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A search for axions and massive neutrinos

This experiment relies on the production of a strong, contamination-free (10$ ^{-12} $) source of radioactive $^{125}$I at the ISOLDE facility. Technical developments to achieve the necessary beam intensity are in progress. \\ \\The possible emission of axions in the 35.5 keV M1 transition of the $^...

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Autor principal: Hornshoj, P
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:http://cds.cern.ch/record/5691
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author Hornshoj, P
author_facet Hornshoj, P
author_sort Hornshoj, P
collection CERN
description This experiment relies on the production of a strong, contamination-free (10$ ^{-12} $) source of radioactive $^{125}$I at the ISOLDE facility. Technical developments to achieve the necessary beam intensity are in progress. \\ \\The possible emission of axions in the 35.5 keV M1 transition of the $^{125}$Te daughter isotope is searched for by the axion analogue of the Mössbauer effect, i.e. the axion resonance absorption in a $^{125}$Te resonance absorber. For this purpose all other radiation emitted from the source is shielded by a non-resonant absorber, which is transparent, however, to axions. The resonance absorption is detected by measurement of subsequently emitted X-rays. A sensitivity to the axion emission branching ratio in the nuclear decay of 10$ ^{-7} $ is strived for.
id cern-5691
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
record_format invenio
spelling cern-56912020-11-19T09:52:06Zhttp://cds.cern.ch/record/5691engHornshoj, PA search for axions and massive neutrinosNuclear Physics - ExperimentThis experiment relies on the production of a strong, contamination-free (10$ ^{-12} $) source of radioactive $^{125}$I at the ISOLDE facility. Technical developments to achieve the necessary beam intensity are in progress. \\ \\The possible emission of axions in the 35.5 keV M1 transition of the $^{125}$Te daughter isotope is searched for by the axion analogue of the Mössbauer effect, i.e. the axion resonance absorption in a $^{125}$Te resonance absorber. For this purpose all other radiation emitted from the source is shielded by a non-resonant absorber, which is transparent, however, to axions. The resonance absorption is detected by measurement of subsequently emitted X-rays. A sensitivity to the axion emission branching ratio in the nuclear decay of 10$ ^{-7} $ is strived for.oai:cds.cern.ch:56912002
spellingShingle Nuclear Physics - Experiment
Hornshoj, P
A search for axions and massive neutrinos
title A search for axions and massive neutrinos
title_full A search for axions and massive neutrinos
title_fullStr A search for axions and massive neutrinos
title_full_unstemmed A search for axions and massive neutrinos
title_short A search for axions and massive neutrinos
title_sort search for axions and massive neutrinos
topic Nuclear Physics - Experiment
url http://cds.cern.ch/record/5691
work_keys_str_mv AT hornshojp asearchforaxionsandmassiveneutrinos
AT hornshojp searchforaxionsandmassiveneutrinos