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Landau Theory of Fermi Liquid in a Relativistic Nonlinear (σ, ω) Model at Finite Temperature

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Figure

Figure 1. Binding energies of symmetric nuclear matter at T = 0. The dotted-line is for LHA (linear σ, ω Hartree approximation), and solid-line is for NHA (nonlinear σ, ω Hartree approximation), which maintain the saturation condition: ρB = 0.148 fm−3, ρ
Figure 2. The effctive masses of nucleons and mesons in NHA (solid-lines) and LHA (dotted-line)
Figure 3. The effective masses of nucleons at finite temperatures: T = 0, T = 10, T = 30, T = 50 MeV
Figure 6 shows that baryon-antibaryon, ( NN ), interactions contribute negative in all densities, and it indicates ()()
+6

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