Parameter Optimisation for the Latest Quark-Meson Coupling Energy Density Functional
arXiv:1811.06628 · doi:10.1103/PhysRevC.100.024333
Abstract
The Quark--Meson--Coupling (QMC) model self-consistently relates the dynamics of the internal quark structure of a hadron to the relativistic mean fields arising in nuclear matter. It offers a natural explanation to some open questions in nuclear theory, including the origin of many-body nuclear forces and their saturation, the spin-orbit interaction and properties of hadronic matter at a wide range of densities. The QMC energy density functionals QMC-I and QMC-I have been successfully applied to calculate ground state observables of finite nuclei in the Hartree-Fock + BCS approximation, as well as to predict properties of dense nuclear matter and cold non-rotating neutron stars. Here we report the latest development of the model, QMC-II, extended to include higher order self-interaction of the meson. A derivative-free optimization algorithm has been employed to determine a new set of the model parameters and their statistics, including errors and correlations. QMC-II predictions for a wide range of properties of even-even nuclei across the nuclear chart, with fewer adjustable parameters, are comparable with other models. Predictions of ground state binding energies of even-even isotopes of superheavy elements with Z96 are particularly encouraging.
References in corpus (29)
- Big-Bang Nucleosynthesis
- Nuclear ground-state masses and deformations: FRDM(2012)
- Skyrme Interaction and Nuclear Matter Constraints
- Nuclear Energy Density Optimization
- Nuclear energy density optimization: Large deformations
- The Skyrme Interaction in finite nuclei and nuclear matter
- Pairing gaps from nuclear mean-field models
- Unexpectedly large charge radii of neutron-rich calcium isotopes
- Constraining the neutron-proton effective mass splitting using empirical constraints on the density dependence of nuclear symmetry energy around normal density
- The role of nucleon structure in finite nuclei
- The Compression-Mode Giant Resonances and Nuclear Incompressibility
- Nucleon and hadron structure changes in the nuclear medium and impact on observables
- Neutron skin of Pb from Coherent Pion Photoproduction
- Nuclear energy density optimization: Shell structure
- Incompressibility in finite nuclei and nuclear matter
- Towards the global description of nuclear charge radii: exploring the Fayans energy density functional
- Binding of Hypernuclei in the Latest Quark-Meson Coupling Model
- Physical Origin of Density Dependent Force of the Skyrme Type within the Quark Meson Coupling Model
- Are eta- and omega-nuclear states bound ?
- Quark structure and nuclear effective forces
- Eta bound states in nuclei: a probe of flavour-singlet dynamics
- Quark-Meson-Coupling (QMC) model for finite nuclei, nuclear matter and beyond
- Covariant energy density functionals: nuclear matter constraints and global ground state properties
- Finite Nuclei in the Quark-Meson Coupling (QMC) Model
- nuclei: A laboratory for neutron-proton collective mode
- Derivative-free optimization for parameter estimation in computational nuclear physics
- Giant Resonances from TDHF
- Superheavy Nuclei in the Quark-Meson-Coupling Model
- Nuclear symmetry energy and neutron skin thickness
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- Novel neutron decay mode inside neutron stars
- The Role of Baryon Structure in Neutron Stars
- Tensor and pairing interactions within the QMC energy density functional
- The outer crust of a cold, non-accreting neutron star within the Quark-Meson Coupling (QMC) model
- Neutron stars from crust to core within the Quark-meson coupling model
- Heavy Neutron Star Phenomenology with an H-dibaryon
- Neutrino mean free path in neutron stars in the presence of hyperons
- -mode Oscillations for Hyperons and H-dibaryons in Neutron Stars