The CERN n_TOF facility: Neutron beams performances for cross section measurements
- CHIAVERI E.
- ALTSTADT S.
- ANDRZEJEWSKI J.
- AUDOUIN L.
- BARBAGALLO M.
- BECARES V.
- Becvár F.
- BELLONI F.
- BERTHOUMIEUX E.
- BILLOWES J.
- BOCCONE V.
- BOSNAR D.
- CALVIANI M.
- BRUGGER M.
- CALVIÑO F.
- CANO-OTT D.
- CARRAPIÇO C.
- CERUTTI F.
- CHIN M.
- CORTES G.
- CORTES-GIRALDO M. A.
- COLONNA N.
- DIAKAKI M.
- DOMINGO-PARDO C.
- DURAN I.
- DZYSIUK N.
- ELEFTHERIADIS C.
- FERRARI A.
- TASSAN-GOT L.
- FRAVAL K.
- GANESAN S.
- GARCIA A. R.
- GIUBRONE G.
- GOMEZ-HORNILLOS M. B.
- GONZALEZ-ROMERO E.
- GONÇALVES I.
- GRIESMAYER E.
- GUERRERO C.
- GUNSING F.
- GURUSAMY P.
- JENKINS D. G.
- JERICHA E.
- KADI Y.
- KARADIMOS D.
- KÄPPELER F.
- KOEHLER P.
- KOKKORIS M.
- KROLL J.
- Krticka M.
- LANGER C.
- LEDERER C.
- LEEB H.
- LOSITO R.
- MANOUSOS A
- MARGANIEC J.
- MARTÍNEZ T.
- MASSIMI C.
- MASTINU P.
- MASTROMARCO M.
- MEAZE M.
- MENDOZA E.
- MENGONI A.
- MILAZZO P. M.
- MINGRONE F.
- MIREA M.
- MONDELAERS Willy
- PAVLIK Andreas
- PERKOWSKI J.
- PLOMPEN Arjan
- PRAENA J.
- QUESADA J.
- RAUSCHER T.
- REIFARTH R.
- RIEGO A.
- ROMAN F.
- RUBBIA C.
- SARMENTO R.
- SCHILLEBEECKX Peter
- SCHMIDT S.
- TAGLIENTE G.
- TAIN J. L.
- TSINGANIS A.
- VALENTA S.
- VANNINI G.
- VARIALE V.
- VAZ P.
- VENTURA A.
- VERMEULEN M.
- VERSACI R.
- VLACHOUDIS V.
- VLASTOU R.
- WALLNER A.
- WARE T.
- WEIGAND M.
- WEISS C.
- WRIGHT T. J.
- ZUGEC P.
- DRESSLER R.
- HERNANDEZ-PRIETO A.
- KIVEL Niko
- LAMPOUDIS C.
- LEAL-CIDONCHA E.
- MALLICK A.
- ROBLES M. S.
- SABATE-GILARTE M
- SAXENA A.
- SCHUMANN D.
- PARADELA C.
- LEONG L. S.
- TARRIO D.
Publication date
October 2014
DOI Publisher
Elsevier BV ISSN
0090-3752 Journal
Nuclear Data Sheets Citation count (estimate)
4Abstract
This paper presents the characteristics of the existing CERN n_TOF neutron beam facility (n_TOF-EAR1 with a flight path of 185 meters) and the future one (n_TOF EAR-2 with a flight path of 19 meters), which will operate in parallel from Summer 2014. The new neutron beam will provide a 25 times higher neutron flux delivered in 10 times shorter neutron pulses, thus offering more powerful capabilities for measuring small mass, low cross section and/or high activity samples.JRC.D.4-Standards for Nuclear Safety, Security and Safeguard
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