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Beta Beams : Neutrino Beams.

The beta-beam concept for the generation of electron neutrino beams was first proposed by Piero Zucchelli in 2002. The idea created quite a stir, challenging the idea that intense neutrino beams only could be produced from the decay of pions or muons in classical neutrino beams facilities or in futu...

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Detalles Bibliográficos
Clasificación:Libro Electrónico
Formato: Electrónico eBook
Idioma:Inglés
Publicado: World Scientific 2009.
Temas:
Acceso en línea:Texto completo

MARC

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505 0 |a Cover13; -- Contents -- Acknowledgments -- Foreword -- 1. Introduction -- 1.1 Neutrino Oscillations -- 1.1.1 Experiments -- 1.1.2 Phenomenology -- 1.2 Three-family Oscillations and CP or T Violation -- 1.2.1 How to measure leptonic CP violation -- 1.2.2 The problem of degenerate solutions -- 1.3 Experimental Setups -- 1.3.1 Conventional neutrino beams -- 1.3.2 First generation long-baseline experiments -- 1.3.3 Second generation long-baseline experiments -- 1.3.4 Next generation conventional neutrino beams -- 1.4 Why Look For New Concepts in Neutrino Beams? -- 1.5 New Concepts on Neutrino Beams -- 1.5.1 Neutrino factories -- 2. Machine Aspects -- 2.1 Introduction -- 2.2 A Possible Beta-Beam Facility -- 2.3 The Beta BeamIsotopes -- 2.3.1 Which isotope to use -- 2.3.2 Isotope production -- 2.3.3 The ISOLmethod -- 2.3.4 Direct production -- 2.3.5 Production ring -- 2.3.6 Production rates -- 2.4 Ion Transfer, Ionization and Bunching -- 2.5 Acceleration -- 2.5.1 Linear accelerators -- 2.5.2 Some basics about synchrotrons -- 2.6 Stacking and Storage -- 2.6.1 Why do we need stacking? -- 2.6.2 Beam-cooling -- 2.6.3 Stacking -- 2.6.4 Annual rate of neutrinos -- 2.6.5 Other limitations -- 2.7 Possible Future Development -- 2.7.1 Accumulation at low energy -- 2.7.2 Two isotopes in the ring at the same time -- 2.7.3 Higher gamma -- 2.7.4 Barrier buckets in the decay ring -- 2.7.5 Acceleration of partly stripped ions -- 3. CERN-Fr180;ejus Beta Beam Physics Potential -- 3.1 Introduction -- 3.2 The CERN-Fr180;ejus Configuration -- 3.3 Data Analysis -- 3.3.1 Backgrounds -- 3.3.2 Signals -- 3.3.3 Systematic errors -- 3.4 Oscillation Analysis -- 3.4.1 952;13 searches -- 3.4.2 Leptonic CP violation searches -- 3.4.3 Searches that cannot be done in this con.guration -- 3.5 Combined Analyses with the Atmospheric Neutrinos -- 3.5.1 Mass hierarchy -- 3.5.2 Degeneracy breaking -- 3.6 Combined Analyses with the SPL Super Beam -- 3.7 Comparison with Other Super Beam Experiments -- 4. Physics Potential of Other Beta Beam Settings -- 4.1 Introduction -- 4.2 High Energy Beta Beams -- 4.3 Monochromatic Neutrino Beams -- 4.4 Beta Beams Based on 8B and 8Li Ions -- 4.5 High Energy 8B/8LiBeta Beams -- 4.6 Comparison with Other Neutrino Facilities and Green-.eld Scenarios -- 4.7 Conclusions -- 5. Low Energy Beta Beams -- 5.1 Introduction -- 5.2 Low Energy Setups -- 5.2.1 Off-axis configurations -- 5.3 Nuclear Structure, Neutrino-nucleus, Nuclear Astrophysics Applications -- 5.4 Fundamental Interaction Studies -- 5.4.1 Weinberg angle measurement -- 5.4.2 Conserved vector current hypothesis -- 5.4.3 Neutrino magnetic moment -- Bibliography -- Index. 
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650 6 |a Neutrinos. 
650 6 |a Faisceaux de neutrons. 
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650 7 |a Neutron beams  |2 fast 
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