Measurement and analysis of the 243Am neutron capture cross section at the n_TOF facility at CERN
- MENDOZA E.
- CANO-OTT D.
- GUERRERO C.
- BERTHOUMIEUX E.
- ABBONDANNO U.
- AERTS G.
- ALVAREZ-VELARDE F.
- ANDRIAMONJE S.
- ANDRZEJEWSKI J.
- ASSIMAKOPOULOS P.
- AUDOUIN L.
- BADUREK G.
- BAUMANN P.
- Becvár F.
- CALVIÑO F.
- CAPOTE R.
- CARRILLO DE ALBORNOZ A.
- Chepel V
- CHIAVERI E.
- COLONNA N.
- CORTES G.
- COUTURE A.
- COX J.
- DOLFINI R.
- DAVID S.
- DOMINGO-PARDO C.
- KONOVALOV V.
- KARADIMOS D.
- PAVLOPOULOS P.
- DRIDI W.
- DURAN I.
- ELEFTHERIADIS C.
- FERRANT L.
- FERRARI A.
- FERREIRA-MARQUES R.
- FITZPATRICK L.
- FRAIS-KOELBL H
- FUJII K.
- FURMAN W.
- GONCALVES I.
- CENNINI P.
- GONZALEZ-ROMERO E.
- GRIESMAYER E.
- GOVERDOVSKI A.
- GUNSING F.
- HAAS B.
- HAIGHT R.
- HEIL M.
- HERRERA-MARTINEZ A.
- IGASHIRA M.
- ISAEV S.
- JERICHA E.
- KOEHLER P.
- KRTICKA M.
- KERVENO M.
- KADI Y.
- KARAMANIS D.
- LEEB H.
- LAMPOUDIS C.
- MARGANIEC J.
- MASTINU P.
- MENGONI A.
- MILAZZO P. M.
- PARADELA C.
- PAVLIK A.
- PLOMPEN Arjan
- QUESADA J.
- RAUSCHER T.
- REIFARTH R.
- RUBBIA C.
- TAGLIENTE G.
- TAIN J. L.
- TASSAN-GOT L.
- LINDOTE A.
- LOPES I.
- LOZANO M.
- LUKIC S.
- MARRONE S.
- MOREAU C.
- MOSCONI M.
- NEVES F.
- OBERHUMMER H.
- O'BRIEN S.
- PAPADOPOULOS C.
- PATRONIS N.
- PERROT L.
- PLAG R.
- PLUKIS A.
- POCH A.
- PRETEL C.
- RUDOLF G.
- RULLHUSEN P.
- SALGADO J.
- SARCHIAPONE L.
- SAVVIDIS I.
- KÄPPELER F.
- STEPHAN C.
- TAVORA L.
- TERLIZZI R.
- VANNINI G.
- VENTURA A.
- VILLAMARIN D.
- VAZ P.
- VINCENTE M. C.
- VOSS F.
- WIESCHER M.
- WISSHAK K.
- GRAMEGNA F.
- MARQUES L.
- OSHIMA M.
- PANCIN J.
- WENDLER H.
- KETLEROV V.
- MASSIMI C.
- VLASTOU R.
- VLACHOUDIS V.
- BALIBREA J.
- BELLONI F.
- CALVIANI M.
- CARRAPICO C.
- DAHLFORS M.
- DILLMANN I.
- KOSSIONIDES E.
- LO MEO S.
- LOSSITO R.
- MARTINEZ T.
- PAPACHRISTODOULOU C.
- PIGNI M. T.
- PRAENA J.
- SANTOS C.
- WALTER S.
DOIAbstract
Background: The design of new nuclear reactors and transmutation devices requires to reduce the present neutron cross section uncertainties of minor actinides. Purpose: Improvement of the 243Am(n,γ ) cross section uncertainty. Method: The 243Am(n,γ ) cross section has been measured at the n_TOF facility at CERN with a BaF2 total absorption calorimeter, in the energy range between 0.7 eV and 2.5 keV. Results: The 243Am(n,γ ) cross section has been successfully measured in the mentioned energy range. The resolved resonance region has been extended from 250 eV up to 400 eV. In the unresolved resonance region our results are compatible with one of the two incompatible capture data sets available below 2.5 keV. The data available in EXFOR and in...
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