Preface |
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xi | |
I Lectures |
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1 | (290) |
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3 | (16) |
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3 | (1) |
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4 | (1) |
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4 | (1) |
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5 | (8) |
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5 Phenomenology of the landscape |
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13 | (6) |
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QUANTIZATION OF HOLOMORPHIC FORMS AND N = 1 SUPERSYMMETRY ON SPECIAL MANIFOLDS |
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19 | (22) |
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19 | (1) |
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2 N = 1 supersymmetry and the holomorphic BF theory |
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20 | (2) |
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3 Four dimensions: Kähler manifold |
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22 | (5) |
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4 Six dimensions: Calabi—Yau three—fold |
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27 | (4) |
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31 | (10) |
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41 | (38) |
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by MICHEL BAUER AND DENIS BERNARD |
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1 Critical interfaces and stochastic processes |
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44 | (17) |
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61 | (18) |
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THEORY OF COSMOLOGICAL PERTURBATIONS AND APPLICATIONS TO SUPERSTRING COSMOLOGY |
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79 | (38) |
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by ROBERT H. BRANDENBERGER |
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79 | (2) |
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2 Overview of Inflationary Cosmology |
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81 | (5) |
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3 Newtonian Theory of Cosmological Perturbations |
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86 | (6) |
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4 Relativistic Theory of Cosmological Fluctuations |
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92 | (7) |
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5 Quantum Theory of Cosmological Fluctuations |
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99 | (5) |
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6 Conceptual Problems of Inflationary Cosmology |
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104 | (2) |
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7 The Trans-Planckian Window for Superstring Cosmology |
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106 | (6) |
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112 | (5) |
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TOWARDS A TOPOLOGICAL G2 STRING |
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117 | (12) |
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by JAN DE BOER, ASAD NAQVI AND ASSAF SHOMER |
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117 | (1) |
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118 | (1) |
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3 Tri-Critical Ising Model |
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119 | (2) |
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121 | (1) |
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122 | (2) |
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124 | (1) |
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125 | (4) |
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CHALLENGES OF MATRIX MODELS |
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129 | (34) |
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129 | (1) |
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2 Classical period: introduction of models |
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130 | (1) |
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3 First stringy period: generalizations and hunt for structures |
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131 | (4) |
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4 Transcendental period: absolutization of structures |
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135 | (8) |
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5 Towards exhaustive theory of 1-matrix model: the Dijkgraaf-Vafa theory |
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143 | (12) |
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6 Neoclassical period: back to concrete results and back to physics? |
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155 | (8) |
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PHENOMENOLOGY OF NEUTRINO OSCILLATIONS |
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163 | (14) |
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1 A short history of neutrinos [1-16] |
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163 | (1) |
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2 Simple formulas for oscillations |
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164 | (2) |
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3 "Same energy" vs "same momentum" [12-14], [17-25] |
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166 | (1) |
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167 | (2) |
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5 Reactor antineutrinos [27-30] |
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169 | (1) |
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6 Atmospheric neutrinos [26] |
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170 | (1) |
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7 Accelerator neutrinos [27] |
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171 | (1) |
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8 Patterns of mixing angles and masses [25.31] |
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171 | (1) |
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172 | (1) |
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10 Cosmological and stellar inputs 1331 |
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172 | (1) |
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11 Challenges and Prospects [31,34] |
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173 | (4) |
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CLOSED STRINGS IN MISNER SPACE: A TOY MODEL FOR A BIG BOUNCE? |
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177 | (24) |
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by BRUNO DURIN AND BORIS PIOLINE |
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1 Semi-classics of closed strings in Misner space |
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178 | (9) |
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2 One-loop vacuum amplitude |
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187 | (4) |
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3 Tree-level scattering amplitudes |
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191 | (6) |
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197 | (4) |
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PHENOMENOLOGICAL GUIDE TO PHYSICS BEYOND THE STANDARD MODEL |
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201 | (28) |
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201 | (2) |
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203 | (8) |
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3 Hints from the Standard Model for its extensions |
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211 | (10) |
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4 Supersymmetric extensions of the Standard Model |
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221 | (6) |
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227 | (2) |
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INTRODUCTION TO COSMIC F- AND D-STRINGS |
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229 | (26) |
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229 | (1) |
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230 | (6) |
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3 Cosmic strings from string theory |
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236 | (3) |
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4 Production of cosmic F- and D-strings |
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239 | (2) |
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241 | (4) |
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245 | (3) |
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7 Distinguishing Superstrings |
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248 | (2) |
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250 | (5) |
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LONG TIME SCALES AND ETERNAL BLACK HOLES |
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255 | (10) |
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by JOSE L. E BARBÓN AND ELIEZER RABINOVICI |
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255 | (2) |
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2 Long-time details of thermal quasi-equilibrium |
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257 | (3) |
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3 Topological diversity and unitarity |
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260 | (2) |
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262 | (3) |
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SEMICLASSICAL STRINGS AND ADS/CFT |
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265 | (26) |
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265 | (7) |
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2 Effective actions for coherent states |
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272 | (8) |
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3 General fast motion in S5 and SO(6) scalar operators |
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280 | (4) |
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284 | (7) |
II SEMINARS |
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291 | (106) |
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BARYOGENESIS WITH LARGE EXTRA DIMENSIONS |
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293 | (4) |
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BRANEWORLD COSMOLOGY ALMOST WITHOUT BRANES |
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297 | (8) |
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297 | (1) |
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297 | (2) |
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299 | (1) |
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4 Cosmological perturbations: theory and observations |
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300 | (2) |
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302 | (3) |
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CHAOTIC CASCADES FOR D-BRANES ON SINGULARITIES |
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305 | (6) |
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by SEBASTIAN FRANCO ET AL. |
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305 | (1) |
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2 Cascades in coupling space |
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305 | (1) |
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3 Duality Walls and Fractals |
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306 | (1) |
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307 | (1) |
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308 | (3) |
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N = 1 GAUGE THEORY EFFECTIVE SUPERPOTENTIALS |
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311 | (8) |
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311 | (1) |
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2 The Gauge Theory/Matrix Model Correspondence |
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312 | (2) |
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314 | (2) |
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316 | (3) |
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GROMOV-WITTEN THEORY AND AUTOMORPHIC FORMS |
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319 | (1) |
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319 | (1) |
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320 | (1) |
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321 | (1) |
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322 | (1) |
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322 | (1) |
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323 | (2) |
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BLACK HOLE INSTABILITIES AND PHASE TRANSITIONS |
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325 | (1) |
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1 Generalised AdS black holes |
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325 | (1) |
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326 | (3) |
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329 | (8) |
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329 | (1) |
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330 | (2) |
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3 Cosmological singularity |
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332 | (1) |
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333 | (4) |
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337 | (4) |
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337 | (1) |
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338 | (2) |
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340 | (1) |
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D-BRANE EFFECTIVE ACTIONS |
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341 | (4) |
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341 | (1) |
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341 | (1) |
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342 | (3) |
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ADS2 X S² AS AN EXACT HETEROTIC STRING BACKGROUND |
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345 | (6) |
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345 | (1) |
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2 SU (2) asymmetric deformation |
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345 | (2) |
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347 | (1) |
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348 | (3) |
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STRINGS AND D-BRANES IN HOLOGRAPHIC BACKGROUNDS |
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351 | (4) |
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by DAN ISRAËL AND ARI PAKMAN |
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351 | (1) |
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2 SL(2,R)/U(1) and N=2 Lionville |
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352 | (1) |
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3 D-branes from boundary AdS3 |
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353 | (1) |
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4 strings near NS5 branes |
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353 | (2) |
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COSMIC CENSORSHIP IN ADS/CFT |
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355 | (8) |
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355 | (1) |
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356 | (2) |
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3 The Size of the singularity |
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358 | (2) |
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360 | (3) |
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TOPICS IN BLACK HOLE PRODUCTION |
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363 | (8) |
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363 | (1) |
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2 Wavepackets and Semiclassics |
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363 | (2) |
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3 Multiple Black Hole Production |
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365 | (1) |
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366 | (5) |
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TOWARDS THE EXACT DILATATION OPERATOR OF N = 4 SUPER YANG-MILLS THEORY |
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371 | (8) |
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371 | (1) |
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372 | (2) |
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3 Summing D(¹) to all orders |
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374 | (2) |
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376 | (3) |
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MODULI TRAPPING AND STRING GAS COSMOLOGY |
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379 | (6) |
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379 | (1) |
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2 Strings at Finite Temperature |
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380 | (1) |
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381 | (1) |
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382 | (3) |
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STRINGY GEOMETRY: GENERALIZED COMPLEX STRUCTURE |
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385 | (8) |
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1 Mathematical preliminaries |
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385 | (3) |
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388 | (2) |
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3 Topological model with WZ term |
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390 | (3) |
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INTEGRABILITY OF SUPERCONFORMAL FIELD THEORY AND SUSY N=1 KDV |
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393 | (1) |
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393 | (1) |
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394 | (1) |
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395 | (2) |
APPENDIX |
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397 | |
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399 | (2) |
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401 | |