Preface | xiii |
1 The Cosmological Parameters | 1 |
1.1 Introduction | 1 |
1.2 Why Measure the Parameters? | 2 |
1.2.1 Testing the Physics | 2 |
1.2.2 How Will It All End? | 7 |
1.3 The State of the Measurements | 11 |
1.4 Cosmology for the Next Generation | 17 |
2 In the Beginning... | 25 |
2.1 The Future Fate of Cosmology | 25 |
2.2 Testing Inflation | 27 |
2.3 The Power of the Cosmic Microwave Background | 28 |
2.4 Cosmic Concordance | 35 |
2.5 A New Age? | 40 |
3 Understanding Data Better with Bayesian and Global Statistical Methods | 49 |
3.1 Introduction | 49 |
3.2 Combining Experimental Measurements | 50 |
3.3 Bayesian Combination of Incompatible Measurements | 51 |
3.4 Another Variant of the Method | 56 |
3.5 Results for the Hubble Constant | 56 |
3.6 Conclusion | 59 |
4 Large-Scale Structure in the Universe | 61 |
4.1 Introduction | 61 |
4.2 Clustering and Large-Scale Structure | 65 |
4.2.1 Galaxies and Large-Scale Structure | 65 |
4.2.2 Clusters and Large-Scale Structure | 69 |
4.3 Peculiar Motions on Large Scales | 74 |
4.4 Dark Matter and Baryons in Clusters of Galaxies | 79 |
4.5 Is < 1? | 81 |
4.6 The SDSS and Large-Scale Structure | 82 |
4.6.1 The Sloan Digital Sky Survey | 82 |
4.6.2 Clusters of Galaxies | 83 |
4.7 Summary | 86 |
5 Unsolved Problems in Gravitational Lensing | 93 |
5.1 Introduction | 94 |
5.2 Gravitational Lens Optics | 94 |
5.3 The Problems | 98 |
5.3.1 How Old Is the Universe? | 98 |
5.3.2 What Is the Shape of the Universe? | 101 |
5.3.3 What Is the Large Scale Distribution of Matter? | 101 |
5.3.4 How Are Rich Clusters of Galaxies Formed? | 102 |
5.3.5 When Did Galaxies Form and How Did They Evolve? | 105 |
5.3.6 How Big Are Galaxies? | 106 |
5.3.7 Of What Are Galaxies Made? | 107 |
5.3.8 How Big Are AGN Ultraviolet Emission Regions? | 107 |
5.4 How Many More Surprises Will Gravitational Lenses Provide? | 108 |
6 What Can Be Learned from Numerical Simulations of Cosmology | 115 |
6.1 Introduction | 116 |
6.2 Simulation Methods | 119 |
6.2.1 Specification of Models | 119 |
6.2.2 Physical Processes and Numerical Methods | 122 |
6.3 Results: Comparison with Observations | 126 |
6.3.1 Hot Components | 126 |
6.3.2 Warm Components | 127 |
6.3.3 Cold Condensed Components | 128 |
6.4 Conclusions, Prospects, and More Questions | 129 |
7 The Centers of Elliptical Galaxies | 137 |
7.1 Introduction | 137 |
7.1.1 Black Holes and Quasars | 138 |
7.1.2 The Sphere of Influence | 139 |
7.1.3 Cores and Cusps | 140 |
7.2 Photometry | 142 |
7.2.1 The Peebles-Young Model | 145 |
7.3 Kinematic Evidence for Central Black Holes | 147 |
7.4 Physical Processes | 148 |
7.5 Summary | 152 |
8 The Morphological Evolution of Galaxies | 159 |
8.1 Introduction | 159 |
8.2 Early Formation of Massive Ellipticals | 161 |
8.3 Slow Evolution of Massive Disk Galaxies | 164 |
8.4 Redshift Surveys and the Dwarf-Dominated Universe | 166 |
8.5 Faint Galaxy Morphologies from HST | 170 |
8.6 Conclusions | 174 |
9 Quasars | 181 |
9.1 Quasars and the End of the `Dark Age' | 181 |
9.2 The Relation of AGNs to the Central Bulges of Galaxies | 183 |
9.3 Quasars and Their Remnants: Probes of General Relativity? | 186 |
9.3.1 Dead Quasars in Nearby Galaxies | 186 |
9.3.2 Do These Holes Have a Kerr Metric? | 187 |
10 Solar Neutrinos: Solved and Unsolved Problems | 195 |
10.1 Why Study Solar Neutrinos? | 195 |
10.2 What Does the Combined Standard Model Tell Us About Solar Neutrinos? | 198 |
10.2.1 The Combined Standard Model | 198 |
10.2.2 The Solar Neutrino Spectrum | 200 |
10.3 Why Are the Predicted Neutrino Fluxes Robust? | 201 |
10.4 What Are the Three Solar Neutrino Problems? | 202 |
10.4.1 Calculated versus Observed Chlorine Rate | 203 |
10.4.2 Incompatibility of Chlorine and Water (Kamiokande) Experiments | 204 |
10.4.3 Gallium Experiments: No Room for 7Be Neutrinos | 205 |
10.5 What Have We Learned? | 206 |
10.5.1 About Astronomy | 206 |
10.5.2 About Physics | 208 |
10.6 What Next? | 209 |
10.6.1 Solvable Problems in Physics | 209 |
10.6.2 Solvable Problems in Astronomy | 212 |
10.7 Summary | 217 |
11 Particle Dark Matter | 221 |
11.1 Introduction: Three Arguments for Non-Baryonic Dark Matter | 221 |
11.2 The Case for Non-baryonic Matter | 222 |
11.2.1 We've Looked for Baryonic Dark Matter and Failed | 222 |
11.2.2 We Can't Seem To Make the Observed Large-Scale Structure with Baryons | 223 |
11.2.3 Dynamical Mass Is Much Larger than Big Bang Nucleosynthesis Allows | 224 |
11.3 Neutrinos As Dark Matter | 225 |
11.3.1 Detecting Massive Neutrinos | 226 |
11.4 WIMPs | 227 |
11.4.1 Searching for WIMPs | 228 |
11.4.2 Indirect WIMP Detection | 230 |
11.4.3 What Is To Be Done? | 231 |
11.5 Axions | 231 |
11.6 Conclusions | 233 |
12 Stars in the Milky Way and Other Galaxies | 241 |
12.1 Introduction | 241 |
12.2 Recent Star Count Results | 241 |
12.3 Microlensing and Star Counts | 243 |
12.4 Disk Dark Matter: Still a Question | 243 |
12.5 Mystery of the Long Events | 244 |
12.6 Proper Motions from EROS II | 245 |
12.7 Pixel Lensing: Stellar Mass Functions in Other Galaxies | 246 |
12.8 Star Formation History of the Universe | 248 |
12.9 Conclusions | 249 |
13 Searching for MACHOs with Microlensing | 253 |
13.1 Introduction | 253 |
13.2 The Gravitational Microlens | 254 |
13.3 The "Macho Fraction" in the Galactic Halo | 256 |
13.4 The Experimental Situation | 258 |
13.5 Next Generation Experiments | 260 |
13.5.1 What Can Be Achieved from the Ground? | 260 |
13.5.2 Observing Macho Parallax | 261 |
13.6 Working on Gravitational Microlensing | 263 |
13.7 Summary | 264 |
13.7.1 What We Know Now | 264 |
13.7.2 What We Will Learn from Current Experiments | 264 |
13.7.3 Next Generation Experiments | 264 |
13.8 Late Breaking News | 265 |
14 Globally Asymmetric Supernova | 269 |
14.1 Introduction | 269 |
14.1.1 Preamble | 269 |
14.1.2 Evidence for Asymmetry | 270 |
14.1.3 State of the Art | 271 |
14.2 Instability During Core Collapse | 272 |
14.2.1 Accomplishments | 273 |
14.2.2 Future Directions | 273 |
14.3 Overstable Core g-Modes | 274 |
14.3.1 Accomplishments | 275 |
14.3.2 Future Directions | 276 |
14.3.3 Turbulent Excitation of g-Modes | 277 |
15 In and around Neutron Stars | 281 |
15.1 Introduction | 281 |
15.2 Superfluid-Superconductor Interactions in a Neutron Star Core | 284 |
15.3 The Stellar Crust | 288 |
15.4 Spun-up Neutron Stars | 289 |
15.5 Spinning-down Radiopulsars | 293 |
15.6 Glitches of Radiopulsar Spin Periods | 294 |
16 Accretion Flows around Black Holes | 301 |
16.1 Introduction | 301 |
16.2 X-rays and -rays from Accreting Black Holes | 302 |
16.3 Hot Accretion Flow Models | 304 |
16.3.1 Corona Models | 305 |
16.3.2 SLE Two-Temperature Model | 306 |
16.3.3 Optically-Thin Advection-Dominated Model | 306 |
16.4 Directions for Future Research | 311 |
16.4.1 Unresolved Theoretical Issues | 311 |
16.4.2 Clues from Observations of Black Hole XRBs | 313 |
16.4.3 Black Holes versus Neutron Stars | 315 |
16.5 Conclusion | 316 |
17 The Highest Energy Cosmic Rays | 325 |
17.1 Introduction | 325 |
17.2 Review of Existing Data on the Highest Energy Cosmic Rays | 327 |
17.3 Acceleration and Transport of the Cosmic Rays 1019 eV | 329 |
17.4 The Big Events | 332 |
17.5 The Auger Project | 335 |
17.6 What Can We Learn from Two Large Surface Arrays? | 337 |
17.7 Should a Student Work on This Problem? | 338 |
17.8 Final Remark | 339 |
18 Toward Understanding Gamma-Ray Bursts | 343 |
18.1 Introduction | 343 |
18.2 Observations | 344 |
18.2.1 Observational Open Questions | 348 |
18.3 A Brief Summary | 348 |
18.4 Where? | 349 |
18.5 How? | 349 |
18.5.1 The Compactness Problem | 350 |
18.5.2 Relativistic Motion | 351 |
18.5.3 Slowing Down of Relativistic Particles | 354 |
18.5.4 The Acceleration Mechanism? | 362 |
18.6 What? | 364 |
18.6.1 What Do We Need from the Internal Engine? | 364 |
18.6.2 Coincidences and Other Astronomical Hints | 365 |
18.7 Why? | 367 |
18.8 Conclusions | 369 |
18.9 Some Open Questions | 369 |