Results of the 244Cm, 246Cm and 248Cm neutron-induced capture cross sections measurements at EAR1 and EAR2 of the n_TOF facility
Metadatos
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Alcayne, V.; Ogállar Ruiz, Francisco; Porras Sánchez, José Ignacio; Praena Rodríguez, Antonio Javier; Torres Sánchez, PabloEditorial
EDP Sciences
Fecha
2023-05-26Referencia bibliográfica
Alcayne, V. et al. Results of the 244Cm, 246Cm and 248Cm neutron-induced capture cross sections measurements at EAR1 and EAR2 of the n_TOF facility. EPJ Web of Conferences , 01009 (2023)284 ND2022. [https://doi.org/10.1051/epjconf/202328401009]
Patrocinador
MCIN/AEI/10.13039/501100011033 I+D+i PGC2018-096717-B-C21; European Commission H2020 Framework Programme SANDA 847552Resumen
Accurate neutron capture cross section data for minor actinides (MAs) are required to estimate the production and transmutation rates of MAs in light water reactors, critical fast reactors like Gen-IV systems, and other innovative reactor systems such as accelerator driven systems (ADS). In particular, Cm-244, Cm-246 and Cm-248 play a role in the transport, storage and transmutation of the nuclear waste of the current nuclear reactors, due to the contribution of these isotopes to the radiotoxicity, neutron emission, and decay heat in the spent nuclear fuel. Also, capture reactions in these Cm isotopes open the path for the formation of heavier elements. In this work, the results of the capture cross section measurement on Cm-244, Cm-246 and Cm-248 performed at the CERN n_TOF facility are presented. It is important to notice that the Cm samples used in the experiment at n_TOF have been used previously in an experiment at J-PARC, this experiment and the previous one done in the 70s with a nuclear explosion were the only previous capture experiments for these isotopes. At n_TOF, the capture cross section measurements of (244)cm, Cm-246 and Cm-248 were performed at the 20 m vertical flight path (EAR2) with three C6D6 total energy detectors. In addition, the cross section of Cm-244 was measured at the 185 m flight path (EAR1) with a Total Absorption Calorimeter (TAC). The combination of measurements in EAR1 and EAR2 has contributed to controlling and reducing the systematic uncertainties in the results. The compatibility of the different measurements performed and the techniques to obtain the results are presented in this paper as well as the procedure to obtain the resonance parameters.