TY - JOUR
T1 - Measurement of the 35Cl(n, p)35S cross-section at the CERN n_TOF facility from subthermal energy to 120 keV
AU - The n_TOF Collaboration
AU - Martinez-Cañadas, Marco Antonio
AU - Torres-Sánchez, Pablo
AU - Praena, Javier
AU - Porras, Ignacio
AU - Sabaté-Gilarte, Marta
AU - Aberle, Oliver
AU - Alcayne, Victor
AU - Amaducci, Simone
AU - Andrzejewski, Józef
AU - Audouin, Laurent
AU - Bécares, Vicente
AU - Babiano-Suarez, Victor
AU - Bacak, Michael
AU - Barbagallo, Massimo
AU - Bečvář, František
AU - Bellia, Giorgio
AU - Berthoumieux, Eric
AU - Billowes, Jon
AU - Bosnar, Damir
AU - Brown, Adam
AU - Busso, Maurizio
AU - Caamaño, Manuel
AU - Caballero, Luis
AU - Calviño, Francisco
AU - Calviani, Marco
AU - Cano-Ott, Daniel
AU - Casanovas, Adria
AU - Cerutti, Francesco
AU - Chen, Yonghao
AU - Chiaveri, Enrico
AU - Colonna, Nicola
AU - Cortés, Guillem
AU - Cortés-Giraldo, Miguel
AU - Cosentino, Luigi
AU - Cristallo, Sergio
AU - Damone, Lucia Anna
AU - Diakaki, Maria
AU - Dietz, Mirco
AU - Domingo-Pardo, César
AU - Dressler, Rugard
AU - Dupont, Emmeric
AU - Durán, Ignacio
AU - Eleme, Zinovia
AU - Fernández-Domínguez, Beatriz
AU - Ferrari, Alfredo
AU - Ferrer, Francisco Javier
AU - Finocchiaro, Paolo
AU - Furman, Valter
AU - Göbel, Kathrin
AU - Rauscher, Thomas
N1 - © The Author(s) 2026. Open Access This article is licensed under a Creative Commons Attribution 4.0 International License. To view a copy of this licence, visit http://creativecommons.org/licenses/by/4.0/.
PY - 2026/5/9
Y1 - 2026/5/9
N2 - The 35Cl(n, p)35S reaction plays a key role in neutron dosimetry for Boron Neutron Capture Therapy, in the synthesis of the isotope 36S, whose astrophysical origin remains unresolved, and in the design of next-generation molten-salt reactors. Its relevance has motivated its inclusion in the High Priority Request List (HPRL) of NEA. The goal of this work is to determine the 35Cl(n, p)35S cross-section from thermal energy to 120 keV for the first time ever in a single measurement, thus reducing systematic uncertainties related to the normalization to the thermal value. This had been a subject of concern in previous evaluations of this reaction. We made use of the Time-of-Flight technique with microMEGAS detectors at Experimental Area 2 (EAR-2) of n_TOF facility at CERN. The 10B(n,α)7Li and 235U(n, f) reactions were used as references. Rutherford Back-scattering Spectrometry was performed at Centro Nacional de Aceleradores (CNA) in Sevilla, in order to accurately determine the masses of the irradiated samples. We obtained a thermal cross-section of 0.470±0.009 barns. The 1/v energy dependence of the cross-section is observed up to the first resonance at 0.398 keV, the resonances up to 120 keV are analyzed and resonance parameters extracted using SAMMY. Maxwellian Averaged Cross-Section (MACS) was calculated for kBT from 1 to 100 keV, and lower values compared to estimations from ENDF were found, e.g., 1.07 ± 0.20 mb at kBT=30 keV. The thermal cross-section and first two resonances are in agreement with the latest evaluation in ENDF/B-VIII.1, while remarkably lower resonance strengths were found for high energy resonances.
AB - The 35Cl(n, p)35S reaction plays a key role in neutron dosimetry for Boron Neutron Capture Therapy, in the synthesis of the isotope 36S, whose astrophysical origin remains unresolved, and in the design of next-generation molten-salt reactors. Its relevance has motivated its inclusion in the High Priority Request List (HPRL) of NEA. The goal of this work is to determine the 35Cl(n, p)35S cross-section from thermal energy to 120 keV for the first time ever in a single measurement, thus reducing systematic uncertainties related to the normalization to the thermal value. This had been a subject of concern in previous evaluations of this reaction. We made use of the Time-of-Flight technique with microMEGAS detectors at Experimental Area 2 (EAR-2) of n_TOF facility at CERN. The 10B(n,α)7Li and 235U(n, f) reactions were used as references. Rutherford Back-scattering Spectrometry was performed at Centro Nacional de Aceleradores (CNA) in Sevilla, in order to accurately determine the masses of the irradiated samples. We obtained a thermal cross-section of 0.470±0.009 barns. The 1/v energy dependence of the cross-section is observed up to the first resonance at 0.398 keV, the resonances up to 120 keV are analyzed and resonance parameters extracted using SAMMY. Maxwellian Averaged Cross-Section (MACS) was calculated for kBT from 1 to 100 keV, and lower values compared to estimations from ENDF were found, e.g., 1.07 ± 0.20 mb at kBT=30 keV. The thermal cross-section and first two resonances are in agreement with the latest evaluation in ENDF/B-VIII.1, while remarkably lower resonance strengths were found for high energy resonances.
UR - https://www.scopus.com/pages/publications/105039184353
U2 - 10.1140/epja/s10050-026-01826-3
DO - 10.1140/epja/s10050-026-01826-3
M3 - Article
AN - SCOPUS:105039184353
SN - 1434-6001
VL - 62
JO - European Physical Journal A
JF - European Physical Journal A
M1 - 90
ER -