Author:
Alcayne V.,Cano-Ott D.,Garcia J.,González-Romero E.,Martínez T.,Mendoza E.,Sánchez A.,Plaza J.,Balibrea-Correa J.,Casanovas A.,Domingo-Pardo C.,Lerendegui-Marco J.,Aberle O.,Altieri S.,Amaducci S.,Amar Es-Sghir H.,Andrzejewski J.,Babiano-Suarez V.,Bacak M.,Balibrea J.,Bennett S.,Bernardes A. P.,Berthoumieux E.,Bosnar D.,Busso M.,Caamaño M.,Calviño F.,Calviani M.,Cano-Ott D.,Casanovas A.,Castelluccio D. M.,Cerutti F.,Cescutti G.,Chasapoglou S.,Chiaveri E.,Colombetti P.,Colonna N.,Console Camprini P. C.,Cortés G.,Cortés-Giraldo M. A.,Cosentino L.,Cristallo S.,Di Castro M.,Diacono D.,Diakaki M.,Dietz M.,Domingo-Pardo C.,Dressler R.,Dupont E.,Durán I.,Eleme Z.,Fargier S.,Fernández-Domínguez B.,Finocchiaro P.,Fiore S.,Furman V.,García-Infantes F.,Gawlik-Ramięga A.,Gervino G.,Gilardoni S.,González-Romero E.,Guerrero C.,Gunsing F.,Gustavino C.,Heyse J.,Jenkins D. G.,Jericha E.,Junghans A.,Kadi Y.,Katabuchi T.,Knapová I.,Kokkoris M.,Kopatch Y.,Krtička M.,Kurtulgil D.,Ladarescu I.,Lederer-Woods C.,Lerendegui-Marco J.,Lerner G.,Manna A.,Martínez T.,Masi A.,Massimi C.,Mastinu P.,Mastromarco M.,Matteucci F.,Maugeri E. A.,Mazzone A.,Mendoza E.,Mengoni A.,Michalopoulou V.,Milazzo P. M.,Mucciola R.,Murtas† F.,Musacchio-Gonzalez E.,Musumarra A.,Negret A.,Oprea A.,Pérez-Maroto P.,Patronis N.,Pavón-Rodríguez J. A.,Pellegriti M. G.,Perkowski J.,Petrone C.,Piersanti L.,Pirovano E.,Pomp S.,Porras I.,Praena J.,Protti N.,Quesada J. M.,Rauscher T.,Reifarth R.,Rochman D.,Romanets Y.,Romano F.,Rubbia C.,Sánchez A.,Sabaté-Gilarte M.,Schillebeeckx P.,Schumann D.,Sekhar A.,Smith A. G.,Sosnin N. V.,Spelta M.,Stamati M. E.,Tagliente G.,Tarifeño-Saldivia A.,Tarrío D.,Terranova N.,Torres-Sánchez P.,Urlass S.,Valenta S.,Variale V.,Vaz P.,Vescovi D.,Vlachoudis V.,Vlastou R.,Wallner A.,Woods P. J.,Wright T.,Žugec P.,
Abstract
The neutron time-of-flight facility n_TOF is characterised by its high instantaneous neutron intensity, high-resolution and broad neutron energy spectra, specially conceived for neutron-induced reaction cross section measurements. Two Time-Of-Flight (TOF) experimental areas are available at the facility: experimental area 1 (EAR1), located at the end of the 185 m horizontal flight path from the spallation target, and experimental area 2 (EAR2), placed at 20 m from the target in the vertical direction. The neutron fluence in EAR2 is ˜ 300 times more intense than in EAR1 in the relevant time-of-flight window. EAR2 was designed to carry out challenging cross-section measurements with low mass samples (approximately 1 mg), reactions with small cross-sections or/and highly radioactive samples. The high instantaneous fluence of EAR2 results in high counting rates that challenge the existing capture systems. Therefore, the sTED detector has been designed to mitigate these effects. In 2021, a dedicated campaign was done validating the performance of the detector up to at least 300 keV neutron energy. After this campaign, the detector has been used to perform various capture cross section measurements at n_TOF EAR2.