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A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility
This work presents the production and extraction of the short-lived radionuclide (6)He in yet unmatched yields from the ISOLDE facility at CERN. It is the first report of (6)He production using spallation neutrons via the (9)Be(n, alpha)(6)He react ion. These neutrons are produced from the 1.4GeV pr...
Autores principales: | , , , , , , , , , , , |
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Publicado: |
2012
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1209/0295-5075/98/32001 http://cds.cern.ch/record/1559784 |
_version_ | 1780930650192216064 |
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author | Stora, Thierry Noah, Etam Hodak, Rastislav Hirsh, Tsviki Y Hass, Michael Kumar, Vivek Singh, Kuljeet Vaintraub, Sergey Delahaye, Pierre Franberg-Delahaye, Hanna Saint Laurent, Marie-Genevieve Lhersonneau, Gerard |
author_facet | Stora, Thierry Noah, Etam Hodak, Rastislav Hirsh, Tsviki Y Hass, Michael Kumar, Vivek Singh, Kuljeet Vaintraub, Sergey Delahaye, Pierre Franberg-Delahaye, Hanna Saint Laurent, Marie-Genevieve Lhersonneau, Gerard |
author_sort | Stora, Thierry |
collection | CERN |
description | This work presents the production and extraction of the short-lived radionuclide (6)He in yet unmatched yields from the ISOLDE facility at CERN. It is the first report of (6)He production using spallation neutrons via the (9)Be(n, alpha)(6)He react ion. These neutrons are produced from the 1.4GeV proton beam of the Proton Synchrotron Booster (PSB) striking a tungsten converter, and are impinging on a porous BeO material. The central position of (6)He in future experiments is due to its role as a nec essary radioactive nucleus to realize the -beam at CERN, a next-generation facility to study neutrino oscillation parameters, and hence neutrino masses. In the -beam scenario, an intense beam of radioactive (6)He nuclei will be produced, accelerated t o multi-GeV energies and stored in a dedicated storage ring. The resulting virtually mono-directional anti-neutrino beam from the decay of the stored (6)He nuclei will be directed towards a remote underground neutrino detector. A similar beam of, e.g., (1 8)Ne will provide neutrinos, an ideal concept to test CP violation in the neutrino sector. The results of the present experiment demonstrate for the first time that the necessary conditions for the realization of the proposed -beam scheme with anti-neut rinos can be fulfilled. |
id | cern-1559784 |
institution | Organización Europea para la Investigación Nuclear |
publishDate | 2012 |
record_format | invenio |
spelling | cern-15597842019-09-30T06:29:59Zdoi:10.1209/0295-5075/98/32001http://cds.cern.ch/record/1559784Stora, ThierryNoah, EtamHodak, RastislavHirsh, Tsviki YHass, MichaelKumar, VivekSingh, KuljeetVaintraub, SergeyDelahaye, PierreFranberg-Delahaye, HannaSaint Laurent, Marie-GenevieveLhersonneau, GerardA high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facilityAccelerators and Storage RingsDetectors and Experimental TechniquesThis work presents the production and extraction of the short-lived radionuclide (6)He in yet unmatched yields from the ISOLDE facility at CERN. It is the first report of (6)He production using spallation neutrons via the (9)Be(n, alpha)(6)He react ion. These neutrons are produced from the 1.4GeV proton beam of the Proton Synchrotron Booster (PSB) striking a tungsten converter, and are impinging on a porous BeO material. The central position of (6)He in future experiments is due to its role as a nec essary radioactive nucleus to realize the -beam at CERN, a next-generation facility to study neutrino oscillation parameters, and hence neutrino masses. In the -beam scenario, an intense beam of radioactive (6)He nuclei will be produced, accelerated t o multi-GeV energies and stored in a dedicated storage ring. The resulting virtually mono-directional anti-neutrino beam from the decay of the stored (6)He nuclei will be directed towards a remote underground neutrino detector. A similar beam of, e.g., (1 8)Ne will provide neutrinos, an ideal concept to test CP violation in the neutrino sector. The results of the present experiment demonstrate for the first time that the necessary conditions for the realization of the proposed -beam scheme with anti-neut rinos can be fulfilled.oai:cds.cern.ch:15597842012 |
spellingShingle | Accelerators and Storage Rings Detectors and Experimental Techniques Stora, Thierry Noah, Etam Hodak, Rastislav Hirsh, Tsviki Y Hass, Michael Kumar, Vivek Singh, Kuljeet Vaintraub, Sergey Delahaye, Pierre Franberg-Delahaye, Hanna Saint Laurent, Marie-Genevieve Lhersonneau, Gerard A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility |
title | A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility |
title_full | A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility |
title_fullStr | A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility |
title_full_unstemmed | A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility |
title_short | A high intensity $^{6}$He beam for the $\beta$-beam neutrino oscillation facility |
title_sort | high intensity $^{6}$he beam for the $\beta$-beam neutrino oscillation facility |
topic | Accelerators and Storage Rings Detectors and Experimental Techniques |
url | https://dx.doi.org/10.1209/0295-5075/98/32001 http://cds.cern.ch/record/1559784 |
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