2019
DOI: 10.1103/physrevc.100.025205
|View full text |Cite
|
Sign up to set email alerts
|

Constraint to chiral invariant masses of nucleons from GW170817 in an extended parity doublet model

Abstract: We construct nuclear matter based on an extended parity doublet model including four light nucleons N (939), N (1440), N (1535), and N (1650). We exclude some values of the chiral invariant masses by requiring the saturation properties of normal nuclear matter; saturation density, binding energy, incompressibility, and symmetry energy. We find further constraint to the chiral invariant masses from the tidal deformability determined by the observation of the gravitational waves from neutron star merger GW170817… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

0
10
0

Year Published

2020
2020
2022
2022

Publication Types

Select...
7
2

Relationship

1
8

Authors

Journals

citations
Cited by 24 publications
(10 citation statements)
references
References 80 publications
0
10
0
Order By: Relevance
“…When the chiral symmetry is restored, the masses become degenerate with a common finite mass m ± (σ = 0) = m 0 , which reflects the parity doubling structure of the low-lying baryons. Following the previous studies of the parity-doublet-based models [25][26][27][28][29][37][38][39][40][41][42][43][44][45][46][47], as well as recent lattice QCD results [48,49], we choose a rather large value, m 0 = 700 MeV. The couplings g 1 and g 2 in equation 8can be determined by fixing the fermion masses in the vacuum.…”
Section: Hybrid Quark-meson-nucleon Modelmentioning
confidence: 99%
“…When the chiral symmetry is restored, the masses become degenerate with a common finite mass m ± (σ = 0) = m 0 , which reflects the parity doubling structure of the low-lying baryons. Following the previous studies of the parity-doublet-based models [25][26][27][28][29][37][38][39][40][41][42][43][44][45][46][47], as well as recent lattice QCD results [48,49], we choose a rather large value, m 0 = 700 MeV. The couplings g 1 and g 2 in equation 8can be determined by fixing the fermion masses in the vacuum.…”
Section: Hybrid Quark-meson-nucleon Modelmentioning
confidence: 99%
“…When the chiral symmetry is restored, the masses become degenerate with a common finite mass m ± (σ = 0) = m 0 , which reflects the parity doubling structure of the low-lying baryons. Following the previous studies of the parity-doublet-based models [25,26,27,28,29,37,38,39,40,41,42,43,44,45,46,47], as well as recent lattice QCD results [48,49], we choose a rather large value, m 0 = 700 MeV. The couplings g 1 and g 2 in Eq.…”
Section: Hybrid Quark-meson-nucleon Modelmentioning
confidence: 99%
“…The previous study in Ref. [24] based on the PDM extrapolates the hadronic equations state to the baryon density n B ∼ 3n 0 (n 0 0.16 fm −3 : nuclear saturation density). However, as emphasized in Refs.…”
Section: Introductionmentioning
confidence: 99%
“…In Ref. [24], the analyses were further extended to NS matter, the chiral invariant mass is restricted to be m 0 600 MeV by the tidal deformability estimated from the NS merger GW170817 [32][33][34].…”
Section: Introductionmentioning
confidence: 99%