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Symmetry energy: nuclear masses and neutron stars
Nuclear Theory · Submitted 11 Sep 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Comparison with observations of neutron stars again favours a value of J = 30 MeV.
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The abstract, sentence by sentence
We describe the main features of our most recent Hartree-Fock-Bogoliubov nuclear mass models, based on 16-parameter generalized Skyrme forces. They have been fitted to the data of the 2012 Atomic Mass Evaluation, and favour a value of 30 MeV for the symmetry coefficient J, the corresponding root-mean square deviation being 0.549 MeV. We find that this conclusion is compatible with measurements of neutron-skin thickness. By constraining the underlying interactions to fit various equations of state of neutron matter calculated {\it ab initio} our models are well adapted to a realistic and unified treatment of all regions of neutron stars. We use our models to calculate the composition, the equation of state, the mass-radius relation and the maximum mass. Comparison with observations of neutron stars again favours a value of J = 30 MeV.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We describe the main features of our most recent Hartree-Fock-Bogoliubov nuclear mass models, based on 16-parameter generalized Skyrme forces. | method 0.58 | 0.91 | 0.04 | asserted 0.95 |
| s1 | They have been fitted to the data of the 2012 Atomic Mass Evaluation, and favour a value of 30 MeV for the symmetry coefficient J, the corresponding root-mean square deviation being 0.549 MeV. | result 0.83 | 0.87 | 0.35 | asserted 0.97 |
| s2 | We find that this conclusion is compatible with measurements of neutron-skin thickness. | interpretation 0.66 | 0.90 | 0.12 | asserted 0.58 |
| s3 | By constraining the underlying interactions to fit various equations of state of neutron matter calculated {\it ab initio} our models are well adapted to a realistic and unified treatment of all regions of neutron stars. | method 0.78 | 0.85 | 0.08 | asserted 0.99 |
| s4 | We use our models to calculate the composition, the equation of state, the mass-radius relation and the maximum mass. | method 0.60 | 0.96 | 0.05 | asserted 0.98 |
| s5 | Comparison with observations of neutron stars again favours a value of J = 30 MeV. | result 0.92 | 0.83 | 0.35 | asserted 0.77 |
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Original abstract
We describe the main features of our most recent Hartree-Fock-Bogoliubov nuclear mass models, based on 16-parameter generalized Skyrme forces. They have been fitted to the data of the 2012 Atomic Mass Evaluation, and favour a value of 30 MeV for the symmetry coefficient J, the corresponding root-mean square deviation being 0.549 MeV. We find that this conclusion is compatible with measurements of neutron-skin thickness. By constraining the underlying interactions to fit various equations of state of neutron matter calculated {\it ab initio} our models are well adapted to a realistic and unified treatment of all regions of neutron stars. We use our models to calculate the composition, the equation of state, the mass-radius relation and the maximum mass. Comparison with observations of neutron stars again favours a value of J = 30 MeV.
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References
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For the BSk models, the $M-R$ relations obtained with EoSs based on a simplified CLDM used in this work are close to the ones calculated with a full microscopic model in [ref] , see in discussion in [ref] .
Strong correlations of neutron star radii with the slopes of nuclear matter incompressibility and symmetry energy at saturation · Introduction · 0.99
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The numerical calculations have been done using the LORENE library (, see also Ref. [ref] ).
An introduction to the theory of rotating relativistic stars · Implications of HFB models for neutron stars · 0.99
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