PaperPanorama

Nuclear Theory·nucl-th

Monday·October 22, 2018

3 papers3 primary·0 cross-listed

  1. 01

    [Submitted on 19 Oct 2018]

    From Asymmetric to Symmetric Fission in the Fermium Isotopes within the Time-Dependent GCM Formalism

    D. Regnier🇫🇷 · N. Dubray🇫🇷 · N. Schunck🇺🇸

    Predicting the properties of neutron-rich nuclei far from the valley of stability is one of the major challenges of modern nuclear theory. In heavy and superheavy nuclei, a difference of only a few neutrons is sufficient to change the dominant fission mode. A theoretical approach capable of predicting such rapid transitions for neutron-rich systems would be a valuable tool to better understand r-process nucleosynthesis or the decay of super-heavy elements. In this work, we investigate for the first time the transition from asymmetric to symmetric fission through the calculation of primary fission yields with the time-dependent generator coordinate method (TDGCM). We choose here the transition in neutron-rich Fermium isotopes, which was the first to be observed experimentally in the late seventies and is often used as a benchmark for theoretical studies. We compute the primary fission fragment mass and charge yields for 254 Fm, 256 Fm and 258 Fm from the TDGCM under the Gaussian overlap approximation. The static part of the calculation (generation of a potential energy surface) consists in a series of constrained Hartree-Fock-Bogoliubov calculations based on the D1S, D1M or D1N parameterizations of the Gogny effective interaction in a two-center harmonic oscillator basis. The 2-dimensional dynamics in the collective space spanned by the quadrupole and octupole moments is then computed with the finite element solver FELIX-2.0. The available experimental data and the TDGCM post-dictions are consistent and agree especially on the position in the Fermium isotopic chain at which the transition occurs. The main limitation of the method lies in the presence of discontinuities in the 2-dimensional manifold of generator states.

    Subjects:
    Nuclear Theory (nucl-th)
    arXiv:
    1810.08402 [pdf]
    PRC(2019)·64 citations
  2. 02

    [Submitted on 19 Oct 2018]

    A Study of the Three Body Force Effect on the EOS Properties of Asymmetric Nuclear Matter

    H. M. M.Mansour🇪🇬 · M. El Zohry🇪🇬 · A. E. Elmeshneb🇪🇬

    Three body effects are studied for both asymmetric nuclear matter and pure neutron matter to calculate the nuclear Equation of State . The Brueckner Hartree Fock approximation is used using CD Bonn B and Argonne V18 potentials. A two body density dependent Skyrme potential is added to reproduce the empirical saturation point. Good agreement is obtained in comparison with exact calculation including three body forces.

    Comments:
    10 pages,5 figures,1 table
    Subjects:
    Nuclear Theory (nucl-th)
    arXiv:
    1810.08405 [pdf]
    Armenian J.Phys.(2018)·1 citation
  3. 03

    [Submitted on 19 Oct 2018]

    Tensor-decomposition techniques for ab initio nuclear structure calculations. From chiral nuclear potentials to ground-state energies

    Alexander Tichai🇫🇷 · Roman Schutski🇺🇸 · Gustavo E. Scuseria🇺🇸 · Thomas Duguet🇫🇷

    The impact of applying state-of-the-art tensor factorization techniques to modern nuclear Hamiltonians derived from chiral effective field theory is investigated. Subsequently, the error induced by the tensor decomposition of the input Hamiltonian on ground-state energies of closed-shell nuclei calculated via second-order many-body perturbation theory is benchmarked. With the aid of the factorized Hamiltonian, the second-order perturbative correction to ground-state energies is decomposed and the scaling properties of the underlying tensor network are discussed. The employed tensor formats are found to lead to an efficient data compression of two-body matrix elements of the nuclear Hamiltonian. In particular, the sophisticated \emph{tensor hypercontraction} (THC) scheme yields low tensor ranks with respect to both harmonic-oscillator and Hartree-Fock single-particle bases. It is found that the tensor rank depends on the two-body total angular momentum for which one performs the decomposition, which is itself directly related to the sparsity the corresponding tensor. Furthermore, including normal-ordered two-body contributions originating from three-body interactions does not compromise the efficient data compression. Ultimately, the use of factorized matrix elements authorizes controlled approximations of the exact second-order ground-state energy corrections. In particular, a small enough error is obtained from low-rank factorizations in He, O and Ca.

    Comments:
    16 pages, 13 figures, 1 table
    Subjects:
    Nuclear Theory (nucl-th); physics.chem-ph (physics.chem-ph); Computational Physics (physics.comp-ph)
    arXiv:
    1810.08419 [pdf]
    PRC(2019)·24 citations

Affiliations

first authorsco-authorsvia INSPIRE