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$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector
This paper presents$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurements performed at the Van de Graaff facility of the Joint Research Centre Geel. The$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section was measured relative to the$^{12}$C(n, $\alpha_{0}$ )$^{9}$Be cross section at 14.3 MeV a...
Autores principales: | , , , , , |
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Lenguaje: | eng |
Publicado: |
2016
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epja/i2016-16179-9 http://cds.cern.ch/record/2262102 |
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author | Kavrigin, P Griesmayer, E Belloni, F Plompen, A J M Schillebeeckx, P Weiss, C |
author_facet | Kavrigin, P Griesmayer, E Belloni, F Plompen, A J M Schillebeeckx, P Weiss, C |
author_sort | Kavrigin, P |
collection | CERN |
description | This paper presents$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurements performed at the Van de Graaff facility of the Joint Research Centre Geel. The$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section was measured relative to the$^{12}$C(n, $\alpha_{0}$ )$^{9}$Be cross section at 14.3 MeV and 17.0 MeV neutron energies. The measurements were performed with an sCVD (single-crystal chemical vapor deposition) diamond detector which acted as sample and as sensor simultaneously. A novel analysis technique was applied, which is based on the pulse-shape analysis of the detector’s ionization current. This technique resulted in an efficient separation of background events and consequently in a well-determined selection of the nuclear reaction channels$^{12}$C(n, $\alpha_{0}$ )$^{9}$Be and$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be. |
id | oai-inspirehep.net-1472230 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2016 |
record_format | invenio |
spelling | oai-inspirehep.net-14722302019-09-30T06:29:59Zdoi:10.1140/epja/i2016-16179-9http://cds.cern.ch/record/2262102engKavrigin, PGriesmayer, EBelloni, FPlompen, A J MSchillebeeckx, PWeiss, C$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detectorNuclear Physics - ExperimentThis paper presents$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurements performed at the Van de Graaff facility of the Joint Research Centre Geel. The$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section was measured relative to the$^{12}$C(n, $\alpha_{0}$ )$^{9}$Be cross section at 14.3 MeV and 17.0 MeV neutron energies. The measurements were performed with an sCVD (single-crystal chemical vapor deposition) diamond detector which acted as sample and as sensor simultaneously. A novel analysis technique was applied, which is based on the pulse-shape analysis of the detector’s ionization current. This technique resulted in an efficient separation of background events and consequently in a well-determined selection of the nuclear reaction channels$^{12}$C(n, $\alpha_{0}$ )$^{9}$Be and$^{13}$C(n, $\alpha_{0}$ )$^{10}$Be.oai:inspirehep.net:14722302016 |
spellingShingle | Nuclear Physics - Experiment Kavrigin, P Griesmayer, E Belloni, F Plompen, A J M Schillebeeckx, P Weiss, C $^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector |
title | $^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector |
title_full | $^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector |
title_fullStr | $^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector |
title_full_unstemmed | $^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector |
title_short | $^{13}$C(n, $\alpha_{0}$ )$^{10}$Be cross section measurement with sCVD diamond detector |
title_sort | $^{13}$c(n, $\alpha_{0}$ )$^{10}$be cross section measurement with scvd diamond detector |
topic | Nuclear Physics - Experiment |
url | https://dx.doi.org/10.1140/epja/i2016-16179-9 http://cds.cern.ch/record/2262102 |
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