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- W2892263402 abstract "The systematic of the spontaneous fission half-lives for the nuclei $^{242--262}mathrm{Fm}$ and $^{250--260}mathrm{No}$ is analyzed, within a least action scheme, with the parametrization D1M of the Gogny energy density functional. The properties of the dynamic (least action) fission paths are analyzed and compared to those of the static (minimal energy) ones. The constrained Hartree-Fock-Bogoliubov approximation is used to compute deformed mean-field configurations, zero-point quantum corrections, and collective inertias. It is shown that a cumbersome full variational search of the least action fission path, within the space of Hartree-Fock-Bogoliubov (HFB) states, might not be required if the relevant degrees of freedom are taken into account in the minimization of the Wentzel-Kramers-Brillouin action. The action is minimized in terms of pairing fluctuations that explore the pairing content of the HFB states along the fission paths of the considered nuclei. It is found that, for a given shape, the minimum of the action in fermium and nobelium nuclei corresponds to a value of the pairing fluctuations larger than the one associated with the minimal energy solution for the same shape. The reduction of the action, via larger pairing correlations, has a significant impact on the predicted spontaneous fission half-lives, improving their comparison with experiments by several orders of magnitude." @default.
- W2892263402 created "2018-09-27" @default.
- W2892263402 creator A5049709261 @default.
- W2892263402 creator A5074723674 @default.
- W2892263402 date "2018-09-10" @default.
- W2892263402 modified "2023-10-15" @default.
- W2892263402 title "Least action description of spontaneous fission in fermium and nobelium nuclei based on the Gogny energy density functional" @default.
- W2892263402 cites W1552338467 @default.
- W2892263402 cites W1556276470 @default.
- W2892263402 cites W1579593335 @default.
- W2892263402 cites W1639512300 @default.
- W2892263402 cites W1896196146 @default.
- W2892263402 cites W1967598125 @default.
- W2892263402 cites W1970060762 @default.
- W2892263402 cites W1975387297 @default.
- W2892263402 cites W1979139742 @default.
- W2892263402 cites W1986990727 @default.
- W2892263402 cites W1989034092 @default.
- W2892263402 cites W1997300181 @default.
- W2892263402 cites W2001068932 @default.
- W2892263402 cites W2001228541 @default.
- W2892263402 cites W2007831508 @default.
- W2892263402 cites W2008894279 @default.
- W2892263402 cites W2009308450 @default.
- W2892263402 cites W2009535788 @default.
- W2892263402 cites W2010092102 @default.
- W2892263402 cites W2010191978 @default.
- W2892263402 cites W2012648862 @default.
- W2892263402 cites W2014887833 @default.
- W2892263402 cites W2016739453 @default.
- W2892263402 cites W2017310574 @default.
- W2892263402 cites W2017767315 @default.
- W2892263402 cites W2021335627 @default.
- W2892263402 cites W2027637333 @default.
- W2892263402 cites W2030511146 @default.
- W2892263402 cites W2033174649 @default.
- W2892263402 cites W2033362413 @default.
- W2892263402 cites W2035114019 @default.
- W2892263402 cites W2035305989 @default.
- W2892263402 cites W2042843404 @default.
- W2892263402 cites W2043888849 @default.
- W2892263402 cites W2048914769 @default.
- W2892263402 cites W2049085419 @default.
- W2892263402 cites W2052324542 @default.
- W2892263402 cites W2065968493 @default.
- W2892263402 cites W2070664900 @default.
- W2892263402 cites W2070941391 @default.
- W2892263402 cites W2077494662 @default.
- W2892263402 cites W2080962162 @default.
- W2892263402 cites W2087930898 @default.
- W2892263402 cites W2089460978 @default.
- W2892263402 cites W2093638339 @default.
- W2892263402 cites W2094660523 @default.
- W2892263402 cites W2095113619 @default.
- W2892263402 cites W2095627876 @default.
- W2892263402 cites W2098013088 @default.
- W2892263402 cites W2130009343 @default.
- W2892263402 cites W2130066640 @default.
- W2892263402 cites W2139721257 @default.
- W2892263402 cites W2144017325 @default.
- W2892263402 cites W2168802219 @default.
- W2892263402 cites W2171757040 @default.
- W2892263402 cites W2173821512 @default.
- W2892263402 cites W2174447864 @default.
- W2892263402 cites W2253409574 @default.
- W2892263402 cites W2268670642 @default.
- W2892263402 cites W2289607259 @default.
- W2892263402 cites W230778086 @default.
- W2892263402 cites W2315759723 @default.
- W2892263402 cites W2316597683 @default.
- W2892263402 cites W2323703035 @default.
- W2892263402 cites W2329220747 @default.
- W2892263402 cites W2513751716 @default.
- W2892263402 cites W2615252108 @default.
- W2892263402 cites W2725691849 @default.
- W2892263402 cites W2750525225 @default.
- W2892263402 cites W2781262276 @default.
- W2892263402 cites W2789930919 @default.
- W2892263402 cites W2804950444 @default.
- W2892263402 cites W2962898822 @default.
- W2892263402 cites W3098537671 @default.
- W2892263402 cites W3106242714 @default.
- W2892263402 cites W4244885879 @default.
- W2892263402 cites W4248387952 @default.
- W2892263402 cites W4255292033 @default.
- W2892263402 cites W4299580424 @default.
- W2892263402 doi "https://doi.org/10.1103/physrevc.98.034308" @default.
- W2892263402 hasPublicationYear "2018" @default.
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