Cargando…
$^{13}$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: | , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2016
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epja/i2016-16179-9 http://cds.cern.ch/record/2262102 |
Sumario: | 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. |
---|