AERTS, G.; ABBONDANNO, U.; ÁLVAREZ, H.; ALVAREZ-VELARDE, F.; ANDRIAMONJE, S.; MOSCONI, M.; MENGONI, A.; HEIL, M.; KÄPPELER, F.; TERLIZZI, R.; FURMAN, W.; KETLEROV, V.; GOVERDOVSKI, A.; KONOVALOV, V.; ANDRZEJEWSKI, J.; ASSIMAKOPOULOS, P.; AUDOUIN, L.; BADUREK, G.; BAUMANN, P.; BECVÁR, F.; BENLLIURE, J.; BERTHOUMIEUX, E.; CALVIÑO, F.; CANO-OTT, D.; CAPOTE, R.; CARRILLO DE ALBORNOZ, A.; CENNINI, P.; CHEPEL, V.; CHIAVERI, E.; COLONNA, N.; CORTES, G.; CORTINA, D.; COUTURE, A.; COX, J.; DAVID, S.; DOLFINI, R.; DOMINGO-PARDO, C.; DRIDI, W.; DURAN, I.; EMBID-SEGURA, M.; FERRANT, L.; FERRARI, Anthony; FERREIRA-MARQUES, R.; FITZPATRICK, L.; FRAIS-KÖLBL, H.; FUJII, K.; GUERRERO, C.; GONCALVES, I.; GALLINO, R.; GONZALEZ-ROMERO, E.; GRAMEGNA, F.; GRIESMAYER, E.; GUNSING, F.; HAAS, B.; HAIGHT, R.; HERRERA-MARTINEZ, A.; IGASHIRA, M.; ISAEV, S.; JERICHA, E.; KADI, Y.; KARAMANIS, D.; KARADIMOS, D.; KERVENO, M.; KOEHLER, P.; KOLOKOLOV, D.; KOSSIONIDES, E.; KRTICKA, M.; LAMBOUDIS, C.; LEEB, H.; LINDOTE, A.; LOPES, I.; LOZANO, M.; LUKIC, S.; MARGANIEC, J.; MARQUES, L.; MARRONE, S.; MASTINU, P.; M. MILAZZO, P.; MOREAU, C.; NEVES, F.; OBERHUMMER, H.; O'BRIEN, S.; OSHIMA, M.; PANCIN, J.; PAPACHRISTODOULOU, C.; PAPADOPOULOS, C.; PARADELA, C.; PATRONIS, N.; PAVLIK, A.; PAVLOPOULOS, P.; PERROT, L.; PLAG, R.; PLOMPEN, A.; PLUKIS, A.; POCH, A.; PRETEL, C.; QUESADA, J.; RAUSCHER, T.; REIFARTH, R.; ROSETTI, M.; RUBBIA, C.; RUDOLF, G.; RULLHUSEN, P.; SALGADO, J.; SARCHIAPONE, L.; STEPHAN, C.; TAGLIENTE, G.; L. TAIN, J.; TASSAN-GOT, L.; TAVORA, L.; VANNINI, G.; VAZ, P.; VENTURA, A.; VILLAMARIN, D.; C. VINCENTE, M.; VLACHOUDIS, V.; VLASTOU, R.; VOSS, F.; WENDLER, H.; WIESCHER, M.; WISSHAK, K.

doi:10.1063/1.1945282

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Proceedings of the International Conference on Nuclear Data for Science and Technology, Proceedings of the International Conference on Nuclear Data for Science and Technology, 2004-09-26, Santa Fe. 2005, vol. 769, n° 769, p. 1470-1473

American Institute of Physics

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The use of a fuel cycle based on 232Th can substantially reduce the radiotoxicity of the produced nuclear waste since the lower atomic and mass number of thorium results in a strongly suppressed build-up of the higher actinides and especially americium and curium. The design and realization of nuclear power stations based on the use of thorium, either in a critical or subcritical system, require an accurate knowledge of the 232Th(n,gamma) reaction cross section. We have measured the neutron capture cross section of 232Th at the recently constructed neutron time-of-flight facility n_TOF at CERN in the energy range from 1 eV to 1 MeV. In the resolved resonance region, the resonance parameters have been extracted. In the unresolved resonance region, the neutron capture cross section is given as point-wise data. ©2005 American Institute of Physics< Réduire

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Measurement of the $^{232}$Th Neutron Capture Cross Section at the CERN n_TOF Facility

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