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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 $^...
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Lenguaje: | eng |
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2002
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Acceso en línea: | http://cds.cern.ch/record/5691 |
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author | Hornshoj, P |
author_facet | Hornshoj, P |
author_sort | Hornshoj, P |
collection | CERN |
description | This experiment relies on the production of a strong, contamination-free (10$ ^{-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 |