PaperPanorama

Nuclear Theory·nucl-th

Friday·April 9, 2021

7 papers2 primary·5 cross-listed

  1. 01

    [Submitted on 8 Apr 2021]

    Benchmarking projected Hartree-Fock as an approximation

    Stephanie M. Lauber🇺🇸 · Hayden C. Frye🇺🇸 · Calvin W. Johnson🇺🇸

    We benchmark angular-momentum projected{-after-variation} Hartree-Fock calculations as an approximation to full configuration-interaction results in a shell model basis. For such a simple approximation we find reasonably good agreement between excitation spectra, including for many odd- and odd-odd nuclides. We frequently find shape coexistence, in the form of multiple Hartree-Fock minima; {mixing in shape coexistence, the first step beyond single-reference projected Hartree-Fock}, demonstrably improves the spectrum in the - and -shells. The complex spectra of germanium isotopes present a challenge: for even the spectra are only moderately good and those of odd bear little resemblance to the configuration-interaction results. Despite this failure we are able to broadly reproduce the odd-even staggering of ground state binding energies, save for germanium isotopes with . To illustrate potential applications, we compute the spectrum of the recently measured dripline nuclide Mg. All in all, projected Hartree-Fock often provides a better description of low-lying nuclear spectra than one might expect. Key to this is the use of gradient descent and unrestricted shapes.

    Comments:
    21 pages, 11 figures, 2 tables
    Subjects:
    Nuclear Theory (nucl-th)
    arXiv:
    2104.03455 [pdf]
    J.Phys.G(2021)·13 citations
  2. 02

    [Submitted on 8 Apr 2021]

    The signature of charge dependent directed flow observables by electromagnetic fields in heavy ion collisions

    Yifeng Sun🇮🇹 · Vincenzo Greco🇮🇹 · Salvatore Plumari🇮🇹

    We discuss the generation of the directed flow induced by the electromagnetic field as a function of and . Despite the complex dynamics of charged particles due to strong interactions generating several anisotropies in the azimuthal angle, it is possible at to directly correlate the splitting in of heavy quarks with different charges to some main features of the magnetic field, and in particular its values at formation and freeze-out time. We further found that the slope of the splitting of positively and negatively charged particles at high can be formulated as , where the constants and are constrained by the component of magnetic fields and the sign of is simply determined by the difference in the center of colliding systems at the formation time of particles and at the time when particles leave the effective range of electromagnetic fields or freeze out. The formula is derived from general considerations and is confirmed by several related numerical simulations; it supplies a useful guide to quantify the effect of different magnetic field configurations and provides an evidence of why the measurement of of charm, bottom and leptons from decay and their correlations are a powerful probe of the initial e.m. fields in ultra-relativistic collisions.

    Comments:
    12 pages, 12 figures
    Subjects:
    Nuclear Theory (nucl-th); High Energy Physics — Phenomenology (hep-ph); Nuclear Experiment (nucl-ex)
    arXiv:
    2104.03742 [pdf]
    Eur.Phys.J.Plus(2021)·9 citations

Affiliations

first authorsco-authorsvia INSPIRE