Author:
Pirovano E.,Manna A.,Colonna N.,Console Camprini P.,Cosentino L.,Dietz M.,Ducasse Q.,Finocchiaro P.,Massimi C.,Mengoni A.,Nolte R.,Radeck D.,Tassan-Got L.,Terranova N.,Ventura A.,Aberle O.,Alcayne V.,Amaducci S.,Andrzejewski J.,Audouin L.,Babiano-Suarez V.,Bacak M.,Barbagallo M.,Bennett S.,Berthoumieux E.,Billowes J.,Bosnar D.,Brown A.,Busso M.,Caamaño M.,Caballero-Ontanaya L.,Calviño F.,Calviani M.,Cano-Ott D.,Casanovas A.,Cerutti F.,Chiaveri E.,Cortés G.,Cortés-Giraldo M. A.,Cristallo S.,Damone L. A.,Davies P. J.,Diakaki M.,Domingo-Pardo C.,Dressler R.,Dupont E.,Durán I.,Eleme Z.,Fernández-Domínguez B.,Ferrari A.,Göbel K.,Garg R.,Gawlik-Ramie˛ga A.,Gilardoni S.,Gonçalves I. F.,González-Romero E.,Guerrero C.,Gunsing F.,Harada H.,Heinitz S.,Heyse J.,Jenkins D. G.,Junghans A.,Käppeler† F.,Kadi Y.,Kimura A.,Knapová I.,Kokkoris M.,Krtička M.,Kurtulgil D.,Ladarescu I.,Lederer-Woods C.,Leeb H.,Lerendegui-Marco J.,Lonsdale S. J.,Macina D.,Martínez T.,Masi A.,Mastinu P.,Mastromarco M.,Maugeri E. A.,Mazzone A.,Mendoza E.,Michalopoulou V.,Milazzo P. M.,Mingrone F.,Moreno-Soto J.,Musumarra A.,Negret A.,Ogállar F.,Oprea A.,Patronis N.,Pavlik A.,Perkowski J.,Piersanti L.,Petrone C.,Porras I.,Praena J.,Quesada J. M.,Ramos-Doval D.,Rauscher T.,Reifarth R.,Rochman D.,Rubbia C.,Sabaté-Gilarte M.,Saxena A.,Schillebeeckx P.,Schumann D.,Sekhar A.,Smith A. G.,Sosnin N. V.,Sprung P.,Stamatopoulos A.,Tagliente G.,Tain J. L.,Tarifeño-Saldivia A.,Thomas Th.,Torres-Sánchez P.,Tsinganis A.,Ulrich J.,Urlass S.,Valenta S.,Vannini G.,Variale V.,Vaz P.,Vescovi D.,Vlachoudis V.,Vlastou R.,Wallner A.,Woods P. J.,Wright T.,Žugec P.
Abstract
A new measurement of the 235U(n,f) fission cross section was carried out at n_TOF. The experiment covered the neutron energy range from 10 MeV up to 500 MeV, and it used the 1H(n,n) cross section as normalization for the neutron fluence measurement. In this contribution, the measurements and the characterization of the detectors covering the incident energy range up to 150 MeV are discussed.