Fission yields at different fission-product kinetic energies for thermal-neutron-induced fission of 239Pu☆
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Cited by (116)
Calorimetric low temperature detectors for heavy ion physics and their application in nuclear and atomic physics
2023, Progress in Particle and Nuclear PhysicsCharge distribution of heavy mass fission products in the thermal neutron induced fission of <sup>233</sup>U, <sup>235</sup>U and <sup>239</sup>Pu
2022, Applied Radiation and IsotopesCitation Excerpt :The IAEA-EXFOR Databases compilation (Izak-Biran and Amiel, 1977; Otsuka et al., 2014) shows that the study of charge distribution of light mass fission products have been done by using different online methods. The online methods used for such study are recoil mass separator for the 233U (nth,f) reaction (Quade et al., 1988), 235U (nth,f) reaction (Lang et al., 1980; Siegert et al., 1976, Clerc et al., 1975) and 239Pu(nth,f) reaction (Schmitt et al., 1984). Similarly, COSIFANTUTTE spectrometer has been used in the 239Pu(nth,f) reaction (Boucheneb et al., 1991) to carry out the charge distribution of light mass fission products.
Stopping power of fission fragments in thin Mylar and nickel foils
2021, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :For some fragments, however, the distribution is strongly deformed and can reach 30+. It is due to the presence of nanosecond isomeric states in the de-excitation cascade that decay in the path between the target and the spectrometer by the ejection of an electron and finally lead to the emission of several electrons in the reorganization of the atomic shell [41,42]. Only few nuclides have such nanosecond isomeric states and setting the spectrometer to a particularly high ionic charge state allows to produce a quasi isotopically pure beam.
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This work forms part of the Ph.D. thesis of C. Schmitt and A. Guessous.