G. Tagliente,O. Aberle,V. Alcayne,S. Amaducci,J. Andrzejewski,V. Babiano-Suarez,M. Bacak,J. Balibrea Correa,A. P. Bernardes,E. Berthoumieux,R. Beyer,M. Boromiza,D. Bosnar,M. Caamano,F. Calvino,M. Calviani,D. Cano-Ott,A. Casanovas,D. M. Castelluccio,F. Cerutti,G. Cescutti,S. Chasapoglou,E. Chiaveri,G. Claps,P. Colombetti,N. Colonna,P. Console Camprini,G. Cortes,M. A. Cortes-Giraldo,L. Cosentino,S. Cristallo,S. Dellmann,D. Diacono,M. Di Castro,M. Diakaki,M. Dietz,C. Domingo-Pardo,R. Dressler,E. Dupont,I. Duran,Z. Eleme,M. Eslami,S. Fargier,B. Fernandez-Dominguez,P. Finocchiaro,V. Furman,A. Gandhi,F. Garcia-Infantes,A. Gawlik-Ramiega,G. Gervino,S. Gilardoni,E. Gonzalez-Romero,S. Goula,E. Griesmayer,C. Guerrero,F. Gunsing,C. Gustavino,J. Heyse,W. Hillman,D. G. Jenkins,E. Jericha,A. Junghans,Y. Kadi,K. Kaperoni,M. Kokkoris,D. Koll,Y. Kopatch,M. Krticka,N. Kyritsis,I. Ladarescu,C. Lederer-Woods,J. Lerendegui-Marco,G. Lerner,A. Manna,T. Martinez,A. Masi,C. Massimi,P. Mastinu,M. Mastromarco,E. A. Maugeri,A. Mazzone,E. Mendoza,A. Mengoni,V. Michalopoulou,P. M. Milazzo,R. Mucciola,E. Musacchio-Gonzalez,A. Musumarra,A. Negret,A. Perez de Rada,P. Perez-Maroto,N. Patronis,J. A. Pavon-Rodriguez,M. G. Pellegriti,J. Perkowski,C. Petrone,L. Piersanti,E. Pirovano,J. Plaza del Olmo,S. Pomp,I. Porras,J. Praena,J. M. Quesada,R. Reifarth,D. Rochman,Y. Romanets,A. Rooney,C. Rubbia,A. Sanchez-Caballero,M. Sabate-Gilarte,D. Scarpa,P. Schillebeeckx,D. Schumann,A. G. Smith,N. V. Sosnin,M. Spelta,M. E. Stamati,A. Tamburrino,A. Tarifeno-Saldivia,D. Tarrio,P. Torres-Sanchez,S. Tosi,G. Tsiledakis,S. Valenta,P. Vaz,G. Vecchio,D. Vescovi,V. Vlachoudis,R. Vlastou,A. Wallner,C. Weiss,P. J. Woods,T. Wright,P. Zugee
16TH VARENNA CONFERENCE ON NUCLEAR REACTION MECHANISMS, NRM 2023（2024）
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摘要
The neutron Time-of-Flight facility (n_TOF) is an innovative facility operative since 2001 at CERN, with three experimental areas. In this paper the n_TOF facility will be described, together with the upgrade of the facility during the Long Shutdown 2 at CERN. The main features of the detectors used for capture fission cross section measurements will be presented with perspectives for the future measurements.
