Cargando…
Measurement of the $^{16}$O(n, α)$^{13}$C cross-section using a Double Frisch Grid Ionization Chamber
The $^{16}$O(n, α)$^{13}$C reaction was proposed to be measured at the neutron time-of-flight (n_TOF) facility of CERN. To this purpose, a Double Frisch Grid Ionization Chamber (DFGIC) containing the oxygen atoms as a component in the counting gas coupled with a switch device in order to prevent the...
Autores principales: | , , , , , , , , , , , , , , , , |
---|---|
Lenguaje: | eng |
Publicado: |
2020
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1051/epjconf/202023901030 http://cds.cern.ch/record/2800364 |
Sumario: | The $^{16}$O(n, α)$^{13}$C reaction was proposed to be measured at the neutron time-of-flight (n_TOF) facility
of CERN. To this purpose, a Double Frisch Grid Ionization Chamber (DFGIC) containing the oxygen atoms as
a component in the counting gas coupled with a switch device in order to prevent the charge collection from
the so-called γ-flash has been developed at Helmholtz-Zentrum Dresden-Rossendorf (HZDR), in Germany.
The first $^{16}$O(n, α)$^{13}$C measurement without seeing the charge of the γ-flash at n_TOF has been performed in
November 2018. After the electronics did not suffer from the γ-flash any more, another huge charge collection
was discovered. Due to the high instantaneous flux at the n_TOF facility [1] the amount of that induced charge
from neutron induced background reactions was piling up so much that the recognition of $^{16}$O(n, α)$^{13}$C reactions
from that background was very difficult. For that reason another $^{16}$O(n, α)$^{13}$C measurement at the time-of-flight
facility nELBE at HZDR which has a low instantaneous flux [2], has been performed in April 2019. Both measurements from n_TOF and nELBE will be presented here. |
---|