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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...

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Autores principales: 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
Publicado: 2012
Materias:
Acceso en línea:https://dx.doi.org/10.1209/0295-5075/98/32001
http://cds.cern.ch/record/1559784
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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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