1996
DOI: 10.1016/0375-9474(95)00509-9
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Nuclear properties according to the Thomas-Fermi model

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Cited by 584 publications
(483 citation statements)
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“…In addition, we also chose to explore a combination of TF fission barriers and FRDM nuclear mass predictions and to gauge the resulting effect. The latter are close to the TF predictions, containing also the same shell corrections (Myers & Swiatecki 1996) and have already been used in some astrophysical rate calculations for nuclei with Z < 84. Figure 4 shows the quantity of primary importance, B f − S n , for the calculation of neutron-induced fission cross sections, based on the two model sets FRDM+TF and ETFSI.…”
Section: Neutron-induced Fission Rates For a Variety Of Mass Modelssupporting
confidence: 80%
“…In addition, we also chose to explore a combination of TF fission barriers and FRDM nuclear mass predictions and to gauge the resulting effect. The latter are close to the TF predictions, containing also the same shell corrections (Myers & Swiatecki 1996) and have already been used in some astrophysical rate calculations for nuclei with Z < 84. Figure 4 shows the quantity of primary importance, B f − S n , for the calculation of neutron-induced fission cross sections, based on the two model sets FRDM+TF and ETFSI.…”
Section: Neutron-induced Fission Rates For a Variety Of Mass Modelssupporting
confidence: 80%
“…With the energy spread of the incident cyclotron beam, the small variation of the beam energy during irradiation, and the energy losses in the target (3.0 MeV), we expected the resulting 297 117 compound nuclei to have excitation energies between 37.2 and 41.4 MeV. Excitation energies of the compound nuclei are calculated using the masses found in [38,39]. The beam energy losses in the separator's entrance window (0.74 mg/cm 2 Ti foil), target backing, and target layer were calculated using the Nuclear Data Tables [40,41].…”
Section: Resultsmentioning
confidence: 99%
“…This could indicate a larger probability for decay by spontaneous fission in preference to β + /EC decay leading to 1 h 267 Rf and 11 s 281 Ds [5]. However, large uncertainties in half-life and/or the calculated β + /EC-decay energy [26,38,39,55,[59][60][61][62] for these isotopes prevent us from drawing definite conclusions.…”
Section: Discussionmentioning
confidence: 97%
“…36 In complete nuclear fusion reactions 292 Fl* compound nuclei at an excitation energy, E*, of 40-45 MeV were formed. 37,38 After deexcitation by evaporation of three or four neutrons, the resulting 288,289 Fl nuclei recoiled from the target into the separator TASCA operated in the "Small Image Mode". 32 The primary beam and unwanted nuclear reaction products were deflected inside the dipole magnet to a beam stop, while Fl was guided to the focal plane (Figure 1).…”
Section: Methodsmentioning
confidence: 99%