Table A.1.
Empirical constraints from experimental and observational data.
Symmetric matter | ||||
---|---|---|---|---|
Constraints | n (fm−3) | PSNM (MeV/fm3) | Ref. | |
HIC(DLL) | 0.32 | 10.1 ± 3.0 | Danielewicz et al. (2002) | |
HIC(FOPI) | 0.32 | 10.3 ± 2.8 | Le Fèvre et al. (2016) | |
Asymmetric matter | ||||
Constraints | n (fm−3) | esym (MeV) | Psym (MeV/fm3) | Ref. |
Nuclear structure | ||||
αD | 0.05 | 15.9 ± 1.0 | Zhang & Chen (2015) | |
PREX-II | 0.11 | 2.38 ± 0.75 | Adhikari et al. (2021), Reed et al. (2021), Lynch & Tsang (2022) | |
Nuclear masses | ||||
Mass(Skyrme) | 0.101 | 24.7 ± 0.8 | Brown & Schwenk (2014), Lynch & Tsang (2022) | |
Mass(DFT) | 0.115 | 25.4 ± 1.1 | Kortelainen et al. (2012), Lynch & Tsang (2022) | |
IAS | 0.106 | 25.5 ± 1.1 | Danielewicz et al. (2017), Lynch & Tsang (2022) | |
Heavy-ion collisions | ||||
HIC(Isodiff) | 0.035 | 10.3 ± 1.0 | Tsang et al. (2009), Lynch & Tsang (2022) | |
HIC(n/p ratio) | 0.069 | 16.8 ± 1.2 | Morfouace et al. (2019), Lynch & Tsang (2022) | |
HIC(π) | 0.232 | 52 ± 13 | 10.9 ± 8.7 | Estee et al. (2021), Lynch & Tsang (2022) |
HIC(n/p flow) | 0.240 | 12.1 ± 8.4 | Cozma (2018), Russotto et al. (2011, 2016), Lynch & Tsang (2022) | |
Astrophysical | ||||
Constraints | M⊙ | R (km) | Λ1.36 | Ref. |
LIGO 1 | 1.36 |
![]() |
Abbott et al. (2019) | |
Riley PSR J0030+0451 2 | 1.34 |
![]() |
Riley et al. (2019) | |
Miller PSR J0030+0451 3 | 1.44 |
![]() |
Miller et al. (2019) | |
Riley PSR J0740+6620 4 | 2.07 | 12.39![]() |
Riley et al. (2021) | |
Miller PSR J0740+6620 5 | 2.08 |
![]() |
Miller et al. (2021) | |
Choudhury PSR J0437-4715 6 | 1.418 |
![]() |
Choudhury et al. (2024) |
Notes. This table presents empirical values of symmetry energy (esym), symmetry energy pressure (Psym), and symmetric nuclear matter pressure (PSNM) from experimental data on the bulk properties of finite nuclei and HIC. The astrophysical observational constraints on the radii and tidal deformability of neutron stars are also included. See Ref Tsang et al. (2024) for details.
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