detectors |
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274 | (8) |
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274 | (1) |
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Basic Semiconductor Physics |
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275 | (1) |
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276 | (4) |
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Position Sensitive Silicon Detectors |
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280 | (1) |
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Comparison of Silicon and Gaseous Detectors |
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281 | (1) |
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Radiation Damage Issues - (a) Gaseous Detectors |
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282 | (9) |
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Introduction and Historical Remarks |
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282 | (1) |
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Aging Mechanisms - Case Studies |
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282 | (1) |
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The Choice of the Gas Composition |
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283 | (2) |
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285 | (2) |
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287 | (2) |
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Gain and Irradiation Type |
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289 | (1) |
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Recommendations/Conclusions |
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290 | (1) |
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Radiation Damage Issues - (b) Silicon Detectors |
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291 | (7) |
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New Tracking Systems - Selected Example |
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298 | (9) |
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The ATLAS Semiconductor Tracker |
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300 | (3) |
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303 | (4) |
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307 | (6) |
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313 | (56) |
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313 | (2) |
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Physics of electromagnetic showers |
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315 | (3) |
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Energy resolution of electromagnetic calorimeters |
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318 | (6) |
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319 | (2) |
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321 | (1) |
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321 | (1) |
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322 | (2) |
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Physics of hadronic showers |
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324 | (1) |
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Energy resolution of hadronic calorimeters |
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325 | (4) |
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325 | (1) |
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325 | (1) |
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326 | (1) |
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326 | (2) |
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328 | (1) |
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Calorimeter performance requirements |
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329 | (5) |
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Main calorimeter techniques |
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334 | (22) |
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334 | (1) |
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Semiconductor calorimeters |
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335 | (1) |
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336 | (2) |
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Scintillation calorimeters |
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338 | (8) |
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Noble liquid calorimeters |
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346 | (3) |
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349 | (1) |
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Scintillation sampling calorimeters |
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350 | (1) |
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Gas sampling calorimeters |
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350 | (1) |
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Solid-state sampling calorimeters |
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351 | (1) |
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Liquid sampling calorimeters |
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351 | (5) |
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356 | (5) |
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Calorimeter integration in an experiment |
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361 | (3) |
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362 | (2) |
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364 | (1) |
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364 | (5) |
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An Update on the Properties of the Top Quark |
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369 | (12) |
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369 | (3) |
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More on mass and cross Section |
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372 | (2) |
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Search for decay of top into a charged Higgs |
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374 | (1) |
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Helicity of the W and spin correlations in top decays |
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375 | (2) |
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377 | (4) |
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Accelerator Physics and Circular Colliders |
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381 | (8) |
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Accelerator Physics Concepts |
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381 | (1) |
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Present Day Circular Colliders |
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382 | (2) |
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Future Circular Colliders |
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384 | (5) |
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Workshop on Confidence Limits |
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389 | (12) |
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389 | (1) |
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390 | (1) |
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391 | (8) |
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391 | (2) |
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What are confidence limits? |
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393 | (1) |
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393 | (2) |
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Feldman and Cousins: The Unified Approach |
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395 | (1) |
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Alex Read: The CLs Method |
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396 | (1) |
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397 | (1) |
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How should one handle nuisance parameters? |
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398 | (1) |
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398 | (1) |
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399 | (2) |
| Participants |
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401 | (4) |
| Index |
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405 | |
