2017
DOI: 10.1103/physrevc.95.034326
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Equation of state of nuclear and neutron matter at third-order in perturbation theory from chiral effective field theory

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 a… Show more

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Cited by 116 publications
(120 citation statements)
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“…Meanwhile, it is worth mentioning that the covariant density functional PKDD adopted here is phenomenological, where the nucleon-meson coupling constants are fixed according to the masses of spherical nuclei, the incompressibility, saturation density, and symmetry energy of nuclear matter [70]. In light of the recent developments of microscopic many-body calculations in describing finite nuclei and nuclear matter starting from realistic nucleonnucleon interactions [82][83][84][85][86][87][88], a more refined adjustment of parameters incorporating those results are necessary. A possible way to reach this in RMF model is to intro-duce density-dependent coupling constants derived from self-energies of Dirac-Brueckner calculations of nuclear matter [57,89], which are found decreasing with density and can be reproduced with Eqs.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…Meanwhile, it is worth mentioning that the covariant density functional PKDD adopted here is phenomenological, where the nucleon-meson coupling constants are fixed according to the masses of spherical nuclei, the incompressibility, saturation density, and symmetry energy of nuclear matter [70]. In light of the recent developments of microscopic many-body calculations in describing finite nuclei and nuclear matter starting from realistic nucleonnucleon interactions [82][83][84][85][86][87][88], a more refined adjustment of parameters incorporating those results are necessary. A possible way to reach this in RMF model is to intro-duce density-dependent coupling constants derived from self-energies of Dirac-Brueckner calculations of nuclear matter [57,89], which are found decreasing with density and can be reproduced with Eqs.…”
Section: Theoretical Frameworkmentioning
confidence: 99%
“…The correlations between the neutron-skins, the mirror charge radii, and the properties of the equations of state obtained with the Skryme EDF should be compared to results obtained from ab-initio approaches based on chiral two-and three-body interactions [16], [35], [36] in order to constrain and extend the functional forms used for the EDF calculations.…”
Section: And 5) Formentioning
confidence: 99%
“…Still, several reliable calculations have been performed up to twice that saturation density, beyond which uncertainties were estimated by analysing the order-by-order convergence in the chiral expansion and the many-body perturbation theory [120,121,122,123]. They were performed by extending the calculations of PNM with developed local chiral N 2 LO and N 3 LO interactions, including two-and three-body forces (see figure 14).…”
Section: Low-density Limitmentioning
confidence: 99%
“…For the low-density end, we collected calculations of the neutron matter EoS from microscopic nuclear forces at different orders in Chiral effective field theory from several standing works [120,121,122,123,134]. Those sets extend only up to nucleon-number density n of order of 1-2 n 0 ( ∼ 250MeV/fm 3 ) (only [121] extends the computation up to n = 2.5n 0 ( < 380 MeV/fm 3 for N3LO), Figure 16: Scheme of the interpolation through intermediate densities between a chiral computation [123] and the high-density pQCD physics at µ match ∼ 2.6 GeV.…”
Section: Interpolations At Intermediate Densitymentioning
confidence: 99%