The most recent parametrization D1M of the Gogny energy density functional is
used to describe fission in the isotopes 232−280 Pu. We resort to the
methodology introduced in our previous studies [Phys. Rev. C \textbf{88},
054325 (2013) and Phys. Rev. C \textbf {89}, 054310 (2014)] to compute the
fission paths, collective masses and zero point quantum corrections within the
Hartree-Fock-Bogoliubov framework. The systematics of the spontaneous fission
half-lives tSF, masses and charges of the fragments in Plutonium isotopes
is analyzed and compared with available experimental data. We also pay
attention to isomeric states, the deformation properties of the fragments as
well as to the competition between the spontaneous fission and α-decay
modes. The impact of pairing correlations on the predicted tSF values is
demonstrated with the help of calculations for 232−280Pu in which the
pairing strengths of the Gogny-D1M energy density functional are modified by 5
% and 10 %, respectively. We further validate the use of the D1M
parametrization through the discussion of the half-lives in 242−262Fm. Our
calculations corroborate that, though the uncertainties in the absolute values
of physical observables are large, the Gogny-D1M Hartree-Fock-Bogoliubov
framework still reproduces the trends with mass and/or neutron numbers and
therefore represents a reasonable starting point to describe fission in heavy
nuclear systems from a microscopic point of view.Comment: 14 pages, 11 figures. arXiv admin note: text overlap with
arXiv:1312.722