<p>Temperature effect in proto neutron star (PNS) PSR J0740+6620 is studied by using relativistic mean field theory and considering baryon octet. The nucleon coupling constant is chosen as GM1, and the temperature of the PNS is set as T = 7, 14, 21, 28, 35 MeV, respectively. Our results show that under the constraint of mass M = 2. 08 M<sub>⨀</sub> of the PNS PSR J0740+6620, the radius R increases with increasing temperature T. With respect to the same baryon density ρ, the field strength of mesons σ, ω, ρ and the chemical potential of neutrons μ<sub>n</sub> decrease while the field strength of σ<sup>*</sup> and ϕ increase with the increase of temperature T. The chemical potential of electron μ<sub>e</sub> increases when the baryon density is less than ρ = 0.3 fm<sup>-3</sup>, but decreases when the baryon density is greater than ρ = 0.3 fm<sup>-3</sup>, companying with the increase of temperature T. Relative to the same baryon density ρ, the relative density of neutrons decreases while those of proton, Λ, Σ<sup>+</sup>, Σ<sup>0</sup>, Σ<sup>–</sup>, Ξ<sup>0</sup>, and Ξ<sup>–</sup> all increases with increasing temperature T. The central relative densities of neutrons decrease, while those of protons, hyperons Σ<sup>+</sup>, Σ<sup>0</sup>, Σ<sup>–</sup>, Ξ<sup>0</sup>, and Ξ<sup>–</sup> all increase with increasing temperature T. As for the relative density of hyperon Λ, it increases firstly, reaching a maximum value when the temperature is about T = 20 MeV, and then decreases with the increase of temperature T.</p>

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Temperature Effects in the Proto Neutron Star Phase of PSR J0740+6620

  • Xian-Feng Zhao,
  • Wen-Bo Ding,
  • Bin Tang

摘要

Temperature effect in proto neutron star (PNS) PSR J0740+6620 is studied by using relativistic mean field theory and considering baryon octet. The nucleon coupling constant is chosen as GM1, and the temperature of the PNS is set as T = 7, 14, 21, 28, 35 MeV, respectively. Our results show that under the constraint of mass M = 2. 08 M of the PNS PSR J0740+6620, the radius R increases with increasing temperature T. With respect to the same baryon density ρ, the field strength of mesons σ, ω, ρ and the chemical potential of neutrons μn decrease while the field strength of σ* and ϕ increase with the increase of temperature T. The chemical potential of electron μe increases when the baryon density is less than ρ = 0.3 fm-3, but decreases when the baryon density is greater than ρ = 0.3 fm-3, companying with the increase of temperature T. Relative to the same baryon density ρ, the relative density of neutrons decreases while those of proton, Λ, Σ+, Σ0, Σ, Ξ0, and Ξ all increases with increasing temperature T. The central relative densities of neutrons decrease, while those of protons, hyperons Σ+, Σ0, Σ, Ξ0, and Ξ all increase with increasing temperature T. As for the relative density of hyperon Λ, it increases firstly, reaching a maximum value when the temperature is about T = 20 MeV, and then decreases with the increase of temperature T.