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List of tables | |
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List of figures | |
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Preface | |
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Overview | |
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Where do we stand? | |
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Why does anyone care? | |
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Stellar evolution | |
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Nuclear energy generation and neutrino fluxes | |
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Uncertainties in the predictions | |
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Experiments are required for progress | |
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The [superscript 37]Cl experiment | |
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The Kamiokande II experiment | |
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A geochemical experiment: [superscript 98]Mo | |
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Gallium detectors | |
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Next-generation experiments | |
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Electronic detection of pp neutrinos | |
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Coherent scattering detectors | |
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Some explanations of the solar neutrino problem | |
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Discriminating among explanations | |
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The next decade | |
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Questions and answers | |
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Stellar structure and evolution | |
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Life history of a star | |
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Basic equations | |
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Principal results | |
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Present status | |
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Nuclear fusion reactions | |
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The essentials | |
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Reaction rates | |
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The pp chain | |
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Neutrino fluxes and terminations of the pp chain | |
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The CNO cycle | |
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Energy generation | |
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What remains to be done? | |
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The standard solar model | |
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The input parameters | |
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General method | |
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Some characteristics of the standard solar model | |
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Helioseismology | |
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Nonstandard solar models | |
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The low Z model | |
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Iron precipitation | |
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A burnt-out core | |
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Rapid rotation | |
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A strong magnetic field | |
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A mixed-up Sun | |
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Turbulent diffusion | |
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Thermal instabilities | |
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Hydrodynamic phenomena | |
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[superscript 3]He instability | |
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Massive mass loss | |
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A central black hole | |
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WIMPs | |
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Q-nuclei | |
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Non-Maxwellian velocity distribution | |
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No [superscript 8]B produced or S[subscript 34] = 0 | |
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CNO reaction dominant | |
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The neutrinos | |
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The neutrino-producing reactions | |
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Information content | |
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Neutrino energy spectra | |
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Solar neutrino fluxes | |
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Fluxes from other stars | |
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Theoretical uncertainties | |
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Logic | |
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Examples | |
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Neutrino cross sections | |
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Power-law dependences | |
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Monte Carlo simulations | |
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Principal uncertainties | |
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Neutrino cross sections | |
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Absorption cross sections | |
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Neutrino-electron scattering cross sections | |
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Neutral currents | |
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Beyond the standard model of electroweak interactions | |
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Vacuum oscillations | |
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Matter oscillations | |
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Neutrino magnetic moment | |
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Neutrino decay | |
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WIMPs | |
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Ockham's razor | |
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The [superscript 37]Cl experiment | |
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Standard model predictions | |
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The experiment | |
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The results | |
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Theory versus experiment: the implications | |
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Do solar neutrino fluxes vary with time? | |
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Recent data | |
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The future of the [superscript 37]Cl experiment | |
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The [superscript 71]Ga experiments | |
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Predictions of the standard model | |
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The experiments | |
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What can be learned? | |
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Geochemical and radiochemical detectors: Mo, Tl, Li, Br, I | |
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[superscript 98]Mo | |
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[superscript 205]Tl | |
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[superscript 7]Li | |
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[superscript 81]Br | |
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[superscript 127]I | |
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Neutrino-electron scattering experiments | |
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Water detectors | |
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Kamiokande II | |
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SUNLAB | |
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LVD | |
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Super Kamiokande: water | |
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Sudbury neutrino observatory: deuterium | |
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ICARUS I: liquid argon | |
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Low-temperature detectors | |
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Direct counting experiments | |
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SNO: D[subscript 2]O | |
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ICARUS: [superscript 40]Ar | |
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[superscript 115]In | |
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BOREX: [superscript 11]B | |
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[superscript 19]F | |
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Coherent scattering detectors | |
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Stellar collapse | |
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How a star gets into trouble | |
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Neutrino emission from a standard stellar collapse | |
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Neutrino bombs: how often and where? | |
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Neutrinos from other galaxies | |
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SN1987A | |
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Expected number of events in detectors | |
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Synopsis and future directions | |
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What is needed | |
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Solar neutrino detectors | |
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Stellar collapses | |
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Stellar evolution | |
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Nuclear physics | |
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Particle physics | |
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The bottom line | |
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An account of the development of the solar neutrino problem, John N. Bahcall and Raymond Davis, Jr. | |
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References | |
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Index | |