1982
DOI: 10.1016/0375-9474(82)90535-8
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Empirical saddle-point and ground-state masses as a probe of the droplet model

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Cited by 94 publications
(87 citation statements)
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“…The same is at the end of nuclear stability for the heaviest nuclei. At the same time, this component disappears in going from Hs to Cn nuclei according to the model calculations [30,[44][45][46][47]. So fission barriers for the Figure 8) and without it along with a different scaling for the LD fission barriers are shown by different lines for both the reactions.…”
Section: Cnr*11mentioning
confidence: 78%
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“…The same is at the end of nuclear stability for the heaviest nuclei. At the same time, this component disappears in going from Hs to Cn nuclei according to the model calculations [30,[44][45][46][47]. So fission barriers for the Figure 8) and without it along with a different scaling for the LD fission barriers are shown by different lines for both the reactions.…”
Section: Cnr*11mentioning
confidence: 78%
“…In the same way the macroscopic components of fission barriers for the heavier nuclei from Rn to Th were obtained, but in this case only very asymmetric combinations were considered in the SM analysis. These data are shown in Figure 6 together with the predictions of different models [30,[44][45][46][47] and tabulated values [48] for the macroscopic barriers (bottom panels). Shell corrections calculated in [17] and those obtained in the framework of the present analysis (see Section 2) could be also compared (upper panels).…”
Section: Er Production In the Vicinity Of N=126 Shellmentioning
confidence: 99%
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“…The macroscopic components of the barriers B m = k f B LD derived from the analysis of Fr and Ra data [9,10] are lower than any predictions [2,3,11] (apart the values from [12]). The B m values are about a smooth function of N , e.g., for Fr nuclei k f is reduced from 0.85 to 0.8, in going from N = 131 to 117 (Fig.…”
Section: Statistical Model Considerationsmentioning
confidence: 96%
“…At the same time, a reasonable description of FBHs close to the stability line (where model parameters are tuned to experimental data) is usually accomplished [2]. Large discrepancies between predictions of different models and FBHs derived for neutron-deficient nuclei produced in nuclear reactions were also observed earlier [3]. The differences between different calculations for extremely neutron-rich (hypothetical) Po nuclei reach 30 MeV.…”
Section: Introductionmentioning
confidence: 99%