| Literature DB >> 28621970 |
J N Wilson1, M Lebois1, L Qi1, P Amador-Celdran2, D Bleuel3, J A Briz4, R Carroll5, W Catford5, H De Witte6, D T Doherty7, R Eloirdi2, G Georgiev8, A Gottardo1, A Goasduff8, K Hadyńska-Klęk9, K Hauschild8, H Hess10, V Ingeberg11, T Konstantinopoulos8, J Ljungvall8, A Lopez-Martens8, G Lorusso12, R Lozeva8, R Lutter13, P Marini14, I Matea1, T Materna7, L Mathieu15, A Oberstedt16, S Oberstedt17, S Panebianco7, Zs Podolyák5, A Porta4, P H Regan5,12, P Reiter10, K Rezynkina6, S J Rose11, E Sahin11, M Seidlitz10, O Serot18, R Shearman5,12, B Siebeck10, S Siem11, A G Smith19, G M Tveten11, D Verney1, N Warr10, F Zeiser11, M Zielinska7.
Abstract
Fast-neutron-induced fission of ^{238}U at an energy just above the fission threshold is studied with a novel technique which involves the coupling of a high-efficiency γ-ray spectrometer (MINIBALL) to an inverse-kinematics neutron source (LICORNE) to extract charge yields of fission fragments via γ-γ coincidence spectroscopy. Experimental data and fission models are compared and found to be in reasonable agreement for many nuclei; however, significant discrepancies of up to 600% are observed, particularly for isotopes of Sn and Mo. This indicates that these models significantly overestimate the standard 1 fission mode and suggests that spherical shell effects in the nascent fission fragments are less important for low-energy fast-neutron-induced fission than for thermal neutron-induced fission. This has consequences for understanding and modeling the fission process, for experimental nuclear structure studies of the most neutron-rich nuclei, for future energy applications (e.g., Generation IV reactors which use fast-neutron spectra), and for the reactor antineutrino anomaly.Entities:
Year: 2017 PMID: 28621970 DOI: 10.1103/PhysRevLett.118.222501
Source DB: PubMed Journal: Phys Rev Lett ISSN: 0031-9007 Impact factor: 9.161