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Universal symmetry energy contribution to the neutron star equation of state
Nuclear Theory · Submitted 28 Apr 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We discuss the observation that under neutron star conditions of charge neutrality and $\beta-$equilibrium the contribution from the symmetry energy to the equation of state (EoS) follows a universal behaviour.
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The abstract, sentence by sentence
We discuss the observation that under neutron star conditions of charge neutrality and $\beta-$equilibrium the contribution from the symmetry energy to the equation of state (EoS) follows a universal behaviour. We call this behaviour the conjecture of a Universal Symmetry Energy Contribution (USEC). We find that an USEC holds provided the density dependence of the symmetry energy $E_s(n)$ follows a behaviour that limits the proton fraction $x(n)$ to values below the threshold for the direct Urca (DU) cooling process. The absence of DU cooling in typical mass neutron stars appears to be supported by the phenomenology of neutron star cooling data and allows to constrain the behaviour of $E_s(n)$ at high densities. Two classes of symmetry energy functions are investigated more in detail to elucidate the USEC. We derive an analytic formula for the USEC to the neutron star EoS based on the result for the symmetry energy extracted from isobaric analog states of nuclei.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the observation that under neutron star conditions of charge neutrality and $\beta-$equilibrium the contribution from the symmetry energy to the equation of state (EoS) follows a universal behaviour. | result 0.76 | 0.20 | 0.64 | asserted 0.83 |
| s1 | We call this behaviour the conjecture of a Universal Symmetry Energy Contribution (USEC). | contribution 0.55 | 0.71 | 0.13 | asserted 0.67 |
| s2 | We find that an USEC holds provided the density dependence of the symmetry energy $E_s(n)$ follows a behaviour that limits the proton fraction $x(n)$ to values below the threshold for the direct Urca (DU) cooling process. | result 0.97 | 0.90 | 0.47 | asserted 0.99 |
| s3 | The absence of DU cooling in typical mass neutron stars appears to be supported by the phenomenology of neutron star cooling data and allows to constrain the behaviour of $E_s(n)$ at high densities. | interpretation 0.81 | 0.26 | 0.18 | hedged possibility 0.91 |
| s4 | Two classes of symmetry energy functions are investigated more in detail to elucidate the USEC. | method 0.66 | 0.79 | 0.03 | asserted 0.86 |
| s5 | We derive an analytic formula for the USEC to the neutron star EoS based on the result for the symmetry energy extracted from isobaric analog states of nuclei. | result 0.59 | 0.95 | 0.14 | asserted 1.00 |
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The paper
Original abstract
We discuss the observation that under neutron star conditions of charge neutrality and $\beta-$equilibrium the contribution from the symmetry energy to the equation of state (EoS) follows a universal behaviour. We call this behaviour the conjecture of a Universal Symmetry Energy Contribution (USEC). We find that an USEC holds provided the density dependence of the symmetry energy $E_s(n)$ follows a behaviour that limits the proton fraction $x(n)$ to values below the threshold for the direct Urca (DU) cooling process. The absence of DU cooling in typical mass neutron stars appears to be supported by the phenomenology of neutron star cooling data and allows to constrain the behaviour of $E_s(n)$ at high densities. Two classes of symmetry energy functions are investigated more in detail to elucidate the USEC. We derive an analytic formula for the USEC to the neutron star EoS based on the result for the symmetry energy extracted from isobaric analog states of nuclei.
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References
How the literature uses it
12 arXiv papers cite this in 17 sentences
Papers citing it · 9 sentences without a confident label
Builds on it 1 paper
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Our analysis confirms the universal behavior of the EOS discussed in Ref. [ref] and generalizes it to cases where dUrca is allowed for large masses.
The equation of state for dense nucleonic matter from a meta-modeling. II. Predictions for neutron stars properties · Impact on the equation of state at $β$-equilibrium · 0.98
Uses its method or tool 1 paper
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Here we compute $S$ at saturation density by imposing beta equilibrium on the matter, including the possible presence of muons, using the formulae in Section II of [ref] .
The Radius of PSR J0437-4715 from NICER Data · Statistical Method · 0.99
Cites it as support 2 papers
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It explains why the global properties of the NS shown in Figs. [ref] and [ref] are not very much impacted by these hypothesis, and reflects the universality of the EOS under the charge neutrality and $β$-equilibrium conditions [ref] .
The equation of state for dense nucleonic matter from a meta-modeling. II. Predictions for neutron stars properties · Impact on the equation of state at $β$-equilibrium · 0.97
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We do not expect however that this alters significantly the present comparison because of the compensating mechanism discussed in Refs. [ref] : the increase of the pressure due to the electrons balances the decrease of the symmetry energy due to the proton excess (at fixed total baryon density).
Thermodynamics of the parity-doublet model: Asymmetric and neutron matter · Constraints from neutron stars · 0.96
Cites it as background 3 papers
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During the last two decades, significant efforts have been devoted to exploring the using both terrestrial laboratory experiments [ref] and astrophysical observations [ref] .
How tightly is nuclear symmetry energy constrained by unitary Fermi gas? · Introduction · 0.98
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Comprehensive reviews on the recent progress and remaining challenges in constraining the can be found in the literature [ref] .
Nuclear Symmetry Energy Extracted from Laboratory Experiments · Introduction · 0.94
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[ref] for reviews.
Towards Understanding Astrophysical Effects of Nuclear Symmetry Energy · What have we learned about the symmetry energy so far? · 0.89
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