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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...

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Autores principales: Kavrigin, P, Griesmayer, E, Belloni, F, Plompen, A J M, Schillebeeckx, P, Weiss, C
Lenguaje:eng
Publicado: 2016
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
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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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AT plompenajm 13cnalpha010becrosssectionmeasurementwithscvddiamonddetector
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