Antineutrino induced electron capture is a resonant process that can have a large cross-section for beams of monochromatic antineutrinos. We calculate the cross-section of this process and investigate an experimental setup where monochromatic antineutrinos are produced from the bound-beta decay of fully ionized radioactive atoms in a storage ring. If the energy between the source and the target is well matched, the cross-sections can be significantly larger than the cross-sections of commonly used non-resonant processes. The rate that can be achieved at a small distance between the source and two targets of 10(3) kg is up to one interaction per 8.3a <...10(18) decaying atoms. For a source-target distance corresponding to the first atmospheric neutrino oscillation maximum, the largest rate is one interaction per 3.2a <...10(21) decaying atoms, provided that extremely stringent monochromaticity conditions (10(-7) or better) are achieved in future ion beams.

Resonant antineutrino induced electron capture with low energy bound-beta beams

OLDEMAN, RUDOLF GERHARD CHRISTIAAN;SAITTA, BIAGIO
2010-01-01

Abstract

Antineutrino induced electron capture is a resonant process that can have a large cross-section for beams of monochromatic antineutrinos. We calculate the cross-section of this process and investigate an experimental setup where monochromatic antineutrinos are produced from the bound-beta decay of fully ionized radioactive atoms in a storage ring. If the energy between the source and the target is well matched, the cross-sections can be significantly larger than the cross-sections of commonly used non-resonant processes. The rate that can be achieved at a small distance between the source and two targets of 10(3) kg is up to one interaction per 8.3a <...10(18) decaying atoms. For a source-target distance corresponding to the first atmospheric neutrino oscillation maximum, the largest rate is one interaction per 3.2a <...10(21) decaying atoms, provided that extremely stringent monochromaticity conditions (10(-7) or better) are achieved in future ion beams.
2010
Beta beams; Resonant processes; Electron capture
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11584/106360
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