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Impacts of the $$U(1)_A$$ anomaly on nuclear and neutron star equation of state based on a parity doublet model

カイラル二重項模型をもとにした$$U(1)_A$$異常の原子核と中性子星の状態方程式への影響

Gao, B.*; 南川 拓哉*; 古城 徹*; 原田 正康*

Gao, B.*; Minamikawa, Takuya*; Kojo, Toru*; Harada, Masayasu*

We examine the role of the U(1)$$_{A}$$ anomaly in a parity doublet model of nucleons which include the chiral variant and invariant masses. Our model expresses the U(1)$$_{A}$$ anomaly by the Kobayashi-Maskawa-'t Hooft (KMT) interaction in the mesonic sector. After examining the roles of the KMT term in vacuum, we discuss its impacts on nuclear equations of state (EOS). The U(1)$$_{A}$$ anomaly increases the masses of the $$eta$$' and $$sigma$$ mesons and enhances the chiral symmetry breaking. Also, the U(1)$$_{A}$$ anomaly enlarges the energy difference between chiral symmetric and symmetry broken vacuum; in turn, the chiral restoration at high density adds a larger energy density (often referred as a bag constant) to EOSs than in the case without the anomaly, leading to softer EOSs. Including these U(1)$$_{A}$$ effects, we update the previously constructed unified equations of state that interpolate the nucleonic EOS at $$n$$$$_{B}$$ $$leqq$$ 2$$n$$$$_{0}$$ ($$n$$$$_{0}$$ = 0.16 fm$$^{-3}$$; nuclear saturation density) and quark EOS at $$n$$$$_{B}$$ $$geqq$$ 5 $$n$$$$_{0}$$. The unified EOS is confronted with the observational constraints on the masses and radii of neutron stars. The softening of EOSs associated with the $$U$$(1) anomaly reduces the overall radii, relaxing the previous constraint on the chiral invariant mass $$m$$$$_{0}$$. Including the attractive nonlinear $$rho$$-$$omega$$ coupling for the reduced slope parameter in the symmetry energy, our new estimate is 400 MeV $$leqq$$ $$m$$$$_{0}$$ $$leqq$$ 700 MeV, with $$m$$$$_{0}$$ smaller than our previous estimate by $$approx$$200 MeV.

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パーセンタイル:52.69

分野:Physics, Nuclear

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