Glant Monopole and Quadrupole States in a Chiral Breaking Field Theory

  • The saturating chiral breaking field theory are used to study the compressibility of the Fermi-liquid and the excitation energies of the giant monopole and quadrupole states in the framework of mean-field theory.It is found that the compressibility of the Fermi-liquid in the nuclear system,and the excitation energies of the giant monopole and quadrupole states are more close to the experimental values in comparison with the results of the σ-ω model.
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  • [1] J. D. Walecka, Ann. Phys. (N. Y.), 83(1974). 491.[2] J. Boguta and A. R. Bodtner, Nucl. Phys., A292(1977), 413.[3] J. Boguta, Phys. Lett., B120(1983), 34.[4] M. Kohno, K. Ando, Prog. Theor. Phys., 61(1979), 1065.[5] T. Suzuki, Prog, Theor. Phys., 64(1980), 1627[6] S. Nishizaki, H. Kurasawa, T. Suzuki, Nucl, Phys., A462(1987), 687.[7] M. Gell-Mann and M. Levy, Nuovo Cimento, 16(1960), 705.[8] B. D. Serot, J. D. Walecka, adv. Nucl. Phys., 16, ed. J. W. Negele, E. Vogt (Plenum, N. Y., 1986).[9] C. Y. Zhu and Xi-Jun Qiu, Comm. Theor, Phys., 15(1991), 27;C. Y. Zhu and Xi-Jun Qiu, J. Phys., G17(1991), L11.
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ZHANG Qing-Lan and QIU Xi-Jun. Glant Monopole and Quadrupole States in a Chiral Breaking Field Theory[J]. Chinese Physics C, 1992, 16(7): 615-622.
ZHANG Qing-Lan and QIU Xi-Jun. Glant Monopole and Quadrupole States in a Chiral Breaking Field Theory[J]. Chinese Physics C, 1992, 16(7): 615-622. shu
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Received: 1900-01-01
Revised: 1900-01-01
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Glant Monopole and Quadrupole States in a Chiral Breaking Field Theory

    Corresponding author: ZHANG Qing-Lan,
  • Shanghai Institute of Nuclear Research,Academia Sinica,201800

Abstract: The saturating chiral breaking field theory are used to study the compressibility of the Fermi-liquid and the excitation energies of the giant monopole and quadrupole states in the framework of mean-field theory.It is found that the compressibility of the Fermi-liquid in the nuclear system,and the excitation energies of the giant monopole and quadrupole states are more close to the experimental values in comparison with the results of the σ-ω model.

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