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Equation of state of nuclear and neutron matter at third-order in perturbation theory from chiral EFT

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abstract

We compute from chiral two- and three-nucleon interactions the energy per particle of symmetric nuclear matter and pure neutron matter at third-order in perturbation theory including self-consistent second-order single-particle energies. Particular attention is paid to the third-order particle-hole ring-diagram, which is often neglected in microscopic calculations of the equation of state. We provide semi-analytic expressions for the direct terms from central and tensor model-type interactions that are useful as theoretical benchmarks. We investigate uncertainties arising from the order-by-order convergence in both many-body perturbation theory and the chiral expansion. Including also variations in the resolution scale at which nuclear forces are resolved, we provide new error bands on the equation of state, the isospin-asymmetry energy, and its slope parameter. We find in particular that the inclusion of third-order diagrams reduces the theoretical uncertainty at low densities, while in general the largest error arises from omitted higher-order terms in the chiral expansion of the nuclear forces.

fields

nucl-th 1

years

2025 1

verdicts

CONDITIONAL 1

representative citing papers

Probing of EoS with clusters and hypernuclei

nucl-th · 2025-07-18 · conditional · novelty 5.0

Using the PHQMD transport model, the paper shows that a soft momentum-dependent nuclear equation of state reproduces most STAR 3 GeV Au+Au data for baryons, clusters and hypernuclei, while a hard equation of state gives similar results.

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  • Probing of EoS with clusters and hypernuclei nucl-th · 2025-07-18 · conditional · none · ref 13 · internal anchor

    Using the PHQMD transport model, the paper shows that a soft momentum-dependent nuclear equation of state reproduces most STAR 3 GeV Au+Au data for baryons, clusters and hypernuclei, while a hard equation of state gives similar results.