TY - JOUR
T1 - Pushing the high count rate limits of scintillation detectors for challenging neutron-capture experiments
AU - The n TOF Collaboration (www.cern.ch/ntof)
AU - Balibrea-Correa, J.
AU - Lerendegui-Marco, J.
AU - Babiano-Suarez, V.
AU - Domingo-Pardo, C.
AU - Ladarescu, I.
AU - Tarifeño-Saldivia, A.
AU - Fuente-Rosales, G. de la
AU - Alcayne, V.
AU - Cano-Ott, D.
AU - González-Romero, E.
AU - Martínez, T.
AU - Mendoza, E.
AU - de Rada, A. Pérez
AU - del Olmo, J. Plaza
AU - Sánchez-Caballero, A.
AU - Casanovas, A.
AU - Calviño, F.
AU - Valenta, S.
AU - Aberle, O.
AU - Altieri, S.
AU - Amaducci, S.
AU - Andrzejewski, J.
AU - Bacak, M.
AU - Beltrami, C.
AU - Bennett, S.
AU - Bernardes, A. P.
AU - Berthoumieux, E.
AU - Beyer, R.
AU - Boromiza, M.
AU - Bosnar, D.
AU - Caamaño, M.
AU - Calviani, M.
AU - Castelluccio, D. M.
AU - Cerutti, F.
AU - Cescutti, G.
AU - Chasapoglou, S.
AU - Chiaveri, E.
AU - Colombetti, P.
AU - Colonna, N.
AU - Camprini, P. Console
AU - Cortés, G.
AU - Cortés-Giraldo, M. A.
AU - Cosentino, L.
AU - Cristallo, S.
AU - Dellmann, S.
AU - Di Castro, M.
AU - Di Maria, S.
AU - Diakaki, M.
AU - Dietz, M.
AU - Jenkins, D. G.
N1 - Publisher Copyright:
© 2024 The Author(s)
PY - 2024/7
Y1 - 2024/7
N2 - One of the critical aspects for the accurate determination of neutron capture cross sections when combining time-of-flight and total energy detector techniques is the characterization and control of systematic uncertainties associated to the measuring devices. In this work we explore the most conspicuous effects associated to harsh count rate conditions: dead-time and pile-up effects. Both effects, when not properly treated, can lead to large systematic uncertainties and bias in the determination of neutron cross sections. In the majority of neutron capture measurements carried out at the CERN n_TOF facility, the detectors of choice are the C6D6 liquid-based either in form of large-volume cells or recently commissioned sTED detector array, consisting of much smaller-volume modules. To account for the aforementioned effects, we introduce a Monte Carlo model for these detectors mimicking harsh count rate conditions similar to those happening at the CERN n_TOF 20 m flight path vertical measuring station. The model parameters are extracted by comparison with the experimental data taken at the same facility during 2022 experimental campaign. We propose a novel methodology to consider both, dead-time and pile-up effects simultaneously for these fast detectors and check the applicability to experimental data from 197Au(n, γ), including the saturated 4.9 eV resonance which is an important component of normalization for neutron cross section measurements.
AB - One of the critical aspects for the accurate determination of neutron capture cross sections when combining time-of-flight and total energy detector techniques is the characterization and control of systematic uncertainties associated to the measuring devices. In this work we explore the most conspicuous effects associated to harsh count rate conditions: dead-time and pile-up effects. Both effects, when not properly treated, can lead to large systematic uncertainties and bias in the determination of neutron cross sections. In the majority of neutron capture measurements carried out at the CERN n_TOF facility, the detectors of choice are the C6D6 liquid-based either in form of large-volume cells or recently commissioned sTED detector array, consisting of much smaller-volume modules. To account for the aforementioned effects, we introduce a Monte Carlo model for these detectors mimicking harsh count rate conditions similar to those happening at the CERN n_TOF 20 m flight path vertical measuring station. The model parameters are extracted by comparison with the experimental data taken at the same facility during 2022 experimental campaign. We propose a novel methodology to consider both, dead-time and pile-up effects simultaneously for these fast detectors and check the applicability to experimental data from 197Au(n, γ), including the saturated 4.9 eV resonance which is an important component of normalization for neutron cross section measurements.
KW - Dead-time
KW - Pile-up
KW - Pulse-height weighting technique
KW - Radiative capture
KW - Time-of-flight
KW - Total energy detector
UR - http://www.scopus.com/inward/record.url?scp=85191660097&partnerID=8YFLogxK
U2 - 10.1016/j.nima.2024.169385
DO - 10.1016/j.nima.2024.169385
M3 - Article
AN - SCOPUS:85191660097
SN - 0168-9002
VL - 1064
JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
M1 - 169385
ER -